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<channel>
	<title>Vox Charta &#187; Galactic</title>
	<atom:link href="http://voxcharta.org/category/astro-ph/galactic-astro-ph/feed/" rel="self" type="application/rss+xml" />
	<link>http://voxcharta.org</link>
	<description></description>
	<lastBuildDate>Tue, 22 May 2012 18:03:08 +0000</lastBuildDate>
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			<item>
		<title>A comparison of galaxy peculiar velocities field with the PSCz gravity field&#8211; A hyper-parameter method</title>
		<link>http://voxcharta.org/2012/05/21/a-comparison-of-galaxy-peculiar-velocities-field-with-the-pscz-gravity-field-a-hyper-parameter-method/</link>
		<comments>http://voxcharta.org/2012/05/21/a-comparison-of-galaxy-peculiar-velocities-field-with-the-pscz-gravity-field-a-hyper-parameter-method/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:55:25 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[adequate model]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[galaxy distribution]]></category>
		<category><![CDATA[gravity field]]></category>
		<category><![CDATA[ira]]></category>
		<category><![CDATA[model data]]></category>
		<category><![CDATA[mpc]]></category>
		<category><![CDATA[parameter method]]></category>
		<category><![CDATA[peculiar velocity]]></category>
		<category><![CDATA[sampling]]></category>
		<category><![CDATA[shapley concentration]]></category>
		<category><![CDATA[statistical method]]></category>
		<category><![CDATA[supercluster]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/a-comparison-of-galaxy-peculiar-velocities-field-with-the-pscz-gravity-field-a-hyper-parameter-method/</guid>
		<description><![CDATA[We constructed a hyper-parameter statistical method to quantify the difference between predicted velocities derived from the observed galaxy distribution in the IRAS-PSCz redshift survey and peculiar velocities measured using different distance indicators. In our analysis we find that the model-data comparison becomes unreliable beyond 70 Mpc/h because of the inadequate sampling of prominent, distant superclusters [...]]]></description>
			<content:encoded><![CDATA[<p>We constructed a hyper-parameter statistical method to quantify the difference between predicted velocities derived from the observed galaxy distribution in the IRAS-PSCz redshift survey and peculiar velocities measured using different distance indicators. In our analysis we find that the model-data comparison becomes unreliable beyond 70 Mpc/h because of the inadequate sampling of prominent, distant superclusters like the Shapley Concentration by IRAS galaxies. On the other hand, the analysis of the velocity residuals show that the PSCz gravity field provides an adequate model to the local, &lt;= 70 Mpc/h, peculiar velocity field. The hyper-parameter combination of ENEAR, SN, A1SN and SFI++ catalogues constrains the amplitude of the linear flow to \beta=0.53 \pm 0.01. For an rms density fluctuations in the PSCz galaxy number density \sigma_8^{\rm gal}=0.42\pm0.03, we obtain an estimate of the growth rate of density fluctuations $f\sigma_{8}(z\sim0) = 0.42 \pm 0.03$, which is in excellent agreement with independent estimates based on different techniques.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/a-comparison-of-galaxy-peculiar-velocities-field-with-the-pscz-gravity-field-a-hyper-parameter-method/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>How covariant is the galaxy luminosity function?</title>
		<link>http://voxcharta.org/2012/05/21/how-covariant-is-the-galaxy-luminosity-function/</link>
		<comments>http://voxcharta.org/2012/05/21/how-covariant-is-the-galaxy-luminosity-function/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:54:39 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[analytic model]]></category>
		<category><![CDATA[bia]]></category>
		<category><![CDATA[body simulation]]></category>
		<category><![CDATA[bright galaxy]]></category>
		<category><![CDATA[clf]]></category>
		<category><![CDATA[cluster]]></category>
		<category><![CDATA[cluster expansion]]></category>
		<category><![CDATA[covariance matrix]]></category>
		<category><![CDATA[density field]]></category>
		<category><![CDATA[dependence]]></category>
		<category><![CDATA[estimates]]></category>
		<category><![CDATA[estimators]]></category>
		<category><![CDATA[galaxy catalogue]]></category>
		<category><![CDATA[galaxy luminosity function]]></category>
		<category><![CDATA[mass function]]></category>
		<category><![CDATA[millennium]]></category>
		<category><![CDATA[sample variance]]></category>
		<category><![CDATA[scale structure]]></category>
		<category><![CDATA[three pieces]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/how-covariant-is-the-galaxy-luminosity-function/</guid>
		<description><![CDATA[We investigate the error properties of certain galaxy luminosity function (GLF) estimators. Using a cluster expansion of the density field, we show how, for both volume and flux limited samples, the GLF estimates are covariant. The covariance matrix can be decomposed into three pieces: a diagonal term arising from Poisson noise; a sample variance term [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate the error properties of certain galaxy luminosity function (GLF) estimators. Using a cluster expansion of the density field, we show how, for both volume and flux limited samples, the GLF estimates are covariant. The covariance matrix can be decomposed into three pieces: a diagonal term arising from Poisson noise; a sample variance term arising from large-scale structure in the survey volume; an occupancy covariance term arising due to galaxies of different luminosities inhabiting the same cluster. To evaluate the theory one needs: the mass function and bias of clusters, and the conditional luminosity function (CLF). We use a semi-analytic model (SAM) galaxy catalogue from the Millennium run N-body simulation and the CLF of Yang et al. (2003) to explore these effects. The GLF estimates from the SAM and the CLF qualitatively reproduce results from the 2dFGRS. We also measure the luminosity dependence of clustering in the SAM and find reasonable agreement with 2dFGRS results for bright galaxies. However, for fainter galaxies, L&lt;L*, the SAM overpredicts the relative bias by ~10-20%. We use the SAM data to estimate the errors in the GLF estimates for a volume limited survey of volume V~0.13 [Gpc/h]^3. We find that different luminosity bins are highly correlated: for L0.5. Our theory is in good agreement with these measurements. These strong correlations can be attributed to sample variance. For a flux-limited survey of similar volume, the estimates are only slightly less correlated. We explore the importance of these effects for GLF model parameter estimation. We show that neglecting to take into account the bin-to-bin covariances can lead to significant systematic errors in best-fit parameters.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/how-covariant-is-the-galaxy-luminosity-function/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Physical properties of dense molecular gas in centres of Seyfert galaxies</title>
		<link>http://voxcharta.org/2012/05/21/physical-properties-of-dense-molecular-gas-in-centres-of-seyfert-galaxies/</link>
		<comments>http://voxcharta.org/2012/05/21/physical-properties-of-dense-molecular-gas-in-centres-of-seyfert-galaxies/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:54:11 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[AGN]]></category>
		<category><![CDATA[channel separation]]></category>
		<category><![CDATA[critical value]]></category>
		<category><![CDATA[dense gas]]></category>
		<category><![CDATA[direct evidence]]></category>
		<category><![CDATA[dispersion]]></category>
		<category><![CDATA[dynamical state]]></category>
		<category><![CDATA[fwhm]]></category>
		<category><![CDATA[hcn]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[kinematic parameters]]></category>
		<category><![CDATA[major axis]]></category>
		<category><![CDATA[position angle]]></category>
		<category><![CDATA[radius]]></category>
		<category><![CDATA[resolution data]]></category>
		<category><![CDATA[seyfert galaxy]]></category>
		<category><![CDATA[smearing]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[starburst]]></category>
		<category><![CDATA[velocity gradient]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/physical-properties-of-dense-molecular-gas-in-centres-of-seyfert-galaxies/</guid>
		<description><![CDATA[We present new ~1&#8243; resolution data of the dense molecular gas in the central 50-100 pc of four nearby Seyfert galaxies. PdBI observations of HCN and, in 2 of the 4 sources, simultaneously HCO+ allow us to carefully constrain the dynamical state of the dense gas surrounding the AGN. Analysis of the kinematics shows large [...]]]></description>
			<content:encoded><![CDATA[<p>We present new ~1&#8243; resolution data of the dense molecular gas in the central 50-100 pc of four nearby Seyfert galaxies. PdBI observations of HCN and, in 2 of the 4 sources, simultaneously HCO+ allow us to carefully constrain the dynamical state of the dense gas surrounding the AGN. Analysis of the kinematics shows large line widths of 100-200 km/s FWHM that can only partially arise from beam smearing of the velocity gradient. The observed morphological and kinematic parameters (dimensions, major axis position angle, red and blue channel separation, and integrated line width) are well reproduced by a thick disk, where the emitting dense gas has a large intrinsic dispersion (20-40 km/s), implying that it exists at significant scale heights (25-30% of the disk radius). To put the observed kinematics in the context of the starburst and AGN evolution, we estimate the Toomre Q parameter. We find this is always greater than the critical value, i.e. Q is above the limit such that the gas is stable against rapid star formation. This is supported by the lack of direct evidence, in these 4 Seyfert galaxies, for on-going star formation close around the AGN. Instead, any current star formation tends to be located in a circumnuclear ring. We conclude that the physical conditions are indeed not suited to star formation within the central ~100 pc.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/physical-properties-of-dense-molecular-gas-in-centres-of-seyfert-galaxies/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A multi-wavelength investigation of RCW175: an HII region harboring spinning dust emission</title>
		<link>http://voxcharta.org/2012/05/21/a-multi-wavelength-investigation-of-rcw175-an-hii-region-harboring-spinning-dust-emission/</link>
		<comments>http://voxcharta.org/2012/05/21/a-multi-wavelength-investigation-of-rcw175-an-hii-region-harboring-spinning-dust-emission/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:52:19 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[aromatic hydrocarbon]]></category>
		<category><![CDATA[dust emission]]></category>
		<category><![CDATA[dust grains]]></category>
		<category><![CDATA[emission mechanism]]></category>
		<category><![CDATA[hii region]]></category>
		<category><![CDATA[interstellar medium]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[microwave emission]]></category>
		<category><![CDATA[molecular cloud]]></category>
		<category><![CDATA[pivotal role]]></category>
		<category><![CDATA[radiation field]]></category>
		<category><![CDATA[radio continuum]]></category>
		<category><![CDATA[spectral observation]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[stellar object]]></category>
		<category><![CDATA[vicinity]]></category>
		<category><![CDATA[wavelength]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/a-multi-wavelength-investigation-of-rcw175-an-hii-region-harboring-spinning-dust-emission/</guid>
		<description><![CDATA[Using infrared, radio continuum and spectral observations, we performed a detailed investigation of the HII region RCW175. We determined that RCW175, which actually consists of two separate HII regions, G29.1-0.7 and G29.0-0.6, is located at a distance of 3.2+/-0.2 kpc. Based on the observations we infer that the more compact G29.0-0.6 is less evolved than [...]]]></description>
			<content:encoded><![CDATA[<p>Using infrared, radio continuum and spectral observations, we performed a detailed investigation of the HII region RCW175. We determined that RCW175, which actually consists of two separate HII regions, G29.1-0.7 and G29.0-0.6, is located at a distance of 3.2+/-0.2 kpc. Based on the observations we infer that the more compact G29.0-0.6 is less evolved than G29.1-0.7 and was possibly produced as a result of the expansion of G29.1-0.7 into the surrounding interstellar medium. We compute a star formation rate for RCW175 of (12.6+/-1.9)x10^{-5} M_{\sun}/yr, and identified 6 possible young stellar object candidates within its vicinity. Additionally, we estimate that RCW175 contains a total dust mass of 215+/-53 M_{\sun}.   RCW175 has previously been identified as a source of anomalous microwave emission (AME), an excess of emission at cm wavelengths often attributed to electric dipole radiation from the smallest dust grains. We find that the AME previously detected in RCW175 is not correlated with the smallest dust grains (polycyclic aromatic hydrocarbons or small carbonaceous dust grains), but rather with the exciting radiation field within the region. This is a similar result to that found in the Perseus molecular cloud, another region which harbors AME, suggesting that the radiation field may play a pivotal role in the production of this new Galactic emission mechanism. Finally, we suggest that these observations may hint at the importance of understanding the role played by the major gas ions in spinning dust models.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/a-multi-wavelength-investigation-of-rcw175-an-hii-region-harboring-spinning-dust-emission/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The universal density profile of the central region of dark matter haloes</title>
		<link>http://voxcharta.org/2012/05/21/the-universal-density-profile-of-the-central-region-of-dark-matter-haloes/</link>
		<comments>http://voxcharta.org/2012/05/21/the-universal-density-profile-of-the-central-region-of-dark-matter-haloes/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:50:11 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[body simulation]]></category>
		<category><![CDATA[central core]]></category>
		<category><![CDATA[cusp]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[density profile]]></category>
		<category><![CDATA[extent]]></category>
		<category><![CDATA[initial condition]]></category>
		<category><![CDATA[perturbation]]></category>
		<category><![CDATA[structure formation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/the-universal-density-profile-of-the-central-region-of-dark-matter-haloes/</guid>
		<description><![CDATA[We consider the density profile of the central region of dark matter haloes. It turns out that under very general conditions the profile is universal: it depends almost not at all on the properties of the initial perturbation and is very akin, but not identical, to the Einasto profile.   We estimate the size [...]]]></description>
			<content:encoded><![CDATA[<p>We consider the density profile of the central region of dark matter haloes. It turns out that under very general conditions the profile is universal: it depends almost not at all on the properties of the initial perturbation and is very akin, but not identical, to the Einasto profile.   We estimate the size of the &#8216;central core&#8217; of the distribution, i.e., the extent of the very central region with a respectively gentle profile, and show that the cusp formation is unlikely, even if the dark matter is cold. We also indicate that the density profile of the outer part ($r&gt;0.5 R_{vir}$) of the haloes significantly depends on the initial conditions and should not be universal, in contrast to the central area. All these results can be useful both to indirect search of the dark matter and to N-body simulations of the structure formation.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/the-universal-density-profile-of-the-central-region-of-dark-matter-haloes/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>On turbulent fragmentation and the origin of the stellar IMF</title>
		<link>http://voxcharta.org/2012/05/21/on-turbulent-fragmentation-and-the-origin-of-the-stellar-imf/</link>
		<comments>http://voxcharta.org/2012/05/21/on-turbulent-fragmentation-and-the-origin-of-the-stellar-imf/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:45:13 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[chabrier]]></category>
		<category><![CDATA[characteristic temperature]]></category>
		<category><![CDATA[clump]]></category>
		<category><![CDATA[conversion efficiency]]></category>
		<category><![CDATA[dynamic processes]]></category>
		<category><![CDATA[gas temperature]]></category>
		<category><![CDATA[initial mass function]]></category>
		<category><![CDATA[interstellar medium]]></category>
		<category><![CDATA[kroupa]]></category>
		<category><![CDATA[last decade]]></category>
		<category><![CDATA[lognormal distribution]]></category>
		<category><![CDATA[mass function]]></category>
		<category><![CDATA[power spectrum]]></category>
		<category><![CDATA[random choice]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[spatial scale]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[stellar imf]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[universal nature]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/on-turbulent-fragmentation-and-the-origin-of-the-stellar-imf/</guid>
		<description><![CDATA[Two varieties of the universal stellar initial mass function (IMF) viz., the Kroupa and the Chabrier IMF, have emerged over the last decade to explain the observed distribution of stellar masses. The possibility of the universal nature of the stellar IMF leads us to the interesting prospect of a universal mode of star-formation. It is [...]]]></description>
			<content:encoded><![CDATA[<p>Two varieties of the universal stellar initial mass function (IMF) viz., the Kroupa and the Chabrier IMF, have emerged over the last decade to explain the observed distribution of stellar masses. The possibility of the universal nature of the stellar IMF leads us to the interesting prospect of a universal mode of star-formation. It is well-known that turbulent fragmentation of gas in the interstellar medium produces a lognormal distribution of density which is further reflected by the mass-function for clumps at low and intermediate masses. Stars condense out of unstable clumps through a complex interplay between a number of dynamic processes which must be accounted for when tracing the origin of the stellar IMF. In the present work, applying the theory of gravitational fragmentation we first derive the mass function (MF) for clumps. Then a core mass function (CMF) is derived by allowing the clumps to fragment, having subjected each one to a random choice of gas temperature. Finally, the stellar IMF is derived by applying a random core-to-star conversion efficiency, $\epsilon$, in the range of 5%-15% to each CMF. We obtain a power-law IMF that has exponents within the error-bars on the Kropua IMF. This derived IMF is preceded by a similar core mass function which suggests, gravoturbulent fragmentation plays a key role in assembling necessary conditions that relate the two mass-functions. In this sense the star-formation process, at least at low redshifts where gas cooling is efficient, is likely to be universal. We argue that the observed knee in the CMF and the stellar IMF may alternatively be interpreted in terms of the characteristic temperature at which gas in potential star-forming clouds is likely to be found. Our results also show that turbulence in star-forming clouds is probably driven on large spatial scales with a power-spectrum steeper than Kolmogorov-type.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/on-turbulent-fragmentation-and-the-origin-of-the-stellar-imf/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>On the nature of dust clouds in the region towards M81 and NGC3077</title>
		<link>http://voxcharta.org/2012/05/21/on-the-nature-of-dust-clouds-in-the-region-towards-m81-and-ngc3077/</link>
		<comments>http://voxcharta.org/2012/05/21/on-the-nature-of-dust-clouds-in-the-region-towards-m81-and-ngc3077/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:44:55 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cm 2]]></category>
		<category><![CDATA[co line]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[dust cloud]]></category>
		<category><![CDATA[dust emission]]></category>
		<category><![CDATA[galactic foreground]]></category>
		<category><![CDATA[galactic origin]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[herschel]]></category>
		<category><![CDATA[iram]]></category>
		<category><![CDATA[line emission]]></category>
		<category><![CDATA[m81]]></category>
		<category><![CDATA[m82]]></category>
		<category><![CDATA[map]]></category>
		<category><![CDATA[mip]]></category>
		<category><![CDATA[molecular structure]]></category>
		<category><![CDATA[physical parameter]]></category>
		<category><![CDATA[radio telescope]]></category>
		<category><![CDATA[spire]]></category>
		<category><![CDATA[Spitzer]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/on-the-nature-of-dust-clouds-in-the-region-towards-m81-and-ngc3077/</guid>
		<description><![CDATA[There is some controversy on the nature of dust clouds found in direction of the interacting galaxy triplett M81, M82, and NGC3077. Are they associated with the tidal arms seen in HI around those galaxies or are they simply Galactic foreground clouds? Data from the SPIRE instrument onboard HERSCHEL and MIPS onboard of SPITZER are [...]]]></description>
			<content:encoded><![CDATA[<p>There is some controversy on the nature of dust clouds found in direction of the interacting galaxy triplett M81, M82, and NGC3077. Are they associated with the tidal arms seen in HI around those galaxies or are they simply Galactic foreground clouds? Data from the SPIRE instrument onboard HERSCHEL and MIPS onboard of SPITZER are used to derive physical parameters for the dust clouds. These observions are compared to CO clouds previously mapped with the IRAM and the FCRAO radio telescopes.SPIRE and MIPS maps show several dust clouds north of M81 and south of NGC3077. Modelling of the dust emission provides total hydrogen column densities between 1.5 and 5.0 * 10^20 cm^-2. Dust temperatures are between 13 to 17K. No significant difference in the dust emission can be found between individual clouds. It is shown that CO line emission provides the best clues on the origin of those clouds. Most of the clouds seen towards M81 are associated with small-area molecular structures (SAMS), i.e. tiny CO clouds of Galactic origin. The clouds seen towards NGC3077 are partly associated with the tidal arms and are partly in the Galactic foreground associated with SAMS.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/on-the-nature-of-dust-clouds-in-the-region-towards-m81-and-ngc3077/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Neutrinos from WIMP annihilation in the Sun : Implications of a self-consistent model of the Milky Way&#8217;s dark matter halo [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/neutrinos-from-wimp-annihilation-in-the-sun-implications-of-a-self-consistent-model-of-the-milky-ways-dark-matter-halo-replacement-2/</link>
		<comments>http://voxcharta.org/2012/05/21/neutrinos-from-wimp-annihilation-in-the-sun-implications-of-a-self-consistent-model-of-the-milky-ways-dark-matter-halo-replacement-2/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:38:51 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[annihilation]]></category>
		<category><![CDATA[consistent model]]></category>
		<category><![CDATA[cross section]]></category>
		<category><![CDATA[curve data]]></category>
		<category><![CDATA[dark matter halo]]></category>
		<category><![CDATA[finite size]]></category>
		<category><![CDATA[frame work]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[neutrino]]></category>
		<category><![CDATA[neutrino flux]]></category>
		<category><![CDATA[null result]]></category>
		<category><![CDATA[parameter space]]></category>
		<category><![CDATA[proton]]></category>
		<category><![CDATA[rotation curve]]></category>
		<category><![CDATA[stringent restrictions]]></category>
		<category><![CDATA[super kamiokande]]></category>
		<category><![CDATA[wimp]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/neutrinos-from-wimp-annihilation-in-the-sun-implications-of-a-self-consistent-model-of-the-milky-ways-dark-matter-halo-replacement-2/</guid>
		<description><![CDATA[Upper limits on the spin-independent (SI) as well as spin-dependent (SD) elastic scattering cross sections of WIMPs with protons, imposed by the Super-Kamiokande (S-K) upper limit on the neutrino flux from WIMP annihilation in the Sun, and their compatibility with the &#8220;DAMA-compatible&#8221; regions of the WIMP parameter space within which the annual modulation signal observed [...]]]></description>
			<content:encoded><![CDATA[<p>Upper limits on the spin-independent (SI) as well as spin-dependent (SD) elastic scattering cross sections of WIMPs with protons, imposed by the Super-Kamiokande (S-K) upper limit on the neutrino flux from WIMP annihilation in the Sun, and their compatibility with the &#8220;DAMA-compatible&#8221; regions of the WIMP parameter space within which the annual modulation signal observed by the DAMA/LIBRA experiment is compatible with the null results of other direct detection experiments, are studied within the frame work of a self-consistent model of the finite-size dark matter (DM) halo of the Galaxy, the parameters of which are determined by a fit to the rotation curve data of the Galaxy. We find that the S-K implied upper limits on the WIMP-proton elastic cross section as a function of WIMP mass impose stringent restrictions on the branching fractions of the various WIMP annihilation channels. For SI interaction, while the S-K upper limits are consistent with the DAMA-compatible region of the WIMP parameter space if the WIMPs annihilate dominantly to $\bbarb$\ and/or $\cbarc$, portions of the DAMA-compatible region can be excluded if WIMP annihilations to $\tautau$ and $\nu\anu$ occur at larger than ~ 10% and 0.1% levels, respectively. For SD interaction, the restrictions on the possible annihilation channels are much more stringent, essentially ruling out the DAMA-compatible region of the WIMP parameter space if the relatively low-mass ($\sim$ 2 &#8212; 20 GeV) WIMPs under consideration annihilate predominantly to any mixture of $\bbarb$, \ $\cbarc$, \ $\tautau$, \ and $\nu\anu$ final states.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/neutrinos-from-wimp-annihilation-in-the-sun-implications-of-a-self-consistent-model-of-the-milky-ways-dark-matter-halo-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>The spatial structure of mono-abundance sub-populations of the Milky Way disk [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/the-spatial-structure-of-mono-abundance-sub-populations-of-the-milky-way-disk-replacement-2/</link>
		<comments>http://voxcharta.org/2012/05/21/the-spatial-structure-of-mono-abundance-sub-populations-of-the-milky-way-disk-replacement-2/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:38:18 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[decomposition]]></category>
		<category><![CDATA[elemental abundance]]></category>
		<category><![CDATA[galactic disk]]></category>
		<category><![CDATA[inevitable consequence]]></category>
		<category><![CDATA[internal evolution]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[number density]]></category>
		<category><![CDATA[photometric data]]></category>
		<category><![CDATA[population]]></category>
		<category><![CDATA[radial direction]]></category>
		<category><![CDATA[spatial structure]]></category>
		<category><![CDATA[spectroscopic survey]]></category>
		<category><![CDATA[stellar disk]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[thin disk]]></category>
		<category><![CDATA[vertical structure]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/the-spatial-structure-of-mono-abundance-sub-populations-of-the-milky-way-disk-replacement-2/</guid>
		<description><![CDATA[The spatial, kinematic, and elemental-abundance structure of the Milky Way&#8217;s stellar disk is complex, and has been difficult to dissect with local spectroscopic or global photometric data. Here, we develop and apply a rigorous density modeling approach for Galactic spectroscopic surveys that enables investigation of the global spatial structure of stellar sub-populations in narrow bins [...]]]></description>
			<content:encoded><![CDATA[<p>The spatial, kinematic, and elemental-abundance structure of the Milky Way&#8217;s stellar disk is complex, and has been difficult to dissect with local spectroscopic or global photometric data. Here, we develop and apply a rigorous density modeling approach for Galactic spectroscopic surveys that enables investigation of the global spatial structure of stellar sub-populations in narrow bins of [\alpha/Fe] and [Fe/H], using 23,767 G-type dwarfs from SDSS/SEGUE. We fit models for the number density of each such mono-abundance component, properly accounting for the complex spectroscopic SEGUE sampling of the underlying stellar population. We find that each mono-abundance sub-population has a simple spatial structure that can be described by a single exponential in both the vertical and radial direction, with continuously increasing scale heights (~200 pc to 1 kpc) and decreasing scale lengths (&gt;4.5 kpc to 2 kpc) for increasingly older sub-populations, as indicated by their lower metallicities and [\alpha/Fe] enhancements. That the abundance-selected sub-components with the largest scale heights have the shortest scale lengths is in sharp contrast with purely geometric `thick&#8211;thin disk&#8217; decompositions. To the extent that [\alpha/Fe] is an adequate proxy for age, our results directly show that older disk sub-populations are more centrally concentrated, which implies inside-out formation of galactic disks. The fact that the largest scale-height sub-components are most centrally concentrated in the Milky Way is an almost inevitable consequence of explaining the vertical structure of the disk through internal evolution. Whether the simple spatial structure of the mono-abundance sub-components, and the striking correlations between age, scale length, and scale height can be plausibly explained by satellite accretion or other external heating remains to be seen.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/the-spatial-structure-of-mono-abundance-sub-populations-of-the-milky-way-disk-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Modified Newtonian Dynamics (MOND): Observational Phenomenology and Relativistic Extensions [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/modified-newtonian-dynamics-mond-observational-phenomenology-and-relativistic-extensions-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/modified-newtonian-dynamics-mond-observational-phenomenology-and-relativistic-extensions-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:38:08 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration]]></category>
		<category><![CDATA[astronomical data]]></category>
		<category><![CDATA[cosmological constant]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[discrepancy]]></category>
		<category><![CDATA[galactic scale]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[modified newtonian dynamics]]></category>
		<category><![CDATA[motion]]></category>
		<category><![CDATA[paradigm]]></category>
		<category><![CDATA[phenomenology]]></category>
		<category><![CDATA[relativistic theory]]></category>
		<category><![CDATA[square root]]></category>
		<category><![CDATA[successes]]></category>
		<category><![CDATA[surface density]]></category>
		<category><![CDATA[theoretical attempts]]></category>
		<category><![CDATA[theoretical framework]]></category>
		<category><![CDATA[theory of gravity]]></category>
		<category><![CDATA[universal force]]></category>
		<category><![CDATA[unseen mass]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/modified-newtonian-dynamics-mond-observational-phenomenology-and-relativistic-extensions-replacement/</guid>
		<description><![CDATA[A wealth of astronomical data indicate the presence of mass discrepancies in the Universe. The motions observed in a variety of classes of extragalactic systems exceed what can be explained by the mass visible in stars and gas. Either (i) there is a vast amount of unseen mass in some novel form &#8211; dark matter [...]]]></description>
			<content:encoded><![CDATA[<p>A wealth of astronomical data indicate the presence of mass discrepancies in the Universe. The motions observed in a variety of classes of extragalactic systems exceed what can be explained by the mass visible in stars and gas. Either (i) there is a vast amount of unseen mass in some novel form &#8211; dark matter &#8211; or (ii) the data indicate a breakdown of our understanding of dynamics on the relevant scales, or (iii) both. Here, we first review a few outstanding challenges for the dark matter interpretation of mass discrepancies in galaxies, purely based on observations and independently of any alternative theoretical framework. We then show that many of these puzzling observations are predicted by one single relation &#8211; Milgrom&#8217;s law &#8211; involving an acceleration constant (or a characteristic surface density) of the order of the square-root of the cosmological constant in natural units. This relation can at present most easily be interpreted as the effect of a single universal force law resulting from a modification of Newtonian dynamics (MOND) on galactic scales. We exhaustively review the current observational successes and problems of this alternative paradigm at all astrophysical scales, and summarize the various theoretical attempts (TeVeS, GEA, BIMOND, and others) made to effectively embed this modification of Newtonian dynamics within a relativistic theory of gravity.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/modified-newtonian-dynamics-mond-observational-phenomenology-and-relativistic-extensions-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Disruption of a Proto-Planetary Disk by the Black Hole at the Milky Way Centre [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/disruption-of-a-proto-planetary-disk-by-the-black-hole-at-the-milky-way-centre-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/disruption-of-a-proto-planetary-disk-by-the-black-hole-at-the-milky-way-centre-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:37:48 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[evaporation]]></category>
		<category><![CDATA[galactic centre]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[mass star]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[photo]]></category>
		<category><![CDATA[planetary disk]]></category>
		<category><![CDATA[planets]]></category>
		<category><![CDATA[proto]]></category>
		<category><![CDATA[schwarzschild radii]]></category>
		<category><![CDATA[sgra]]></category>
		<category><![CDATA[supermassive black hole]]></category>
		<category><![CDATA[tidal debris]]></category>
		<category><![CDATA[tidal disruption]]></category>
		<category><![CDATA[young stars]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/disruption-of-a-proto-planetary-disk-by-the-black-hole-at-the-milky-way-centre-replacement/</guid>
		<description><![CDATA[Recently, Gillessen et al. discovered an ionized cloud of gas plunging toward the supermassive black hole, SgrA*, at the centre of the Milky Way. The cloud is being tidally disrupted along its path to closest approach at ~3100 Schwarzschild radii from the black hole. Here, we show that the observed properties of this cloud of [...]]]></description>
			<content:encoded><![CDATA[<p>Recently, Gillessen et al. discovered an ionized cloud of gas plunging toward the supermassive black hole, SgrA*, at the centre of the Milky Way. The cloud is being tidally disrupted along its path to closest approach at ~3100 Schwarzschild radii from the black hole. Here, we show that the observed properties of this cloud of gas can naturally be produced by a proto-planetary disk surrounding a low-mass star, which was scattered from the observed ring of young stars orbiting Sgr A*. As the young star approaches the black hole, its disk experiences both photo-evaporation and tidal disruption, producing a cloud. Our model implies that planets form in the Galactic centre, and that tidal debris from proto-planetary disks can flag low mass stars which are otherwise too faint to be detected.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/disruption-of-a-proto-planetary-disk-by-the-black-hole-at-the-milky-way-centre-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Probing cluster dynamics in RXCJ1504.1-0248 via radial and two-dimensional gas and galaxy properties [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/probing-cluster-dynamics-in-rxcj1504-1-0248-via-radial-and-two-dimensional-gas-and-galaxy-properties-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/probing-cluster-dynamics-in-rxcj1504-1-0248-via-radial-and-two-dimensional-gas-and-galaxy-properties-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:32:55 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[calibration]]></category>
		<category><![CDATA[centroid]]></category>
		<category><![CDATA[cluster dynamics]]></category>
		<category><![CDATA[cluster of galaxies]]></category>
		<category><![CDATA[dimensional gas]]></category>
		<category><![CDATA[galaxy properties]]></category>
		<category><![CDATA[global property]]></category>
		<category><![CDATA[high velocity]]></category>
		<category><![CDATA[line of sight]]></category>
		<category><![CDATA[mass distribution]]></category>
		<category><![CDATA[mass fraction]]></category>
		<category><![CDATA[nearby cluster]]></category>
		<category><![CDATA[optical imaging]]></category>
		<category><![CDATA[optical spectroscopy]]></category>
		<category><![CDATA[pressure maps]]></category>
		<category><![CDATA[reflex survey]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[substructure]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xmm newton]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/probing-cluster-dynamics-in-rxcj1504-1-0248-via-radial-and-two-dimensional-gas-and-galaxy-properties-replacement/</guid>
		<description><![CDATA[We studied one of the most X-ray luminous cluster of galaxies in the REFLEX survey, RXC J1504.1-0248 (hereafter R1504; z=0.2153), using XMM-Newton X-ray imaging spectroscopy, VLT/VIMOS optical spectroscopy, and WFI optical imaging. The mass distributions were determined using both the so-called hydrostatic method with X-ray imaging spectroscopy and the dynamical method with optical spectroscopy, respectively, [...]]]></description>
			<content:encoded><![CDATA[<p>We studied one of the most X-ray luminous cluster of galaxies in the REFLEX survey, RXC J1504.1-0248 (hereafter R1504; z=0.2153), using XMM-Newton X-ray imaging spectroscopy, VLT/VIMOS optical spectroscopy, and WFI optical imaging. The mass distributions were determined using both the so-called hydrostatic method with X-ray imaging spectroscopy and the dynamical method with optical spectroscopy, respectively, which yield M^{H.E.}_{500}=(5.81+/-0.49)*1.e14Msun and M^{caustic}_{500}=(4.17+/-0.42)*1e14Msun. According to recent calibrations, the richness derived mass estimates closely agree with the hydrostatic and dynamical mass estimates. The line-of-sight velocities of spectroscopic members reveal a group of galaxies with high-velocities (&gt;1000 km/s) at a projected distance of about r^{H.E.}_{500}=(1.18+/-0.03) Mpc south-east of the cluster centroid, which is also indicated in the X-ray two-dimensional (2-D) temperature, density, entropy, and pressure maps. The dynamical mass estimate is 80% of the hydrostatic mass estimate at r^{H.E.}_{500}. It can be partially explained by the ~20% scatter in the 2-D pressure map that can be propagated into the hydrostatic mass estimate. The uncertainty in the dynamical mass estimate caused by the substructure of the high velocity group is ~14%. The dynamical mass estimate using blue members is 1.23 times that using red members. The global properties of R1504 obey the observed scaling relations of nearby clusters, although its stellar-mass fraction is rather low.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/probing-cluster-dynamics-in-rxcj1504-1-0248-via-radial-and-two-dimensional-gas-and-galaxy-properties-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>870 micron Imaging of a Transitional Disk in Upper Scorpius: Holdover from the Era of Giant Planet Formation? [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/870-micron-imaging-of-a-transitional-disk-in-upper-scorpius-holdover-from-the-era-of-giant-planet-formation-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/870-micron-imaging-of-a-transitional-disk-in-upper-scorpius-holdover-from-the-era-of-giant-planet-formation-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:31:35 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[binary companion]]></category>
		<category><![CDATA[giant planet]]></category>
		<category><![CDATA[giant planet formation]]></category>
		<category><![CDATA[grains]]></category>
		<category><![CDATA[holdover]]></category>
		<category><![CDATA[images]]></category>
		<category><![CDATA[inner cavity]]></category>
		<category><![CDATA[jupiter masses]]></category>
		<category><![CDATA[micron imaging]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[solar mass star]]></category>
		<category><![CDATA[spectral energy distribution]]></category>
		<category><![CDATA[surface density]]></category>
		<category><![CDATA[transition]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/870-micron-imaging-of-a-transitional-disk-in-upper-scorpius-holdover-from-the-era-of-giant-planet-formation-replacement/</guid>
		<description><![CDATA[We present 880 micron images of the transition disk around the star [PZ99] J160421.7-213028, a solar-mass star in the nearby Upper Scorpius association. With a resolution down to 0.34 arcsec, we resolve the inner hole in this disk, and via model fitting to the visibilities and spectral energy distribution we determine both the structure of [...]]]></description>
			<content:encoded><![CDATA[<p>We present 880 micron images of the transition disk around the star [PZ99] J160421.7-213028, a solar-mass star in the nearby Upper Scorpius association. With a resolution down to 0.34 arcsec, we resolve the inner hole in this disk, and via model fitting to the visibilities and spectral energy distribution we determine both the structure of the outer region and the presence of sparse dust within the cavity. The disk contains about 0.1 Jupiter masses of mm-emitting grains, with an inner disk edge of about 70 AU. The inner cavity contains a small amount of dust with a depleted surface density in a region extending from about 20-70 AU. Taking into account prior observations indicating little to no stellar accretion, the lack of a binary companion, and the presence of dust near 0.1 AU, we determine that the most likely mechanism for the formation of this inner hole is the presence of one or more giant planets.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/870-micron-imaging-of-a-transitional-disk-in-upper-scorpius-holdover-from-the-era-of-giant-planet-formation-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Secular Dynamical Anti-Friction in Galactic Nuclei</title>
		<link>http://voxcharta.org/2012/05/20/secular-dynamical-anti-friction-in-galactic-nuclei/</link>
		<comments>http://voxcharta.org/2012/05/20/secular-dynamical-anti-friction-in-galactic-nuclei/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:46:03 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[body simulation]]></category>
		<category><![CDATA[central star]]></category>
		<category><![CDATA[cluster]]></category>
		<category><![CDATA[eccentric orbit]]></category>
		<category><![CDATA[friction]]></category>
		<category><![CDATA[galactic nuclei]]></category>
		<category><![CDATA[imbh]]></category>
		<category><![CDATA[initial stage]]></category>
		<category><![CDATA[migration rate]]></category>
		<category><![CDATA[numerical experiment]]></category>
		<category><![CDATA[orbital eccentricity]]></category>
		<category><![CDATA[orbital motion]]></category>
		<category><![CDATA[precession]]></category>
		<category><![CDATA[sdaf]]></category>
		<category><![CDATA[star cluster]]></category>
		<category><![CDATA[stellar cluster]]></category>
		<category><![CDATA[supermassive black hole]]></category>
		<category><![CDATA[torque]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/secular-dynamical-anti-friction-in-galactic-nuclei/</guid>
		<description><![CDATA[We identify a gravitational-dynamical process in near-Keplerian potentials of galactic nuclei that occurs when an intermediate-mass black hole (IMBH) is migrating on an eccentric orbit through the stellar cluster towards the central supermassive black hole (SMBH). We find that, apart from conventional dynamical friction, the IMBH experiences an often much stronger systematic torque due to [...]]]></description>
			<content:encoded><![CDATA[<p>We identify a gravitational-dynamical process in near-Keplerian potentials of galactic nuclei that occurs when an intermediate-mass black hole (IMBH) is migrating on an eccentric orbit through the stellar cluster towards the central supermassive black hole (SMBH). We find that, apart from conventional dynamical friction, the IMBH experiences an often much stronger systematic torque due to the secular (i.e., orbit-averaged) interactions with the cluster&#8217;s stars. The force which results in this torque is applied, counterintuitively, in the same direction as the IMBH&#8217;s precession and we refer to its action as &#8220;secular-dynamical anti-friction&#8221; (SDAF). We argue that SDAF, and not the gravitational ejection of stars, is responsible for the IMBH&#8217;s eccentricity increase seen in the initial stages of previous N-body simulations. Our numerical experiments, supported by qualitative arguments, demonstrate that (1) when the IMBH&#8217;s precession direction is artificially reversed, the torque changes sign as well, which decreases the orbital eccentricity, (2) the rate of eccentricity growth is sensitive to the IMBH migration rate, with zero systematic eccentricity growth for an IMBH whose orbit is artificially prevented from inward migration, and (3) SDAF is the strongest when the central star cluster is rapidly rotating. This leads to eccentricity growth/decrease for the clusters rotating in the opposite/same direction relative to the IMBH&#8217;s orbital motion.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/secular-dynamical-anti-friction-in-galactic-nuclei/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>High-velocity stars in the cores of globular clusters: The illustrative case of NGC 2808</title>
		<link>http://voxcharta.org/2012/05/20/high-velocity-stars-in-the-cores-of-globular-clusters-the-illustrative-case-of-ngc-2808/</link>
		<comments>http://voxcharta.org/2012/05/20/high-velocity-stars-in-the-cores-of-globular-clusters-the-illustrative-case-of-ngc-2808/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:45:21 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cluster member]]></category>
		<category><![CDATA[compact object]]></category>
		<category><![CDATA[escape velocity]]></category>
		<category><![CDATA[field spectroscopy]]></category>
		<category><![CDATA[giant branch]]></category>
		<category><![CDATA[giant phase]]></category>
		<category><![CDATA[globular cluster]]></category>
		<category><![CDATA[globular cluster ngc]]></category>
		<category><![CDATA[high velocity]]></category>
		<category><![CDATA[illustrative case]]></category>
		<category><![CDATA[integral field]]></category>
		<category><![CDATA[main sequence star]]></category>
		<category><![CDATA[monte carlo simulation]]></category>
		<category><![CDATA[numerical simulation]]></category>
		<category><![CDATA[red giant]]></category>
		<category><![CDATA[sigma c]]></category>
		<category><![CDATA[spectroscopy data]]></category>
		<category><![CDATA[velocities]]></category>
		<category><![CDATA[velocity dispersion]]></category>
		<category><![CDATA[velocity distribution]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/high-velocity-stars-in-the-cores-of-globular-clusters-the-illustrative-case-of-ngc-2808/</guid>
		<description><![CDATA[We report the detection of five high-velocity stars in the core of the globular cluster NGC 2808. The stars lie on the the red giant branch and show total velocities between 40 and 45 km/s. For a core velocity dispersion sigma_c = 13.4 km/s, this corresponds to up to 3.4 sigma_c. These velocities are close [...]]]></description>
			<content:encoded><![CDATA[<p>We report the detection of five high-velocity stars in the core of the globular cluster NGC 2808. The stars lie on the the red giant branch and show total velocities between 40 and 45 km/s. For a core velocity dispersion sigma_c = 13.4 km/s, this corresponds to up to 3.4 sigma_c. These velocities are close to the estimated escape velocity (~ 50 km/s) and suggest an ejection from the core. Two of these stars have been confirmed in our recent integral field spectroscopy data and we will discuss them in more detail here. These two red giants are located at a projected distance of ~ 0.3 pc from the center. According to their positions on the color magnitude diagram, both stars are cluster members. We investigate several possible origins for the high velocities of the stars and conceivable ejection mechanisms. Since the velocities are close to the escape velocity, it is not obvious whether the stars are bound or unbound to the cluster. We therefore consider both cases in our analysis. We perform numerical simulations of three-body dynamical encounters between binaries and single stars and compare the resulting velocity distributions of escapers with the velocities of our stars. We compare the predictions for a single dynamical encounter with a compact object with those of a sequence of two-body encounters due to relaxation. If the stars are unbound, the encounter must have taken place recently, when the stars were already in the giant phase. After including binary fractions and black-hole retention fractions, projection effects, and detection probabilities from Monte-Carlo simulations, we estimate the expected numbers of detections for all the different scenarios. Based on these numbers, we conclude that the most likely scenario is that the stars are bound and were accelerated by a single encounter between a binary of main-sequence stars and a ~ 10 M_sun black hole.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/high-velocity-stars-in-the-cores-of-globular-clusters-the-illustrative-case-of-ngc-2808/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>On the local dark matter density</title>
		<link>http://voxcharta.org/2012/05/20/on-the-local-dark-matter-density/</link>
		<comments>http://voxcharta.org/2012/05/20/on-the-local-dark-matter-density/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:43:56 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[approximation]]></category>
		<category><![CDATA[circular speed]]></category>
		<category><![CDATA[cm 3]]></category>
		<category><![CDATA[correct assumption]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[estimates]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[mass model]]></category>
		<category><![CDATA[matter density]]></category>
		<category><![CDATA[Measurement]]></category>
		<category><![CDATA[order of magnitude]]></category>
		<category><![CDATA[pc 3]]></category>
		<category><![CDATA[radius]]></category>
		<category><![CDATA[tracers]]></category>
		<category><![CDATA[velocity curve]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/on-the-local-dark-matter-density/</guid>
		<description><![CDATA[An analysis of the kinematics of 412 stars at 1-4 kpc from the Galactic mid-plane by Moni Bidin et al. (2012) has claimed to derive a local density of dark matter that is an order of magnitude below standard expectations. We show that this result is incorrect and that it arises from the invalid assumption [...]]]></description>
			<content:encoded><![CDATA[<p>An analysis of the kinematics of 412 stars at 1-4 kpc from the Galactic mid-plane by Moni Bidin et al. (2012) has claimed to derive a local density of dark matter that is an order of magnitude below standard expectations. We show that this result is incorrect and that it arises from the invalid assumption that the mean azimuthal velocity of the stellar tracers is independent of Galactocentric radius at all heights; the correct assumption&#8212;that is, the one supported by data&#8212;is that the circular speed is independent of radius in the mid-plane. We demonstrate that the assumption of constant mean azimuthal velocity is physically implausible by showing that it requires the circular velocity to drop more steeply than allowed by any plausible mass model, with or without dark matter, at large heights above the mid-plane. Using the correct approximation that the circular velocity curve is flat in the mid-plane, we find that the data imply a local dark-matter density of 0.008 +/- 0.002 Msun/pc^3= 0.3 +/- 0.1 Gev/cm^3, fully consistent with standard estimates of this quantity. This is the most robust direct measurement of the local dark-matter density to date.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/on-the-local-dark-matter-density/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Synchrotron Spectral Curvature from 22 MHz to 23 GHz</title>
		<link>http://voxcharta.org/2012/05/20/synchrotron-spectral-curvature-from-22-mhz-to-23-ghz/</link>
		<comments>http://voxcharta.org/2012/05/20/synchrotron-spectral-curvature-from-22-mhz-to-23-ghz/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:41:47 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[arcade]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[curvature]]></category>
		<category><![CDATA[delta beta]]></category>
		<category><![CDATA[energy spectrum]]></category>
		<category><![CDATA[frequency data]]></category>
		<category><![CDATA[frequency spectrum]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[independent measurement]]></category>
		<category><![CDATA[law index]]></category>
		<category><![CDATA[low frequency]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[octave]]></category>
		<category><![CDATA[radio data]]></category>
		<category><![CDATA[radio sky]]></category>
		<category><![CDATA[radio spectrum]]></category>
		<category><![CDATA[spectral index]]></category>
		<category><![CDATA[survey]]></category>
		<category><![CDATA[synchrotron emission]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/synchrotron-spectral-curvature-from-22-mhz-to-23-ghz/</guid>
		<description><![CDATA[We combine surveys of the radio sky at frequencies 22 MHz to 1.4 GHz with data from the ARCADE-2 instrument at frequencies 3 to 10 GHz to characterize the frequency spectrum of diffuse synchrotron emission in the Galaxy. The radio spectrum steepens with frequency from 22 MHz to 10 GHz. The projected spectral index at [...]]]></description>
			<content:encoded><![CDATA[<p>We combine surveys of the radio sky at frequencies 22 MHz to 1.4 GHz with data from the ARCADE-2 instrument at frequencies 3 to 10 GHz to characterize the frequency spectrum of diffuse synchrotron emission in the Galaxy. The radio spectrum steepens with frequency from 22 MHz to 10 GHz. The projected spectral index at 23 GHz derived from the low-frequency data agrees well with independent measurements using only data at frequencies 23 GHz and above. Comparing the spectral index at 23 GHz to the value from previously published analyses allows extension of the model to higher frequencies. The combined data are consistent with a power-law index beta = -2.64 +/- 0.03 at 0.31 GHz, steepening by an amount Delta beta = 0.07 every octave in frequency. Comparison of the radio data to models including the cosmic ray energy spectrum suggests that any break in the synchrotron spectrum must occur at frequencies above 23 GHz.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/synchrotron-spectral-curvature-from-22-mhz-to-23-ghz/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Properties of dust in the Galactic center region probed by AKARI far-infrared spectral mapping &#8211; detection of a dust feature</title>
		<link>http://voxcharta.org/2012/05/20/properties-of-dust-in-the-galactic-center-region-probed-by-akari-far-infrared-spectral-mapping-detection-of-a-dust-feature/</link>
		<comments>http://voxcharta.org/2012/05/20/properties-of-dust-in-the-galactic-center-region-probed-by-akari-far-infrared-spectral-mapping-detection-of-a-dust-feature/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:39:10 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorption]]></category>
		<category><![CDATA[arches]]></category>
		<category><![CDATA[cluster]]></category>
		<category><![CDATA[dust component]]></category>
		<category><![CDATA[dust continuum emission]]></category>
		<category><![CDATA[fourier transform spectrometer]]></category>
		<category><![CDATA[galactic center region]]></category>
		<category><![CDATA[grains]]></category>
		<category><![CDATA[graphite]]></category>
		<category><![CDATA[intense radiation]]></category>
		<category><![CDATA[interstellar dust]]></category>
		<category><![CDATA[ionized gas]]></category>
		<category><![CDATA[micron]]></category>
		<category><![CDATA[spatial variation]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectrum]]></category>
		<category><![CDATA[surveyor]]></category>
		<category><![CDATA[temperature]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/properties-of-dust-in-the-galactic-center-region-probed-by-akari-far-infrared-spectral-mapping-detection-of-a-dust-feature/</guid>
		<description><![CDATA[We investigate the properties of interstellar dust in the Galactic center region toward the Arches and Quintuplet clusters. With the Fourier Transform Spectrometer of the AKARI/Far-Infrared Surveyor, we performed the far-infrared (60 &#8211; 140 cm^-1) spectral mapping of an area of about 10&#8242; x 10&#8242; which includes the two clusters to obtain a low-resolution (R [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate the properties of interstellar dust in the Galactic center region toward the Arches and Quintuplet clusters. With the Fourier Transform Spectrometer of the AKARI/Far-Infrared Surveyor, we performed the far-infrared (60 &#8211; 140 cm^-1) spectral mapping of an area of about 10&#8242; x 10&#8242; which includes the two clusters to obtain a low-resolution (R = 1.2 cm^-1) spectrum at every spatial bin of 30&#8243; x 30&#8243;. We derive the spatial variations of dust continuum emission at different wavenumbers, which are compared with those of the [O III] 88 micron (113 cm^-1) emission and the OH 119 micron (84 cm^-1) absorption. The spectral fitting shows that two dust modified blackbody components with temperatures of ~20 K and ~50 K can reproduce most of the continuum spectra. For some spectra, however, we find that there exists a significant excess on top of a modified blackbody continuum around 80 &#8211; 90 cm^-1 (110 &#8211; 130 microns). The warmer dust component is spatially correlated well with the [O III] emission and hence likely to be associated with the highly-ionized gas locally heated by intense radiation from the two clusters. The excess emission probably represents a dust feature, which is found to be spatially correlated with the OH absorption and a CO cloud. We find that a dust model including micron-sized graphite grains can reproduce the observed spectrum with the dust feature fairly well.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/properties-of-dust-in-the-galactic-center-region-probed-by-akari-far-infrared-spectral-mapping-detection-of-a-dust-feature/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>The molecular gas content of the Pipe Nebula I. Direct evidence of outflow-generated turbulence in B59?</title>
		<link>http://voxcharta.org/2012/05/20/the-molecular-gas-content-of-the-pipe-nebula-i-direct-evidence-of-outflow-generated-turbulence-in-b59/</link>
		<comments>http://voxcharta.org/2012/05/20/the-molecular-gas-content-of-the-pipe-nebula-i-direct-evidence-of-outflow-generated-turbulence-in-b59/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:38:45 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bow shock]]></category>
		<category><![CDATA[clump]]></category>
		<category><![CDATA[collapse]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[dense gas]]></category>
		<category><![CDATA[density material]]></category>
		<category><![CDATA[direct evidence]]></category>
		<category><![CDATA[energetics]]></category>
		<category><![CDATA[gas content]]></category>
		<category><![CDATA[hierarchical structure]]></category>
		<category><![CDATA[initial condition]]></category>
		<category><![CDATA[jcmt]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[molecular cloud]]></category>
		<category><![CDATA[outflow]]></category>
		<category><![CDATA[pipe nebula]]></category>
		<category><![CDATA[protostar]]></category>
		<category><![CDATA[quiet nature]]></category>
		<category><![CDATA[supersonic turbulence]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/the-molecular-gas-content-of-the-pipe-nebula-i-direct-evidence-of-outflow-generated-turbulence-in-b59/</guid>
		<description><![CDATA[The Pipe Nebula is a molecular cloud hosting the B59 region as its only active star-forming clump. While the particular importance of outflows in active star forming regions is subject of debate, the quiet nature of the gas in B59 makes it a good site to directly see the impact of protostellar feedback on the [...]]]></description>
			<content:encoded><![CDATA[<p>The Pipe Nebula is a molecular cloud hosting the B59 region as its only active star-forming clump. While the particular importance of outflows in active star forming regions is subject of debate, the quiet nature of the gas in B59 makes it a good site to directly see the impact of protostellar feedback on the quiescent dense gas. Using HARP at the JCMT, we mapped the B59 region with the J=3-2 transition of 12CO to study the kinematics and energetics of the outflows, and 13CO and C18O to study the overall dynamics of the ambient cloud, the physical properties of the gas, and the hierarchical structure of the region. The B59 region has a total of 30Msun of cold and quiescent material, mostly gravitationally bound, with narrow line widths throughout. Such low levels of turbulence in non-star-forming sites of B59 are indicative of the intrinsic initial conditions of the cloud. On the other hand, close to the forming protostars the impact of the outflows is observed as a localised increase of both line widths from 0.3 km/s to 1 km/s, and 13CO excitation temperatures by 2-3K. The impact of the outflows is also evident in the low column density material which shows signs of being pushed, shaped and carved by the outflow bow shocks as they pierce their way out of the cloud. Much of this structure is readily apparent in a dendrogram analysis of the cloud. B59&#8217;s low mass, intrinsically quiescent gas and small number of protostars, allows the identification of specific regions of the outflows&#8217; interaction with the dense gas. Our study suggests that outflows are an important mechanism in injecting and sustaining supersonic turbulence at sub-parsec scales. We find that only a fraction of the outflow energy is deposited as turbulent energy of the gas. This turbulent energy is sufficient to slow down the collapse of the region.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/the-molecular-gas-content-of-the-pipe-nebula-i-direct-evidence-of-outflow-generated-turbulence-in-b59/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Two distinct halo populations in the solar neighborhood. IV. Lithium abundances</title>
		<link>http://voxcharta.org/2012/05/20/two-distinct-halo-populations-in-the-solar-neighborhood-iv-lithium-abundances/</link>
		<comments>http://voxcharta.org/2012/05/20/two-distinct-halo-populations-in-the-solar-neighborhood-iv-lithium-abundances/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:38:22 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abundance]]></category>
		<category><![CDATA[bang nucleosynthesis]]></category>
		<category><![CDATA[big bang]]></category>
		<category><![CDATA[constants]]></category>
		<category><![CDATA[environmental effect]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[interpolating]]></category>
		<category><![CDATA[lii]]></category>
		<category><![CDATA[linear dependence]]></category>
		<category><![CDATA[Lithium]]></category>
		<category><![CDATA[main sequence]]></category>
		<category><![CDATA[model atmosphere]]></category>
		<category><![CDATA[resolution spectra]]></category>
		<category><![CDATA[solar neighborhood]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[wmap]]></category>
		<category><![CDATA[yonsei]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/two-distinct-halo-populations-in-the-solar-neighborhood-iv-lithium-abundances/</guid>
		<description><![CDATA[We investigate if there is a difference in the lithium abundances of stars belonging to two halo populations of F and G main-sequence stars previously found to differ in [alpha/Fe] for the metallicity range -1.4 &#60; [Fe/H] &#60; -0.7. Li abundances are derived from the LiI 6707.8 A line measured in high-resolution spectra using MARCS [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate if there is a difference in the lithium abundances of stars belonging to two halo populations of F and G main-sequence stars previously found to differ in [alpha/Fe] for the metallicity range -1.4 &lt; [Fe/H] &lt; -0.7. Li abundances are derived from the LiI 6707.8 A line measured in high-resolution spectra using MARCS model atmospheres. Furthermore, masses of the stars are determined from the logTeff &#8211; logg diagram by interpolating between Yonsei-Yale evolutionary tracks. There is no significant systematic difference in the lithium abundances of high- and low-alpha halo stars. For the large majority of stars with masses 0.7 &lt; M/M_sun &lt; 0.9 and heavy-element mass fractions 0.001 &lt; Z &lt; 0.006, the Li abundance is well fitted by a relation A(Li) = a0 + a1 M + a2 Z + a3 M Z, where a0, a1, a2, and a3 are constants. Extrapolating this relation to Z = 0 leads to a Li abundance close to the primordial value predicted from standard Big Bang nucleosynthesis calculations and the WMAP baryon density. The relation, however, does not apply to stars with [Fe/H] &lt; -1.5. We suggest that metal-rich halo stars were formed with a Li abundance close to the primordial value, and that lithium in their atmospheres has been depleted in time with an approximately linear dependence on stellar mass and Z. The lack of a systematic difference in the Li abundances of high- and low-alpha stars indicates that an environmental effect is not important for the destruction of lithium.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/two-distinct-halo-populations-in-the-solar-neighborhood-iv-lithium-abundances/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>The Green Bank Telescope HII Region Discovery Survey: III. Kinematic Distances</title>
		<link>http://voxcharta.org/2012/05/20/the-green-bank-telescope-hii-region-discovery-survey-iii-kinematic-distances/</link>
		<comments>http://voxcharta.org/2012/05/20/the-green-bank-telescope-hii-region-discovery-survey-iii-kinematic-distances/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:36:21 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[circular arc]]></category>
		<category><![CDATA[circular rotation]]></category>
		<category><![CDATA[galactic structure]]></category>
		<category><![CDATA[gbt]]></category>
		<category><![CDATA[green bank telescope]]></category>
		<category><![CDATA[hi emission]]></category>
		<category><![CDATA[hii region]]></category>
		<category><![CDATA[hrd]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[nebulae]]></category>
		<category><![CDATA[radii]]></category>
		<category><![CDATA[radio continuum emission]]></category>
		<category><![CDATA[recombination]]></category>
		<category><![CDATA[rotation curves]]></category>
		<category><![CDATA[rotation speed]]></category>
		<category><![CDATA[spiral structure]]></category>
		<category><![CDATA[structure results]]></category>
		<category><![CDATA[tangent point]]></category>
		<category><![CDATA[uncertainty analysis]]></category>
		<category><![CDATA[x band]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/the-green-bank-telescope-hii-region-discovery-survey-iii-kinematic-distances/</guid>
		<description><![CDATA[Using the HI Emission/Absorption method, we resolve the kinematic distance ambiguity and derive distances for 149 of 182 (82%) HII regions discovered by the Green Bank Telescope HII Region Discovery Survey (GBT HRDS). The HRDS is an X-band (9GHz, 3cm) GBT survey of 448 previously unknown HII regions in radio recombination line and radio continuum [...]]]></description>
			<content:encoded><![CDATA[<p>Using the HI Emission/Absorption method, we resolve the kinematic distance ambiguity and derive distances for 149 of 182 (82%) HII regions discovered by the Green Bank Telescope HII Region Discovery Survey (GBT HRDS). The HRDS is an X-band (9GHz, 3cm) GBT survey of 448 previously unknown HII regions in radio recombination line and radio continuum emission. Here we focus on HRDS sources from 67deg. &gt; l &gt; 18deg., where kinematic distances are more reliable. The 25 HRDS sources in this zone that have negative recombination line velocities are unambiguously beyond the orbit of the Sun, up to 20kpc distant. They are the most distant HII regions yet discovered. We find that 61% of HRDS sources are located at the far distance, 31% at the tangent point distance, and only 7% at the near distance. &#8220;Bubble&#8221; HII regions are not preferentially at the near distance (as was assumed previously) but average 10kpc from the Sun. The HRDS nebulae, when combined with a large sample of HII regions with previously known distances, show evidence of spiral structure in two circular arc segments of mean Galactocentric radii of 4.25 and 6.0kpc. We perform a thorough uncertainty analysis to analyze the effect of using different rotation curves, streaming motions, and a change to the Solar circular rotation speed. The median distance uncertainty for our sample of HII regions is only 0.5kpc, or 5%. This is significantly less than the median difference between the near and far kinematic distances, 6kpc. The basic Galactic structure results are unchanged after considering these sources of uncertainty.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/the-green-bank-telescope-hii-region-discovery-survey-iii-kinematic-distances/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Parameterizing the flattening of galaxies rotation curves on expanding locally anisotropic backgrounds [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/parameterizing-the-flattening-of-galaxies-rotation-curves-on-expanding-locally-anisotropic-backgrounds-replacement/</link>
		<comments>http://voxcharta.org/2012/05/20/parameterizing-the-flattening-of-galaxies-rotation-curves-on-expanding-locally-anisotropic-backgrounds-replacement/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:35:36 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[ansatz]]></category>
		<category><![CDATA[applicability]]></category>
		<category><![CDATA[density correction]]></category>
		<category><![CDATA[disk galaxy]]></category>
		<category><![CDATA[distributions]]></category>
		<category><![CDATA[energy density]]></category>
		<category><![CDATA[expanding universe]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[generalization]]></category>
		<category><![CDATA[gravitational interaction]]></category>
		<category><![CDATA[intermediate length]]></category>
		<category><![CDATA[length scales]]></category>
		<category><![CDATA[mass energy]]></category>
		<category><![CDATA[negative contributions]]></category>
		<category><![CDATA[parameterization]]></category>
		<category><![CDATA[physical parameter]]></category>
		<category><![CDATA[rotation curve]]></category>
		<category><![CDATA[rotation curves]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/parameterizing-the-flattening-of-galaxies-rotation-curves-on-expanding-locally-anisotropic-backgrounds-replacement/</guid>
		<description><![CDATA[In this work are discussed possible generalizations of the expanding locally anisotropic metric ansatz with respect to approximately Newtonian many body gravitational systems. This ansatz describes local point-like matter distributions on the expanding Universe also allowing for a covariant parameterization of gravitational interactions at intermediate length scales. As an example of applicability it is modelled [...]]]></description>
			<content:encoded><![CDATA[<p>In this work are discussed possible generalizations of the expanding locally anisotropic metric ansatz with respect to approximately Newtonian many body gravitational systems. This ansatz describes local point-like matter distributions on the expanding Universe also allowing for a covariant parameterization of gravitational interactions at intermediate length scales. As an example of applicability it is modelled a disk galaxy model matching the physical parameters of the galaxy UGC2885 and it is shown that, by fine-tuning the metric functional parameter, the flattening of the galaxy rotation curve is fully parameterized by this metric. It is further analysed the mass-energy density corrections due to the expanding anisotropic background being shown that although there are negative contributions within the galaxy plane the total mass-energy density is strictly positive. Outside the galaxy plane, by considering an anisotropic functional parameter, it is shown that the mass-energy density is also strictly positive.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/parameterizing-the-flattening-of-galaxies-rotation-curves-on-expanding-locally-anisotropic-backgrounds-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Infrared imaging and polarimetric observations of the pulsar wind nebula in SNR G21.5-0.9 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/infrared-imaging-and-polarimetric-observations-of-the-pulsar-wind-nebula-in-snr-g21-5-0-9-replacement/</link>
		<comments>http://voxcharta.org/2012/05/20/infrared-imaging-and-polarimetric-observations-of-the-pulsar-wind-nebula-in-snr-g21-5-0-9-replacement/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:35:26 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[canada france]]></category>
		<category><![CDATA[cfht aob]]></category>
		<category><![CDATA[compact nebula]]></category>
		<category><![CDATA[electric vector]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[hawaii telescope]]></category>
		<category><![CDATA[infrared imaging]]></category>
		<category><![CDATA[infrared observation]]></category>
		<category><![CDATA[infrared spectrum]]></category>
		<category><![CDATA[iron line]]></category>
		<category><![CDATA[k band]]></category>
		<category><![CDATA[polarimetric observations]]></category>
		<category><![CDATA[polarisation]]></category>
		<category><![CDATA[shape]]></category>
		<category><![CDATA[snr]]></category>
		<category><![CDATA[spitzer space telescope]]></category>
		<category><![CDATA[supernova remnant]]></category>
		<category><![CDATA[swing]]></category>
		<category><![CDATA[vlt]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/infrared-imaging-and-polarimetric-observations-of-the-pulsar-wind-nebula-in-snr-g21-5-0-9-replacement/</guid>
		<description><![CDATA[We present infrared observations of the supernova remnant G21.5-0.9 with the Very Large Telescope, the Canada-France-Hawaii Telescope and the Spitzer Space Telescope. Using the VLT/ISAAC camera equipped with a narrow-band [FeII] 1.64um filter the entire pulsar wind nebula in SNR G21.5-0.9 was imaged. This led to detection of iron line-emitting material in the shape of [...]]]></description>
			<content:encoded><![CDATA[<p>We present infrared observations of the supernova remnant G21.5-0.9 with the Very Large Telescope, the Canada-France-Hawaii Telescope and the Spitzer Space Telescope. Using the VLT/ISAAC camera equipped with a narrow-band [FeII] 1.64um filter the entire pulsar wind nebula in SNR G21.5-0.9 was imaged. This led to detection of iron line-emitting material in the shape of a broken ring-like structure following the nebula&#8217;s edge. The detected emission is limb-brightened. We also detect the compact nebula surrounding PSR J1833-1034, both through imaging with the CFHT/AOB-KIR instrument (K&#8217; band) and the IRAC camera (all bands) and also through polarimetric observations performed with VLT/ISAAC (Ks band). The emission from the compact nebula is highly polarised with an average value of the linear polarisation fraction $P_{L}^{avg} \simeq 0.47$, and the swing of the electric vector across the nebula can be observed. The infrared spectrum of the compact nebula can be described as a power law of index $\alpha_{IR} = 0.7 \pm 0.3$, and suggests that the spectrum flattens between the infrared and X-ray bands.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/infrared-imaging-and-polarimetric-observations-of-the-pulsar-wind-nebula-in-snr-g21-5-0-9-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A Near-Infrared Survey of the Inner Galactic Plane for Wolf-Rayet Stars II. Going Fainter: 71 More New WR Stars [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/a-near-infrared-survey-of-the-inner-galactic-plane-for-wolf-rayet-stars-ii-going-fainter-71-more-new-wr-stars-replacement/</link>
		<comments>http://voxcharta.org/2012/05/20/a-near-infrared-survey-of-the-inner-galactic-plane-for-wolf-rayet-stars-ii-going-fainter-71-more-new-wr-stars-replacement/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:35:16 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[band spectra]]></category>
		<category><![CDATA[distant spiral]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[few degrees]]></category>
		<category><![CDATA[follow ups]]></category>
		<category><![CDATA[galactic center]]></category>
		<category><![CDATA[galactic longitude]]></category>
		<category><![CDATA[galactic plane]]></category>
		<category><![CDATA[image analysis]]></category>
		<category><![CDATA[infrared survey]]></category>
		<category><![CDATA[k band]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[narrow band imaging]]></category>
		<category><![CDATA[spectroscopic parallax]]></category>
		<category><![CDATA[spiral arm]]></category>
		<category><![CDATA[square degree]]></category>
		<category><![CDATA[star candidates]]></category>
		<category><![CDATA[ups]]></category>
		<category><![CDATA[wr stars]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/a-near-infrared-survey-of-the-inner-galactic-plane-for-wolf-rayet-stars-ii-going-fainter-71-more-new-wr-stars-replacement/</guid>
		<description><![CDATA[We are continuing a J, K and narrow-band imaging survey of 300 square degrees of the plane of the Galaxy, searching for new Wolf-Rayet stars. Our survey spans 150 degrees in Galactic longitude and reaches 1 degree above and below the Galactic plane. The survey has a useful limiting magnitude of K = 15 over [...]]]></description>
			<content:encoded><![CDATA[<p>We are continuing a J, K and narrow-band imaging survey of 300 square degrees of the plane of the Galaxy, searching for new Wolf-Rayet stars. Our survey spans 150 degrees in Galactic longitude and reaches 1 degree above and below the Galactic plane. The survey has a useful limiting magnitude of K = 15 over most of the observed Galactic plane, and K = 14 (due to severe crowding) within a few degrees of the Galactic center. Thousands of emission line candidates have been detected. In spectrographic follow-ups of 146 relatively bright WR star candidates we have re-examined 11 previously known WC and WN stars and discovered 71 new WR stars, 17 of type WN and 54 of type WC. Our latest image analysis pipeline now picks out WR stars with a 57% success rate. Star subtype assignments have been confirmed with K band spectra, and distances approximated using the method of spectroscopic parallax. Some of the new WR stars are amongst the most distant known in our Galaxy. The distribution of these new WR stars is beginning to trace the locations of massive stars along the distant spiral arms of the Milky Way.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/a-near-infrared-survey-of-the-inner-galactic-plane-for-wolf-rayet-stars-ii-going-fainter-71-more-new-wr-stars-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Influence of internal structure on the motion of test bodies in extreme mass ratio situations [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/20/influence-of-internal-structure-on-the-motion-of-test-bodies-in-extreme-mass-ratio-situations-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/20/influence-of-internal-structure-on-the-motion-of-test-bodies-in-extreme-mass-ratio-situations-cross-listing/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:31:05 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[approximation method]]></category>
		<category><![CDATA[binding energy]]></category>
		<category><![CDATA[equatorial plane]]></category>
		<category><![CDATA[general relativity]]></category>
		<category><![CDATA[geometry]]></category>
		<category><![CDATA[gravitational wave physics]]></category>
		<category><![CDATA[internal structure]]></category>
		<category><![CDATA[kerr]]></category>
		<category><![CDATA[mass ratio]]></category>
		<category><![CDATA[tidal interaction]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/influence-of-internal-structure-on-the-motion-of-test-bodies-in-extreme-mass-ratio-situations-cross-listing/</guid>
		<description><![CDATA[We investigate the motion of test bodies with internal structure in General Relativity. With the help of a multipolar approximation method for extended test bodies we derive the equations of motion up to the quadrupolar order. The motion of pole-dipole and quadrupole test bodies is studied in the context of the Kerr geometry. For an [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate the motion of test bodies with internal structure in General Relativity. With the help of a multipolar approximation method for extended test bodies we derive the equations of motion up to the quadrupolar order. The motion of pole-dipole and quadrupole test bodies is studied in the context of the Kerr geometry. For an explicit quadrupole model, which includes spin and tidal interactions, the motion in the equatorial plane is characterized by an effective potential and by the binding energy. We compare our findings to recent results for the conservative part of the self-force of bodies in extreme mass ratio situations. Possible implications for gravitational wave physics are outlined.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/influence-of-internal-structure-on-the-motion-of-test-bodies-in-extreme-mass-ratio-situations-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>HerMES: Candidate Gravitationally Lensed Galaxies and Lensing Statistics at Submillimeter Wavelengths</title>
		<link>http://voxcharta.org/2012/05/17/hermes-candidate-gravitationally-lensed-galaxies-and-lensing-statistics-at-submillimeter-wavelengths/</link>
		<comments>http://voxcharta.org/2012/05/17/hermes-candidate-gravitationally-lensed-galaxies-and-lensing-statistics-at-submillimeter-wavelengths/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:57:19 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[dusty star]]></category>
		<category><![CDATA[foreground]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gravitational lensing]]></category>
		<category><![CDATA[hermes]]></category>
		<category><![CDATA[herschel]]></category>
		<category><![CDATA[interloper]]></category>
		<category><![CDATA[magnification]]></category>
		<category><![CDATA[matter distribution]]></category>
		<category><![CDATA[observational data]]></category>
		<category><![CDATA[s 500]]></category>
		<category><![CDATA[square degree]]></category>
		<category><![CDATA[statistic]]></category>
		<category><![CDATA[statistical model]]></category>
		<category><![CDATA[submillimeter wavelength]]></category>
		<category><![CDATA[surface density]]></category>
		<category><![CDATA[target]]></category>
		<category><![CDATA[unprecedented spatial resolution]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/hermes-candidate-gravitationally-lensed-galaxies-and-lensing-statistics-at-submillimeter-wavelengths/</guid>
		<description><![CDATA[We present a list of 13 candidate gravitationally lensed submillimeter galaxies (SMGs) from 95 square degrees of the Herschel Multi-tiered Extragalactic Survey, a surface density of 0.14\pm0.04deg^{-2}. These sources have 500um flux densities (S_500) greater than 100mJy. Follow-up observations confirm gravitational lensing in 9 of the 13 systems (70%); the lensing status of the four [...]]]></description>
			<content:encoded><![CDATA[<p>We present a list of 13 candidate gravitationally lensed submillimeter galaxies (SMGs) from 95 square degrees of the Herschel Multi-tiered Extragalactic Survey, a surface density of 0.14\pm0.04deg^{-2}. These sources have 500um flux densities (S_500) greater than 100mJy. Follow-up observations confirm gravitational lensing in 9 of the 13 systems (70%); the lensing status of the four remaining sources is undetermined. We also present a supplementary sample of 29 (0.31\pm0.06deg^{-2}) gravitationally lensed SMG candidates with S_500=80&#8211;100mJy, which are expected to contain a higher fraction of interlopers than the primary candidates. The number counts of the candidate lensed galaxies are consistent with a simple statistical model of the lensing rate, which uses a foreground matter distribution, the intrinsic SMG number counts, and an assumed SMG redshift distribution. The model predicts that 43&#8211;83% of our S_500&gt;100mJy candidates are strongly gravitationally lensed, with the brightest sources being the most robust; this is consistent with the observational data. Our statistical model also predicts that, on average, lensed galaxies with S_500=100mJy are magnified by factors of ~6, with brighter galaxies having progressively higher average magnification. 50% of the sources are expected to have intrinsic 500um flux densities less than 30mJy. Thus, samples of strongly gravitationally lensed SMGs, such as those presented here, probe below the nominal Herschel detection limit at 500um. They are ideal targets for the detailed study of the physical conditions in distant dusty, star-forming galaxies, with unprecedented spatial resolution achieved due to the lensing magnification.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/hermes-candidate-gravitationally-lensed-galaxies-and-lensing-statistics-at-submillimeter-wavelengths/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Optically Unbiased GRB Host (TOUGH) survey. IV. Lyman-alpha emitters</title>
		<link>http://voxcharta.org/2012/05/17/the-optically-unbiased-grb-host-tough-survey-iv-lyman-alpha-emitters/</link>
		<comments>http://voxcharta.org/2012/05/17/the-optically-unbiased-grb-host-tough-survey-iv-lyman-alpha-emitters/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:56:59 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[40a]]></category>
		<category><![CDATA[alpha emission]]></category>
		<category><![CDATA[equivalent width]]></category>
		<category><![CDATA[extinction]]></category>
		<category><![CDATA[formation rates]]></category>
		<category><![CDATA[gamma ray burst]]></category>
		<category><![CDATA[grbs]]></category>
		<category><![CDATA[host galaxy]]></category>
		<category><![CDATA[hosts]]></category>
		<category><![CDATA[lyman alpha]]></category>
		<category><![CDATA[redshift range]]></category>
		<category><![CDATA[rest frame]]></category>
		<category><![CDATA[spectroscopic search]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/the-optically-unbiased-grb-host-tough-survey-iv-lyman-alpha-emitters/</guid>
		<description><![CDATA[We report the results of a spectroscopic search for Lyman-alpha emission from gamma-ray burst host galaxies. Based on the well-defined TOUGH sample of 69 X-ray selected Swift GRBs, we have targeted the hosts of a subsample of 20 GRBs known from afterglow spectroscopy to be in the redshift range 1.8-4.5. We detect Lya emission from [...]]]></description>
			<content:encoded><![CDATA[<p>We report the results of a spectroscopic search for Lyman-alpha emission from gamma-ray burst host galaxies. Based on the well-defined TOUGH sample of 69 X-ray selected Swift GRBs, we have targeted the hosts of a subsample of 20 GRBs known from afterglow spectroscopy to be in the redshift range 1.8-4.5. We detect Lya emission from 7 out of the 20 hosts, with the typical limiting 3sigma line flux being 8E-18 erg/cm2/s, corresponding to a Lya luminosity of 6E41 erg/s at z=3. The Lya luminosities for the 7 hosts in which we detect Lya emission are in the range (0.6-2.3)E42 erg/s corresponding to star-formation rates of 0.6-2.1 Msun/yr (not corrected for extinction). The rest-frame Lya equivalent widths (EWs) for the 7 hosts are in the range 9-40A. For 6 of the 13 hosts for which Lya is not detected we place fairly strong 3sigma upper limits on the EW (&lt;20A), while for others the EW is either unconstrained or has a less constraining upper limit. We find that the distribution of Lya EWs is inconsistent with being drawn from the Lya EW distribution of bright Lyman break galaxies at the 98.3% level, in the sense that the TOUGH hosts on average have larger EWs than bright LBGs. We can exclude an early indication, based on a smaller, heterogeneous sample of pre-Swift GRB hosts, that all GRB hosts are Lya emitters. We find that the TOUGH hosts on average have lower EWs than the pre-Swift GRB hosts, but the two samples are only inconsistent at the 92% level. The velocity centroid of the Lya line is redshifted by 200-700 km/s with respect to the systemic velocity, similar to what is seen for LBGs, possibly indicating star-formation driven outflows from the host galaxies. There seems to be a trend between the Lya EW and the optical to X-ray spectral index of the afterglow (beta_OX), hinting that dust plays a role in the observed strength and even presence of Lya emission. [ABRIDGED]</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/the-optically-unbiased-grb-host-tough-survey-iv-lyman-alpha-emitters/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Lick AGN Monitoring Project 2011: Dynamical Modeling of the Broad Line Region in Mrk 50</title>
		<link>http://voxcharta.org/2012/05/17/the-lick-agn-monitoring-project-2011-dynamical-modeling-of-the-broad-line-region-in-mrk-50/</link>
		<comments>http://voxcharta.org/2012/05/17/the-lick-agn-monitoring-project-2011-dynamical-modeling-of-the-broad-line-region-in-mrk-50/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:54:32 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[AGN]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[blr]]></category>
		<category><![CDATA[dynamical model]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[geometry]]></category>
		<category><![CDATA[hole mass]]></category>
		<category><![CDATA[inclination angle]]></category>
		<category><![CDATA[inflow]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[mapping analysis]]></category>
		<category><![CDATA[mapping data]]></category>
		<category><![CDATA[monitoring project]]></category>
		<category><![CDATA[mrk]]></category>
		<category><![CDATA[outflow]]></category>
		<category><![CDATA[pm10]]></category>
		<category><![CDATA[reverberation]]></category>
		<category><![CDATA[scenarios]]></category>
		<category><![CDATA[sigma]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/the-lick-agn-monitoring-project-2011-dynamical-modeling-of-the-broad-line-region-in-mrk-50/</guid>
		<description><![CDATA[We present dynamical modeling of the broad line region (BLR) in the Seyfert 1 galaxy Mrk 50 using reverberation mapping data taken as part of the Lick AGN Monitoring Project (LAMP) 2011. We model the reverberation mapping data directly, constraining the geometry and kinematics of the BLR, as well as deriving a black hole mass [...]]]></description>
			<content:encoded><![CDATA[<p>We present dynamical modeling of the broad line region (BLR) in the Seyfert 1 galaxy Mrk 50 using reverberation mapping data taken as part of the Lick AGN Monitoring Project (LAMP) 2011. We model the reverberation mapping data directly, constraining the geometry and kinematics of the BLR, as well as deriving a black hole mass estimate that does not depend on a normalizing factor or virial coefficient. We find that the geometry of the BLR in Mrk 50 is a nearly face-on thick disk, with a mean radius of 9.6(+1.2,-0.9) light days, a width of the BLR of 6.9(+1.2,-1.1) light days, and a disk opening angle of 25\pm10 degrees above the plane. We also constrain the inclination angle to be 9(+7,-5) degrees, close to face-on. Finally, the black hole mass of Mrk 50 is inferred to be log10(M(BH)/Msun) = 7.57(+0.44,-0.27). By comparison to the virial black hole mass estimate from traditional reverberation mapping analysis, we find the normalizing constant (virial coefficient) to be log10(f) = 0.78(+0.44,-0.27), consistent with the commonly adopted mean value of 0.74 based on aligning the M(BH)-{\sigma}* relation for AGN and quiescent galaxies. While our dynamical model includes the possibility of a net inflow or outflow in the BLR, we cannot distinguish between these two scenarios.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/the-lick-agn-monitoring-project-2011-dynamical-modeling-of-the-broad-line-region-in-mrk-50/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Column Density Variance-Sonic Mach Number Relationship</title>
		<link>http://voxcharta.org/2012/05/17/the-column-density-variance-sonic-mach-number-relationship/</link>
		<comments>http://voxcharta.org/2012/05/17/the-column-density-variance-sonic-mach-number-relationship/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:53:55 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[2ms]]></category>
		<category><![CDATA[best fit]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[density values]]></category>
		<category><![CDATA[diffuse interstellar medium]]></category>
		<category><![CDATA[investigations]]></category>
		<category><![CDATA[mach number]]></category>
		<category><![CDATA[mhd simulation]]></category>
		<category><![CDATA[molecular cloud]]></category>
		<category><![CDATA[observational data]]></category>
		<category><![CDATA[observational study]]></category>
		<category><![CDATA[relationship]]></category>
		<category><![CDATA[rho rho]]></category>
		<category><![CDATA[sigma 2]]></category>
		<category><![CDATA[sigma rho]]></category>
		<category><![CDATA[sigma sigma sigma]]></category>
		<category><![CDATA[taurus]]></category>
		<category><![CDATA[tracers]]></category>
		<category><![CDATA[variance]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/the-column-density-variance-sonic-mach-number-relationship/</guid>
		<description><![CDATA[Although there are a wealth of column density tracers for both the molecular and diffuse interstellar medium, there are very few observational studies investigating the relationship between the density variance (\sigma^2) and the sonic Mach number (Ms). This is in part due to the fact that the \sigma^2-Ms relationship is derived, via MHD simulations, for [...]]]></description>
			<content:encoded><![CDATA[<p>Although there are a wealth of column density tracers for both the molecular and diffuse interstellar medium, there are very few observational studies investigating the relationship between the density variance (\sigma^2) and the sonic Mach number (Ms). This is in part due to the fact that the \sigma^2-Ms relationship is derived, via MHD simulations, for the 3D density variance only, which is not a direct observable. We investigate the utility of a 2D column density \sigma_{\Sigma/\Sigma_0}^2-Ms relationship using solenoidally driven isothermal MHD simulations and find that the best fit follows closely the form of the 3D density \sigma_{\rho/\rho_0}^2-Ms trend but includes a scaling parameter A such that: \sigma_{ln(\Sigma/\Sigma_0)}^2=Axln(1+b^2Ms^2), where A=0.11 and b=1/3. This relation is consistent with the observational data reported for the Taurus and IC 5146 molecular clouds with b=0.5 and A=0.12. These results open up the possibility of using the 2D column density values of \sigma^2 for investigations of the relation between the the sonic Mach number and the PDF variance in addition to existing PDF sonic Mach number relations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/the-column-density-variance-sonic-mach-number-relationship/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
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		<title>HI Power Spectra and the Turbulent ISM of Dwarf Irregular Galaxies</title>
		<link>http://voxcharta.org/2012/05/17/hi-power-spectra-and-the-turbulent-ism-of-dwarf-irregular-galaxies/</link>
		<comments>http://voxcharta.org/2012/05/17/hi-power-spectra-and-the-turbulent-ism-of-dwarf-irregular-galaxies/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:53:31 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[channel maps]]></category>
		<category><![CDATA[fundamental role]]></category>
		<category><![CDATA[galaxy survey]]></category>
		<category><![CDATA[hi line]]></category>
		<category><![CDATA[hi power]]></category>
		<category><![CDATA[irregular galaxy]]></category>
		<category><![CDATA[irregulars]]></category>
		<category><![CDATA[length scales]]></category>
		<category><![CDATA[line profile]]></category>
		<category><![CDATA[nearby galaxy]]></category>
		<category><![CDATA[nonlinear development]]></category>
		<category><![CDATA[power source]]></category>
		<category><![CDATA[power spectra]]></category>
		<category><![CDATA[sfr]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[surface density]]></category>
		<category><![CDATA[thermal dispersion]]></category>
		<category><![CDATA[turbulent structure]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/hi-power-spectra-and-the-turbulent-ism-of-dwarf-irregular-galaxies/</guid>
		<description><![CDATA[HI spatial power spectra (PS) were determined for a sample of 24 nearby dwarf irregular galaxies selected from the LITTLE THINGS (Local Irregulars That Trace Luminosity Extremes &#8211; The HI Nearby Galaxy Survey) sample. The two-dimensional (2D) power spectral indices asymptotically become a constant for each galaxy when a significant part of the line profile [...]]]></description>
			<content:encoded><![CDATA[<p>HI spatial power spectra (PS) were determined for a sample of 24 nearby dwarf irregular galaxies selected from the LITTLE THINGS (Local Irregulars That Trace Luminosity Extremes &#8211; The HI Nearby Galaxy Survey) sample. The two-dimensional (2D) power spectral indices asymptotically become a constant for each galaxy when a significant part of the line profile is integrated. For narrow channel maps, the PS become shallower as the channel width decreases, and this shallowing trend continues to our single channel maps. This implies that even the highest velocity resolution of 1.8 km/s is not smaller than the thermal dispersion of the coolest, widespread HI component. The one-dimensional PS of azimuthal profiles at different radii suggest that the shallower PS for narrower channel width is mainly contributed by the inner disks, which indicates that the inner disks have proportionally more cooler HI than the outer disks. Galaxies with lower luminosity (M_B &gt; -14.5 mag) and star formation rate (SFR, log(SFR (M\odot/yr)) &lt; -2.1) tend to have steeper PS, which implies that the HI line-of-sight depths can be comparable with the radial length scales in low mass galaxies. A lack of a correlation between the inertial-range spectral indices and SFR surface density implies that either non-stellar power sources are playing a fundamental role in driving the interstellar medium (ISM) turbulent structure, or the nonlinear development of turbulent structures has little to do with the driving sources.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/hi-power-spectra-and-the-turbulent-ism-of-dwarf-irregular-galaxies/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Acceleration of Energetic Particles through Reconnection of Weakly Stochastic Magnetic Field</title>
		<link>http://voxcharta.org/2012/05/17/acceleration-of-energetic-particles-through-reconnection-of-weakly-stochastic-magnetic-field/</link>
		<comments>http://voxcharta.org/2012/05/17/acceleration-of-energetic-particles-through-reconnection-of-weakly-stochastic-magnetic-field/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:53:16 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[driven turbulence]]></category>
		<category><![CDATA[energetic particle]]></category>
		<category><![CDATA[intensity]]></category>
		<category><![CDATA[large scale]]></category>
		<category><![CDATA[latter case]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetic reconnection]]></category>
		<category><![CDATA[motion]]></category>
		<category><![CDATA[new evidence]]></category>
		<category><![CDATA[particle acceleration]]></category>
		<category><![CDATA[pino]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[successful testing]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/acceleration-of-energetic-particles-through-reconnection-of-weakly-stochastic-magnetic-field/</guid>
		<description><![CDATA[Astrophysical media are turbulent and therefore reconnection should be treated in the presence of pre-existing turbulence. We consider the model of fast magnetic reconnection in Lazarian &#38; Vishniac (1999) which predicts that the rate of reconnection is controlled by the intensity and the injection scale of turbulent motions. We provide new evidence of successful testing [...]]]></description>
			<content:encoded><![CDATA[<p>Astrophysical media are turbulent and therefore reconnection should be treated in the presence of pre-existing turbulence. We consider the model of fast magnetic reconnection in Lazarian &amp; Vishniac (1999) which predicts that the rate of reconnection is controlled by the intensity and the injection scale of turbulent motions. We provide new evidence of successful testing of the model and argue that the model presents a generic set up for astrophysical reconnection events. We study particle acceleration that takes place in volumes of driven turbulence as well turbulent volumes in the presence of large scale reconnection. We show that in the latter case the acceleration is of the first order Fermi type thus supporting the model of acceleration proposed in Gouveia dal Pino &amp; Lazarian (2005).</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/acceleration-of-energetic-particles-through-reconnection-of-weakly-stochastic-magnetic-field/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A Brightest Cluster Galaxy with an Extremely Large Flat Core</title>
		<link>http://voxcharta.org/2012/05/17/a-brightest-cluster-galaxy-with-an-extremely-large-flat-core/</link>
		<comments>http://voxcharta.org/2012/05/17/a-brightest-cluster-galaxy-with-an-extremely-large-flat-core/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:48:33 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bcg]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[cluster galaxy]]></category>
		<category><![CDATA[core structure]]></category>
		<category><![CDATA[cusp]]></category>
		<category><![CDATA[density profile]]></category>
		<category><![CDATA[extrapolation]]></category>
		<category><![CDATA[galaxy cluster abell]]></category>
		<category><![CDATA[hole mass]]></category>
		<category><![CDATA[hubble show]]></category>
		<category><![CDATA[hubble space telescope]]></category>
		<category><![CDATA[hubble space telescope images]]></category>
		<category><![CDATA[interior surface]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[perturbation]]></category>
		<category><![CDATA[space telescope images]]></category>
		<category><![CDATA[stellar density]]></category>
		<category><![CDATA[surface brightness]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/a-brightest-cluster-galaxy-with-an-extremely-large-flat-core/</guid>
		<description><![CDATA[Hubble Space Telescope images of the galaxy cluster Abell 2261, obtained as part of the Cluster Lensing And Supernova survey with Hubble, show that the brightest galaxy in the cluster, A2261-BCG, has the largest core yet detected in any galaxy. The cusp radius of A2261-BCG is 3.2 kpc, twice as big as the next largest [...]]]></description>
			<content:encoded><![CDATA[<p>Hubble Space Telescope images of the galaxy cluster Abell 2261, obtained as part of the Cluster Lensing And Supernova survey with Hubble, show that the brightest galaxy in the cluster, A2261-BCG, has the largest core yet detected in any galaxy. The cusp radius of A2261-BCG is 3.2 kpc, twice as big as the next largest core known, and ~3x bigger than those typically seen in the most luminous BCGs. The morphology of the core in A2261-BCG is also unusual, having a flat or even slightly-depressed interior surface brightness profile, rather than the typical shallow cusp. This implies that the galaxy has a core with constant or even centrally decreasing stellar density. Interpretation of the core as an end product of the &#8220;scouring&#8221; action of a binary supermassive black hole implies a total black hole mass ~1E+10 M_sun from the extrapolation of most relationships between core structure and black hole mass. The core falls 1-sigma above the cusp-radius versus galaxy luminosity relation. Its large size in real terms, and the extremely large black hole mass required to generate it, raise the possibility that the core has been enlarged by additional processes, such as the ejection of the black holes that originally generated the core. The flat central stellar density profile is consistent with this hypothesis. The core is also displaced by 0.7 kpc from the center of the surrounding envelope, consistent with a local dynamical perturbation of the core.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/a-brightest-cluster-galaxy-with-an-extremely-large-flat-core/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A Keplerian Circumbinary Disk around the Protobinary System L1551 NE</title>
		<link>http://voxcharta.org/2012/05/17/a-keplerian-circumbinary-disk-around-the-protobinary-system-l1551-ne/</link>
		<comments>http://voxcharta.org/2012/05/17/a-keplerian-circumbinary-disk-around-the-protobinary-system-l1551-ne/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:47:47 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[angular momentum]]></category>
		<category><![CDATA[array]]></category>
		<category><![CDATA[central peak]]></category>
		<category><![CDATA[channel maps]]></category>
		<category><![CDATA[companion]]></category>
		<category><![CDATA[continuum emission]]></category>
		<category><![CDATA[images]]></category>
		<category><![CDATA[inner edge]]></category>
		<category><![CDATA[keplerian disks]]></category>
		<category><![CDATA[line emission]]></category>
		<category><![CDATA[msun]]></category>
		<category><![CDATA[protostar]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[thin disk]]></category>
		<category><![CDATA[tidal effect]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/a-keplerian-circumbinary-disk-around-the-protobinary-system-l1551-ne/</guid>
		<description><![CDATA[We present SubMillimeter-Array observations of a Keplerian disk around the Class I protobinary system L1551 NE in 335 GHz continuum emission and submillimeter line emission in 13CO (J=3-2) and C18O (J=3-2) at a resolution of ~120 x 80 AU. The 335-GHz dust-continuum image shows a strong central peak closely coincident with the binary protostars and [...]]]></description>
			<content:encoded><![CDATA[<p>We present SubMillimeter-Array observations of a Keplerian disk around the Class I protobinary system L1551 NE in 335 GHz continuum emission and submillimeter line emission in 13CO (J=3-2) and C18O (J=3-2) at a resolution of ~120 x 80 AU. The 335-GHz dust-continuum image shows a strong central peak closely coincident with the binary protostars and likely corresponding to circumstellar disks, surrounded by a ~600 x 300 AU feature elongated approximately perpendicular to the [Fe II] jet from the southern protostellar component suggestive of a circumbinary disk. The 13CO and C18O images confirm that the circumbinary continuum feature is indeed a rotating disk; furthermore, the C18O channel maps can be well modeled by a geometrically-thin disk exhibiting Keplerian rotation. We estimate a mass for the circumbinary disk of ~0.03-0.12 Msun, compared with an enclosed mass of ~0.8 Msun that is dominated by the protobinary system. Compared with several other Class I protostars known to exhibit Keplerian disks, L1551 NE has the lowest bolometric temperature (~91 K), highest envelope mass (~0.39 Msun), and the lowest ratio in stellar mass to envelope + disk + stellar mass (~0.65). L1551 NE may therefore be the youngest protostellar object so far found to exhibit a Keplerian disk. Our observations present firm evidence that Keplerian disks around binary protostellar systems, &#8220;Keplerian circumbinary disks&#8217;, can exist. We speculate that tidal effects from binary companions could transport angular momenta toward the inner edge of the circumbinary disk and create the Keplerian circumbinary disk.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/a-keplerian-circumbinary-disk-around-the-protobinary-system-l1551-ne/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Gravitational lensing in the Kerr-Randers optical geometry [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/17/gravitational-lensing-in-the-kerr-randers-optical-geometry-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/17/gravitational-lensing-in-the-kerr-randers-optical-geometry-cross-listing/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:47:25 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bonnet]]></category>
		<category><![CDATA[deflection angle]]></category>
		<category><![CDATA[equatorial plane]]></category>
		<category><![CDATA[finsler]]></category>
		<category><![CDATA[gauss]]></category>
		<category><![CDATA[geometric method]]></category>
		<category><![CDATA[gravitational lensing]]></category>
		<category><![CDATA[kerr]]></category>
		<category><![CDATA[naz]]></category>
		<category><![CDATA[optical geometry]]></category>
		<category><![CDATA[osculating]]></category>
		<category><![CDATA[randers]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/gravitational-lensing-in-the-kerr-randers-optical-geometry-cross-listing/</guid>
		<description><![CDATA[A new geometric method to determine the deflection of light in the equatorial plane of the Kerr solution is presented, whose optical geometry is a surface with a Finsler metric of Randers type. Applying the Gauss-Bonnet theorem to a suitable osculating Riemannian manifold, adapted from a construction by Naz\i m, it is shown explicitly how [...]]]></description>
			<content:encoded><![CDATA[<p>A new geometric method to determine the deflection of light in the equatorial plane of the Kerr solution is presented, whose optical geometry is a surface with a Finsler metric of Randers type. Applying the Gauss-Bonnet theorem to a suitable osculating Riemannian manifold, adapted from a construction by Naz\i m, it is shown explicitly how the two leading terms of the asymptotic deflection angle of gravitational lensing can be found in this way.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/gravitational-lensing-in-the-kerr-randers-optical-geometry-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Viscous-Resistive ADAF with a general Large-Scale Magnetic Field</title>
		<link>http://voxcharta.org/2012/05/17/viscous-resistive-adaf-with-a-general-large-scale-magnetic-field/</link>
		<comments>http://voxcharta.org/2012/05/17/viscous-resistive-adaf-with-a-general-large-scale-magnetic-field/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:47:02 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[adaf]]></category>
		<category><![CDATA[diffusivity]]></category>
		<category><![CDATA[dominant mechanism]]></category>
		<category><![CDATA[energy dissipation]]></category>
		<category><![CDATA[existence]]></category>
		<category><![CDATA[field parameter]]></category>
		<category><![CDATA[global magnetic field]]></category>
		<category><![CDATA[keplerian]]></category>
		<category><![CDATA[kinematic viscosity]]></category>
		<category><![CDATA[numerical result]]></category>
		<category><![CDATA[radial velocity]]></category>
		<category><![CDATA[realistic model]]></category>
		<category><![CDATA[resistivity]]></category>
		<category><![CDATA[rotational velocity]]></category>
		<category><![CDATA[sound speed]]></category>
		<category><![CDATA[Turbulence]]></category>
		<category><![CDATA[velocities]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/viscous-resistive-adaf-with-a-general-large-scale-magnetic-field/</guid>
		<description><![CDATA[We have studied the structure of hot accretion flow bathed in a general large-scale magnetic field. We have considered magnetic parameters $ \beta_{r,\varphi,z}[=c^2_{r,\varphi,z}/(2c^2_{s})] $, where $ c^2_{r, \varphi, z} $ are the Alfv\&#8217;{e}n sound speeds in three direction of cylindrical coordinate $ (r,\varphi,z) $. The dominant mechanism of energy dissipation is assumed to be the [...]]]></description>
			<content:encoded><![CDATA[<p>We have studied the structure of hot accretion flow bathed in a general large-scale magnetic field. We have considered magnetic parameters $ \beta_{r,\varphi,z}[=c^2_{r,\varphi,z}/(2c^2_{s})] $, where $ c^2_{r, \varphi, z} $ are the Alfv\&#8217;{e}n sound speeds in three direction of cylindrical coordinate $ (r,\varphi,z) $. The dominant mechanism of energy dissipation is assumed to be the magnetic diffusivity due to turbulence and viscosity in the accretion flow. Also, we adopt a more realistic model for kinematic viscosity $ (\nu=\alpha c_{s} H) $, with both $ c_{s} $ and $ H $ as a function of magnetic field. As a result in our model, the kinematic viscosity and magnetic diffusivity $ (\eta=\eta_{0}c_{s} H) $ are not constant. In order to solve the integrated equations that govern the behavior of the accretion flow, a self-similar method is used. It is found that the existence of magnetic resistivity will increase the radial infall velocity as well as sound speed and vertical thickness of the disk. However the rotational velocity of the disk decreases by the increase of magnetic resistivity. Moreover, we study the effect of three components of global magnetic field on the structure of the disk. We found out that the radial velocity and sound speed are Sub-Keplerian for all values of magnetic field parameters, but the rotational velocity can be Super-Keplerian by the increase of toroidal magnetic field. Also, Our numerical results show that all components of magnetic field can be important and have a considerable effect on velocities and vertical thickness of the disk.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/viscous-resistive-adaf-with-a-general-large-scale-magnetic-field/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Interstellar reddening towards six small areas in Puppis-Vela</title>
		<link>http://voxcharta.org/2012/05/17/interstellar-reddening-towards-six-small-areas-in-puppis-vela/</link>
		<comments>http://voxcharta.org/2012/05/17/interstellar-reddening-towards-six-small-areas-in-puppis-vela/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:46:13 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accuracy]]></category>
		<category><![CDATA[beta]]></category>
		<category><![CDATA[cavity]]></category>
		<category><![CDATA[distance]]></category>
		<category><![CDATA[excesses]]></category>
		<category><![CDATA[gum nebula]]></category>
		<category><![CDATA[high quality]]></category>
		<category><![CDATA[hipparcos catalogue]]></category>
		<category><![CDATA[interstellar dust]]></category>
		<category><![CDATA[interstellar medium]]></category>
		<category><![CDATA[interstellar reddening]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[low density]]></category>
		<category><![CDATA[photometric measurements]]></category>
		<category><![CDATA[sky]]></category>
		<category><![CDATA[spite]]></category>
		<category><![CDATA[standard deviation]]></category>
		<category><![CDATA[Sun]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/interstellar-reddening-towards-six-small-areas-in-puppis-vela/</guid>
		<description><![CDATA[We investigate the distribution of the interstellar dust towards six small volumes of the sky in the region of the Gum nebula. New high-quality four-colour uvby and H\beta\ Str\&#8221;omgren photometry obtained for 352 stars in six selected areas of Kapteyn, complemented with data obtained in a previous investigation for two of these areas, were used [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate the distribution of the interstellar dust towards six small volumes of the sky in the region of the Gum nebula. New high-quality four-colour uvby and H\beta\ Str\&#8221;omgren photometry obtained for 352 stars in six selected areas of Kapteyn, complemented with data obtained in a previous investigation for two of these areas, were used to estimate the colour excess and distance to these objects. The obtained colour excess versus distance diagrams, complemented with other information, when available, were analysed in order to infer the properties of the interstellar medium permeating the observed volumes. On the basis of the overall standard deviation in the photometric measurements, we estimate that colour excesses and distances are determined with an accuracy of 0.010 mag and better than 30%, respectively, for a sample of 520 stars. A comparison with 37 stars in common with the new Hipparcos catalogue attests to the high quality of the photometric distance determination. The obtained colour excess versus distance diagrams testify to the low density volume towards the observed lines-of-sight. Very few stars out to distances of 1 kpc from the Sun have colour excesses larger than E(b-y) = 0.1 mag. In spite of the low density character of the interstellar medium towards the Puppis-Vela direction, the obtained reddening as a function of the distance indicates that two or more interstellar structures are crossed towards the observed lines-of-sight. One of these structures may be associated with the very low density wall of the Local Cavity, which has a distance of 100-150 pc from the Sun. Another structure might be related to the Gum nebula, and if so, its front face would be located at about 350 pc from the Sun.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/interstellar-reddening-towards-six-small-areas-in-puppis-vela/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Oxygen and nitrogen abundances of HII regions in six spiral galaxies</title>
		<link>http://voxcharta.org/2012/05/17/oxygen-and-nitrogen-abundances-of-hii-regions-in-six-spiral-galaxies/</link>
		<comments>http://voxcharta.org/2012/05/17/oxygen-and-nitrogen-abundances-of-hii-regions-in-six-spiral-galaxies/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:45:43 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bta]]></category>
		<category><![CDATA[calibration]]></category>
		<category><![CDATA[dispersion]]></category>
		<category><![CDATA[electron temperature]]></category>
		<category><![CDATA[gradient]]></category>
		<category><![CDATA[hii region]]></category>
		<category><![CDATA[intercept]]></category>
		<category><![CDATA[irregular galaxy]]></category>
		<category><![CDATA[meter telescope]]></category>
		<category><![CDATA[NGC]]></category>
		<category><![CDATA[nitrogen]]></category>
		<category><![CDATA[oxygen]]></category>
		<category><![CDATA[radial distribution]]></category>
		<category><![CDATA[scorpio]]></category>
		<category><![CDATA[special astrophysical observatory]]></category>
		<category><![CDATA[spectral camera]]></category>
		<category><![CDATA[spectral resolution]]></category>
		<category><![CDATA[spectroscopic observation]]></category>
		<category><![CDATA[spiral galaxy]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/oxygen-and-nitrogen-abundances-of-hii-regions-in-six-spiral-galaxies/</guid>
		<description><![CDATA[Spectroscopic observations of 63 HII regions in six spiral galaxies (NGC 628, NGC 783, NGC 2336, NGC 6217, NGC 7331, and NGC 7678) were carried out with the 6-meter telescope (BTA) of Russian Special Astrophysical Observatory with the Spectral Camera attached to the focal reducer SCORPIO in the multislit mode with a dispersion of 2.1A/pixel [...]]]></description>
			<content:encoded><![CDATA[<p>Spectroscopic observations of 63 HII regions in six spiral galaxies (NGC 628, NGC 783, NGC 2336, NGC 6217, NGC 7331, and NGC 7678) were carried out with the 6-meter telescope (BTA) of Russian Special Astrophysical Observatory with the Spectral Camera attached to the focal reducer SCORPIO in the multislit mode with a dispersion of 2.1A/pixel and a spectral resolution of 10A. These observations were used to estimate the oxygen and nitrogen abundances and the electron temperatures in HII regions through the recent variant of the strong line method (NS calibration). The parameters of the radial distribution (the extrapolated central intercept value and the gradient) of the oxygen and nitrogen abundances in the disks of spiral galaxies NGC 628, NGC 783, NGC 2336, NGC 7331, and NGC 7678 have been determined. The abundances in the NGC 783, NGC 2336, NGC 6217, and NGC 7678 are measured for the first time. Galaxies from our sample follow well the general trend in the luminosity &#8211; central metallicity diagram for spiral and irregular galaxies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/oxygen-and-nitrogen-abundances-of-hii-regions-in-six-spiral-galaxies/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Interstellar Dust Close to the Sun</title>
		<link>http://voxcharta.org/2012/05/17/interstellar-dust-close-to-the-sun/</link>
		<comments>http://voxcharta.org/2012/05/17/interstellar-dust-close-to-the-sun/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:38:16 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[amorphous carbon]]></category>
		<category><![CDATA[dimensional model]]></category>
		<category><![CDATA[gas composition]]></category>
		<category><![CDATA[grain characteristics]]></category>
		<category><![CDATA[heliosphere]]></category>
		<category><![CDATA[interstellar dust grain]]></category>
		<category><![CDATA[interstellar gas]]></category>
		<category><![CDATA[iron oxide]]></category>
		<category><![CDATA[ism]]></category>
		<category><![CDATA[low density]]></category>
		<category><![CDATA[nearby reservoir]]></category>
		<category><![CDATA[nearby star]]></category>
		<category><![CDATA[olivine]]></category>
		<category><![CDATA[plume]]></category>
		<category><![CDATA[refractories]]></category>
		<category><![CDATA[relative abundance]]></category>
		<category><![CDATA[shock]]></category>
		<category><![CDATA[solar wind]]></category>
		<category><![CDATA[spacecraft]]></category>
		<category><![CDATA[variation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/interstellar-dust-close-to-the-sun/</guid>
		<description><![CDATA[The low density interstellar medium (ISM) close to the Sun and inside of the heliosphere provides a unique laboratory for studying interstellar dust grains. Grain characteristics in the nearby ISM are obtained from observations of interstellar gas and dust inside of the heliosphere and the interstellar gas towards nearby stars. Comparison between the gas composition [...]]]></description>
			<content:encoded><![CDATA[<p>The low density interstellar medium (ISM) close to the Sun and inside of the heliosphere provides a unique laboratory for studying interstellar dust grains. Grain characteristics in the nearby ISM are obtained from observations of interstellar gas and dust inside of the heliosphere and the interstellar gas towards nearby stars. Comparison between the gas composition and solar abundances suggests that grains are dominated by olivines and possibly some form of iron oxide. Measurements of the interstellar Ne/O ratio by the Interstellar Boundary Explorer spacecraft indicate that a high fraction of interstellar oxygen in the ISM must be depleted onto dust grains. Local interstellar abundances are consistent with grain destruction in ~150 km/s interstellar shocks, provided that the carbonaceous component is hydrogenated amorphous carbon and carbon abundances are correct. Variations in relative abundances of refractories in gas suggest variations in the history of grain destruction in nearby ISM. The large observed grains, &gt; 1 micron, may indicate a nearby reservoir of denser ISM. Theoretical three-dimensional models of the interaction between interstellar dust grains and the solar wind predict that plumes of about 0.18 micron dust grains form around the heliosphere.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/interstellar-dust-close-to-the-sun/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Galaxy evolution in groups and clusters: star formation rates, red sequence fractions, and the persistent bimodality [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/galaxy-evolution-in-groups-and-clusters-star-formation-rates-red-sequence-fractions-and-the-persistent-bimodality-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/galaxy-evolution-in-groups-and-clusters-star-formation-rates-red-sequence-fractions-and-the-persistent-bimodality-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:36:28 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bimodal]]></category>
		<category><![CDATA[central galaxy]]></category>
		<category><![CDATA[cluster catalogs]]></category>
		<category><![CDATA[companion paper]]></category>
		<category><![CDATA[digital sky survey]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[galaxy evolution]]></category>
		<category><![CDATA[galaxy group]]></category>
		<category><![CDATA[halo 2]]></category>
		<category><![CDATA[halo center]]></category>
		<category><![CDATA[massive cluster]]></category>
		<category><![CDATA[msol]]></category>
		<category><![CDATA[satellite galaxy]]></category>
		<category><![CDATA[sky survey data]]></category>
		<category><![CDATA[sloan digital]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[strong break]]></category>
		<category><![CDATA[vir]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/galaxy-evolution-in-groups-and-clusters-star-formation-rates-red-sequence-fractions-and-the-persistent-bimodality-replacement/</guid>
		<description><![CDATA[Using galaxy group/cluster catalogs created from the Sloan Digital Sky Survey Data Release 7, we examine in detail the specific star formation rate (SSFR) distribution of satellite galaxies and its dependence on stellar mass, host halo mass, and halo-centric radius. All galaxies, regardless of central-satellite designation, exhibit a similar bimodal SSFR distribution, with a strong [...]]]></description>
			<content:encoded><![CDATA[<p>Using galaxy group/cluster catalogs created from the Sloan Digital Sky Survey Data Release 7, we examine in detail the specific star formation rate (SSFR) distribution of satellite galaxies and its dependence on stellar mass, host halo mass, and halo-centric radius. All galaxies, regardless of central-satellite designation, exhibit a similar bimodal SSFR distribution, with a strong break at SSFR ~ 10^-11 yr^-1 and the same high SSFR peak; in no regime is there ever an excess of galaxies in the `green valley&#8217;. Satellite galaxies are simply more likely to lie on the quenched (`red sequence&#8217;) side of the SSFR distribution. Furthermore, the satellite quenched fraction excess above the field galaxy value is nearly independent of galaxy stellar mass. An enhanced quenched fraction for satellites persists in groups with halo masses down to 3 x 10^11 Msol and increases strongly with halo mass and toward halo center. We find no detectable quenching enhancement for galaxies beyond ~2R_vir around massive clusters once these galaxies have been decomposed into centrals and satellites. These trends imply that (1) galaxies experience no significant environmental effects until they cross within ~R_vir of a more massive host halo, (2) after this, star formation in active satellites continues to evolve in the same manner as active central galaxies for several Gyrs, and (3) once begun, satellite star formation quenching occurs rapidly. These results place strong constraints on satellite-specific quenching mechanisms, as we will discuss further in companion papers.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/galaxy-evolution-in-groups-and-clusters-star-formation-rates-red-sequence-fractions-and-the-persistent-bimodality-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Kicking massive black holes off clusters: Intermediate-mass ratio inspirals [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/kicking-massive-black-holes-off-clusters-intermediate-mass-ratio-inspirals-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/kicking-massive-black-holes-off-clusters-intermediate-mass-ratio-inspirals-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:35:33 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[compact object]]></category>
		<category><![CDATA[dynamical evolution]]></category>
		<category><![CDATA[energy loss]]></category>
		<category><![CDATA[escape velocity]]></category>
		<category><![CDATA[global dynamics]]></category>
		<category><![CDATA[globular cluster]]></category>
		<category><![CDATA[gravitational radiation]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[imbh]]></category>
		<category><![CDATA[imri]]></category>
		<category><![CDATA[inspiral]]></category>
		<category><![CDATA[irrefutable proof]]></category>
		<category><![CDATA[mass ratio]]></category>
		<category><![CDATA[mission options]]></category>
		<category><![CDATA[msun]]></category>
		<category><![CDATA[relativistic effects]]></category>
		<category><![CDATA[stellar kinematics]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[stellar system]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/kicking-massive-black-holes-off-clusters-intermediate-mass-ratio-inspirals-replacement/</guid>
		<description><![CDATA[Contrary to supermassive and stellar-mass black holes (SBHs), the existence of intermediate-mass black holes (IMBHs) with masses ranging between 100 and 10,000 Msun has not yet been confirmed. The main problem in the detection is that the innermost stellar kinematics of globular clusters (GCs), the natural loci to IMBHs, are very difficult to resolve. However, [...]]]></description>
			<content:encoded><![CDATA[<p>Contrary to supermassive and stellar-mass black holes (SBHs), the existence of intermediate-mass black holes (IMBHs) with masses ranging between 100 and 10,000 Msun has not yet been confirmed. The main problem in the detection is that the innermost stellar kinematics of globular clusters (GCs), the natural loci to IMBHs, are very difficult to resolve. However, if IMBHs reside in the center of GCs, a possibility is that they interact dynamically with their enviroment. A binary formed with the IMBH and a compact object of the GC would naturally lead to a prominent source of gravitational radiation, detectable with future observatories. We run for the first time direct-summation integrations of GCs with an IMBH including the dynamical evolution of the IMBH with the stellar system and relativistic effects, such as energy loss in gravitational waves (GWs) and periapsis shift, and gravitational recoil. We find in one of our models an intermediate-mass ratio inspiral (IMRI), which leads to a merger with a recoiling velocity higher than the escape velocity of the GC. The GWs emitted fall in the range of frequencies that a LISA-like observatory could detect, like the European eLISA or in mission options considered in the recent preliminary mission study conducted in China. The merger has an impact on the global dynamics of the cluster, as an important heating source is removed when the merged system leaves the GC. The detection of one IMRI would constitute a test of GR, as well as an irrefutable proof of the existence of IMBHs.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/kicking-massive-black-holes-off-clusters-intermediate-mass-ratio-inspirals-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Turbulent dynamo with advective magnetic helicity flux</title>
		<link>http://voxcharta.org/2012/05/16/turbulent-dynamo-with-advective-magnetic-helicity-flux/</link>
		<comments>http://voxcharta.org/2012/05/16/turbulent-dynamo-with-advective-magnetic-helicity-flux/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:55:18 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[advection]]></category>
		<category><![CDATA[alpha 2]]></category>
		<category><![CDATA[borders]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[dynamo processes]]></category>
		<category><![CDATA[eddies]]></category>
		<category><![CDATA[evolution equation]]></category>
		<category><![CDATA[galactic wind]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetic helicity]]></category>
		<category><![CDATA[numerical simulation]]></category>
		<category><![CDATA[outer boundary]]></category>
		<category><![CDATA[phenomenon]]></category>
		<category><![CDATA[relative role]]></category>
		<category><![CDATA[reynolds number]]></category>
		<category><![CDATA[Turbulence]]></category>
		<category><![CDATA[wavenumber]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/turbulent-dynamo-with-advective-magnetic-helicity-flux/</guid>
		<description><![CDATA[Many astrophysical bodies harbor magnetic fields that are thought to be sustained by dynamo processes. However, it has been argued that the production of large-scale magnetic fields by a mean-field dynamo is strongly suppressed at large magnetic Reynolds numbers owing to the conservation of magnetic helicity. This phenomenon is known as catastrophic quenching. Advection of [...]]]></description>
			<content:encoded><![CDATA[<p>Many astrophysical bodies harbor magnetic fields that are thought to be sustained by dynamo processes. However, it has been argued that the production of large-scale magnetic fields by a mean-field dynamo is strongly suppressed at large magnetic Reynolds numbers owing to the conservation of magnetic helicity. This phenomenon is known as catastrophic quenching. Advection of magnetic field toward the outer boundaries and away from the dynamo is expected to alleviate such quenching. Examples are stellar and galactic winds. Such advection might be able to overcome the constraint imposed by the conservation of magnetic helicity, transporting a fraction of it outside the domain in which the dynamo operates. We study how the dynamo process is affected by advection. In particular, we study the relative roles played by advective and diffusive fluxes of magnetic helicity. We do this by performing direct numerical simulations of a turbulent dynamo of alpha^2 type driven by forced turbulence in a Cartesian domain in the presence of a constant flow toward the upper and lower borders of the domain. We demonstrate that, within the range of magnetic Reynolds number examined (\Rm &lt; 200, based on the wavenumber of the energy-carrying eddies), the resistive term still dominates over the advective one in the evolution equation of magnetic helicity. This means that for the Rm presently accessible, advection does not alleviate the quenching. Our results lead us to estimate that for Rm ~ 4.10^3. catastrophic quenching can be alleviated by the presence of advection. We also find that in the presence of advection the dynamo, otherwise stationary, becomes oscillatory.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/turbulent-dynamo-with-advective-magnetic-helicity-flux/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The `harder when brighter&#8217; X-ray behaviour of the low luminosity active galactic nucleus NGC 7213</title>
		<link>http://voxcharta.org/2012/05/16/the-harder-when-brighter-x-ray-behaviour-of-the-low-luminosity-active-galactic-nucleus-ngc-7213/</link>
		<comments>http://voxcharta.org/2012/05/16/the-harder-when-brighter-x-ray-behaviour-of-the-low-luminosity-active-galactic-nucleus-ngc-7213/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:53:43 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[eddington limit]]></category>
		<category><![CDATA[electromagnetic spectrum]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[galactic nucleus]]></category>
		<category><![CDATA[gamma]]></category>
		<category><![CDATA[hardness ratio]]></category>
		<category><![CDATA[literature]]></category>
		<category><![CDATA[nuclear emission]]></category>
		<category><![CDATA[optical data]]></category>
		<category><![CDATA[photon index]]></category>
		<category><![CDATA[positive correlation]]></category>
		<category><![CDATA[ray binaries]]></category>
		<category><![CDATA[ray fluxes]]></category>
		<category><![CDATA[robust evidence]]></category>
		<category><![CDATA[spectral energy distribution]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/the-harder-when-brighter-x-ray-behaviour-of-the-low-luminosity-active-galactic-nucleus-ngc-7213/</guid>
		<description><![CDATA[We present the first robust evidence of an anti-correlation between the X-ray photon index, \Gamma, and the X-ray luminosity in a single low luminosity active galactic nuclei (LLAGN), NGC 7213. Up to now, such anti-correlation trends have been seen only in large samples of LLAGN that span a wide range of X-ray fluxes, although the [...]]]></description>
			<content:encoded><![CDATA[<p>We present the first robust evidence of an anti-correlation between the X-ray photon index, \Gamma, and the X-ray luminosity in a single low luminosity active galactic nuclei (LLAGN), NGC 7213. Up to now, such anti-correlation trends have been seen only in large samples of LLAGN that span a wide range of X-ray fluxes, although the opposite behaviour (i.e. a positive correlation between \Gamma and X-ray luminosity) has been extensively studied for individual X-ray bright active galactic nuclei. For NGC 7213, we use the long-term X-ray monitoring data of Rossi X-ray Timing Explorer (RXTE), regularly obtained on average every two days from March 2006 to December 2009. Based on our X-ray data, we derive the \Gamma versus flux and the hardness ratio versus flux relations, indicating clearly that NGC 7213 follows a `harder when brighter&#8217; spectral behaviour. Additionally, by analysing radio and optical data, and combining data from the literature, we form the most complete spectral energy distribution (SED) of the source across the electromagnetic spectrum yielding a bolometric luminosity of 1.7*10^43 erg s^-1. Phenomenologically, the SED of NGC 7213 is similar to that of low-ionization nuclear emission-line region. The robust anti-correlation trend that we find between \Gamma and X-ray luminosity together with the low accretion rate of the source, 0.14 per cent that of Eddington limit, make NGC 7213 the first LLAGN exhibiting a similar spectral behaviour with that of black hole X-ray binaries in `hard state&#8217;.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/the-harder-when-brighter-x-ray-behaviour-of-the-low-luminosity-active-galactic-nucleus-ngc-7213/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>870 micron Imaging of a Transitional Disk in Upper Scorpius: Holdover from the Era of Giant Planet Formation?</title>
		<link>http://voxcharta.org/2012/05/16/870-micron-imaging-of-a-transitional-disk-in-upper-scorpius-holdover-from-the-era-of-giant-planet-formation/</link>
		<comments>http://voxcharta.org/2012/05/16/870-micron-imaging-of-a-transitional-disk-in-upper-scorpius-holdover-from-the-era-of-giant-planet-formation/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:52:28 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[binary companion]]></category>
		<category><![CDATA[giant planet]]></category>
		<category><![CDATA[giant planet formation]]></category>
		<category><![CDATA[grains]]></category>
		<category><![CDATA[holdover]]></category>
		<category><![CDATA[images]]></category>
		<category><![CDATA[inner cavity]]></category>
		<category><![CDATA[jupiter masses]]></category>
		<category><![CDATA[micron imaging]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[solar mass star]]></category>
		<category><![CDATA[spectral energy distribution]]></category>
		<category><![CDATA[surface density]]></category>
		<category><![CDATA[transition]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/870-micron-imaging-of-a-transitional-disk-in-upper-scorpius-holdover-from-the-era-of-giant-planet-formation/</guid>
		<description><![CDATA[We present 880 micron images of the transition disk around the star [PZ99] J160421.7-213028, a solar-mass star in the nearby Upper Scorpius association. With a resolution down to 0.34 arcsec, we resolve the inner hole in this disk, and via model fitting to the visibilities and spectral energy distribution we determine both the structure of [...]]]></description>
			<content:encoded><![CDATA[<p>We present 880 micron images of the transition disk around the star [PZ99] J160421.7-213028, a solar-mass star in the nearby Upper Scorpius association. With a resolution down to 0.34 arcsec, we resolve the inner hole in this disk, and via model fitting to the visibilities and spectral energy distribution we determine both the structure of the outer region and the presence of sparse dust within the cavity. The disk contains about 0.1 Jupiter masses of mm-emitting grains, with an inner disk edge of about 70 AU. The inner cavity contains a small amount of dust with a depleted surface density in a region extending from about 20-70 AU. Taking into account prior observations indicating little to no stellar accretion, the lack of a binary companion, and the presence of dust near 0.1 AU, we determine that the most likely mechanism for the formation of this inner hole is the presence of one or more giant planets.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/870-micron-imaging-of-a-transitional-disk-in-upper-scorpius-holdover-from-the-era-of-giant-planet-formation/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Chemical compositions of thin-disk, high-metallicity red horizontal-branch field stars</title>
		<link>http://voxcharta.org/2012/05/16/chemical-compositions-of-thin-disk-high-metallicity-red-horizontal-branch-field-stars/</link>
		<comments>http://voxcharta.org/2012/05/16/chemical-compositions-of-thin-disk-high-metallicity-red-horizontal-branch-field-stars/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:47:24 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[atmospheric parameters]]></category>
		<category><![CDATA[chemical composition]]></category>
		<category><![CDATA[eff]]></category>
		<category><![CDATA[equivalent width]]></category>
		<category><![CDATA[field star]]></category>
		<category><![CDATA[horizontal branch]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[M. Smith]]></category>
		<category><![CDATA[mcdonald observatory]]></category>
		<category><![CDATA[neutron]]></category>
		<category><![CDATA[ratios]]></category>
		<category><![CDATA[relative abundance]]></category>
		<category><![CDATA[smith telescope]]></category>
		<category><![CDATA[solar metallicity]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectrum analyses]]></category>
		<category><![CDATA[stellar evolution]]></category>
		<category><![CDATA[target star]]></category>
		<category><![CDATA[thin disk]]></category>
		<category><![CDATA[velocities]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/chemical-compositions-of-thin-disk-high-metallicity-red-horizontal-branch-field-stars/</guid>
		<description><![CDATA[We present a detailed abundance analysis and atmospheric parameters of 76 stars from a survey to identify field Galactic red horizontal-branch (RHB) stars. High-resolution echelle spectra (R\simeq60,000, S/N&#62;=100) were obtained with 2.7 m Smith Telescope at McDonald Observatory. The target stars were selected only by color and parallax information. Overall metallicities and relative abundances of [...]]]></description>
			<content:encoded><![CDATA[<p>We present a detailed abundance analysis and atmospheric parameters of 76 stars from a survey to identify field Galactic red horizontal-branch (RHB) stars. High-resolution echelle spectra (R\simeq60,000, S/N&gt;=100) were obtained with 2.7 m Smith Telescope at McDonald Observatory. The target stars were selected only by color and parallax information. Overall metallicities and relative abundances of proton-capture elements (C I, N I, O I, Li I), alpha-elements (Ca I and Si I), and neutron-capture elements (Eu II and La II) were determined by either equivalent width or synthetic spectrum analyses. We used CN features at 7995-8040 {\AA} region in order to determine 12^C/13^C ratios of our targets. Investigation of the evolutionary stages, using spectroscopic T_eff and log g values along with derived 12^C/13^C ratios, revealed the presence of 18 probable RHB stars in our sample. We also derived kinematics of the stars with available distance information. Taking into account both the kinematics and probable evolutionary stages, we conclude that our sample contains five thick disk and 13 thin disk RHB stars. Up until now, RHB stars have been considered as members of the thick disk, and were expected to have large space velocities and sub-solar metallicities. However, our sample is dominated by low velocity solar-metallicity RHB stars; their existence cannot be easily explained with standard stellar evolution.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/chemical-compositions-of-thin-disk-high-metallicity-red-horizontal-branch-field-stars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Radial molecular abundances and gas cooling in starless cores</title>
		<link>http://voxcharta.org/2012/05/16/radial-molecular-abundances-and-gas-cooling-in-starless-cores/</link>
		<comments>http://voxcharta.org/2012/05/16/radial-molecular-abundances-and-gas-cooling-in-starless-cores/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:47:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abundance gradients]]></category>
		<category><![CDATA[chemical species]]></category>
		<category><![CDATA[cm 3]]></category>
		<category><![CDATA[conclusion]]></category>
		<category><![CDATA[core]]></category>
		<category><![CDATA[core stability]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[ebert]]></category>
		<category><![CDATA[exceptions]]></category>
		<category><![CDATA[gas density]]></category>
		<category><![CDATA[gas temperature]]></category>
		<category><![CDATA[grain surface]]></category>
		<category><![CDATA[iterative process]]></category>
		<category><![CDATA[line emission]]></category>
		<category><![CDATA[molecule]]></category>
		<category><![CDATA[profile]]></category>
		<category><![CDATA[radiative transfer model]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[sphere]]></category>
		<category><![CDATA[time step]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/radial-molecular-abundances-and-gas-cooling-in-starless-cores/</guid>
		<description><![CDATA[Aims: We aim to simulate radial profiles of molecular abundances and the gas temperature in cold and heavily shielded starless cores by combining chemical and radiative transfer models. Methods: A determination of the dust temperature in a modified Bonnor-Ebert sphere is used to calculate initial radial molecular abundance profiles. The abundances of selected cooling molecules [...]]]></description>
			<content:encoded><![CDATA[<p>Aims: We aim to simulate radial profiles of molecular abundances and the gas temperature in cold and heavily shielded starless cores by combining chemical and radiative transfer models. Methods: A determination of the dust temperature in a modified Bonnor-Ebert sphere is used to calculate initial radial molecular abundance profiles. The abundances of selected cooling molecules corresponding to two different core ages are then extracted to determine the gas temperature at two time steps. The calculation is repeated in an iterative process yielding molecular abundances consistent with the gas temperature. Line emission profiles for selected substances are calculated using simulated abundance profiles. Results: The gas temperature is a function of time; the gas heats up as the core gets older because the cooling molecules are depleted onto grain surfaces. The contributions of the various cooling molecules to the total cooling power change with time. Radial chemical abundance profiles are non-trivial: different species present varying degrees of depletion and in some cases inward-increasing abundances profiles, even at t &gt; 10^5 years. Line emission simulations indicate that cores of different ages can present significantly different line emission profiles, depending on the tracer species considered. Conclusions: Chemical abundances and the associated line cooling power change as a function of time. Most chemical species are depleted onto grain surfaces at densities exceeding ~10^5 cm^-3. Notable exceptions are NH_3 and N2H^+; the latter is largely undepleted even at n_H~10^6 cm-3. On the other hand, chemical abundances are not significantly developed in regions of low gas density even at t~10^5 years, revealed by inward-increasing abundance gradients. The gas temperature can be significantly different from the dust temperature; this may have implications on core stability.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/radial-molecular-abundances-and-gas-cooling-in-starless-cores/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>The anticentre old open clusters Berkeley 27, Berkeley 34, and Berkeley 36: new additions to the BOCCE project</title>
		<link>http://voxcharta.org/2012/05/16/the-anticentre-old-open-clusters-berkeley-27-berkeley-34-and-berkeley-36-new-additions-to-the-bocce-project/</link>
		<comments>http://voxcharta.org/2012/05/16/the-anticentre-old-open-clusters-berkeley-27-berkeley-34-and-berkeley-36-new-additions-to-the-bocce-project/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:46:21 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[berkeley]]></category>
		<category><![CDATA[bessel]]></category>
		<category><![CDATA[cmd]]></category>
		<category><![CDATA[colour magnitude diagram]]></category>
		<category><![CDATA[evolutionary status]]></category>
		<category><![CDATA[galactic disc]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[new addition]]></category>
		<category><![CDATA[ntt]]></category>
		<category><![CDATA[open cluster]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[solar metallicity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/the-anticentre-old-open-clusters-berkeley-27-berkeley-34-and-berkeley-36-new-additions-to-the-bocce-project/</guid>
		<description><![CDATA[In this paper we present the investigation of the evolutionary status of three open clusters: Berkeley 27, Berkeley 34, and Berkeley 36, all located in the Galactic anti-centre direction. All of them were observed with SUSI2@NTT using the Bessel B, V, and I filters. The cluster parameters have been obtained using the synthetic colour-magnitude diagram [...]]]></description>
			<content:encoded><![CDATA[<p>In this paper we present the investigation of the evolutionary status of three open clusters: Berkeley 27, Berkeley 34, and Berkeley 36, all located in the Galactic anti-centre direction. All of them were observed with SUSI2@NTT using the Bessel B, V, and I filters. The cluster parameters have been obtained using the synthetic colour-magnitude diagram (CMD) method i.e. the direct comparison of the observational CMDs with a library of synthetic CMDs generated with different evolutionary sets (Padova, FRANEC, and FST). This analysis shows that Berkeley 27 has an age between 1.5 and 1.7 Gyr, a reddening E(B-V) in the range 0.40 and 0.50, and a distance modulus (m-M)_0 between 13.1 and 13.3; Berkeley 34 is older with an age in the range 2.1 and 2.5 Gyr, E(B-V) between 0.57 and 0.64, and (m-M)_0 between 14.1 and 14.3; Berkeley 36, with an age between 7.0 and 7.5 Gyr, has a reddening E(B-V)~0.50 and a distance modulus (m-M)_0 between 13.1 and 13.2. For all the clusters our analysis suggests a sub-solar metallicity in accord with their position in the outer Galactic disc.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/the-anticentre-old-open-clusters-berkeley-27-berkeley-34-and-berkeley-36-new-additions-to-the-bocce-project/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Tests of the universality of free fall for strongly self-gravitating bodies with radio pulsars [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/16/tests-of-the-universality-of-free-fall-for-strongly-self-gravitating-bodies-with-radio-pulsars-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/16/tests-of-the-universality-of-free-fall-for-strongly-self-gravitating-bodies-with-radio-pulsars-cross-listing/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:41:56 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[binary system]]></category>
		<category><![CDATA[binding energy]]></category>
		<category><![CDATA[equivalence principle]]></category>
		<category><![CDATA[extreme difference]]></category>
		<category><![CDATA[future prospect]]></category>
		<category><![CDATA[globular cluster]]></category>
		<category><![CDATA[measurement precision]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[orbital eccentricity]]></category>
		<category><![CDATA[orbital motion]]></category>
		<category><![CDATA[phenomenon]]></category>
		<category><![CDATA[precise measurement]]></category>
		<category><![CDATA[probabilistic considerations]]></category>
		<category><![CDATA[pulsar data]]></category>
		<category><![CDATA[radiation]]></category>
		<category><![CDATA[radio pulsar]]></category>
		<category><![CDATA[types of tests]]></category>
		<category><![CDATA[universality]]></category>
		<category><![CDATA[variation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/tests-of-the-universality-of-free-fall-for-strongly-self-gravitating-bodies-with-radio-pulsars-cross-listing/</guid>
		<description><![CDATA[In this paper, we review tests of the strong equivalence principle (SEP) derived from binary pulsar data. The extreme difference in binding energy between both components and the precise measurement of the orbital motion provided by pulsar timing allow the only current precision SEP tests for strongly self-gravitating bodies. We start by highlighting why such [...]]]></description>
			<content:encoded><![CDATA[<p>In this paper, we review tests of the strong equivalence principle (SEP) derived from binary pulsar data. The extreme difference in binding energy between both components and the precise measurement of the orbital motion provided by pulsar timing allow the only current precision SEP tests for strongly self-gravitating bodies. We start by highlighting why such tests are conceptually important. We then review previous work where limits on SEP violation are obtained with an ensemble of wide binary systems with small eccentricity orbits. Then we propose a new SEP violation test based on the measurement of the variation of the orbital eccentricity de/dt. This new method has the following advantages: a) unlike previous methods it is not based on probabilistic considerations, b) it can make a direct detection of SEP violation, c) the measurement of de/dt is not contaminated by any known external effects, which implies that this SEP test is only restricted by the measurement precision of de/dt. In the final part of the review, we conceptually compare the SEP test with the test for dipolar radiation damping, a phenomenon closely related to SEP violation, and speculate on future prospects by new types of tests in globular clusters and future triple systems.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/tests-of-the-universality-of-free-fall-for-strongly-self-gravitating-bodies-with-radio-pulsars-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Hubble Space Telescope Observations of an Outer Field in Omega Centauri: A Definitive Helium Abundance</title>
		<link>http://voxcharta.org/2012/05/16/hubble-space-telescope-observations-of-an-outer-field-in-omega-centauri-a-definitive-helium-abundance/</link>
		<comments>http://voxcharta.org/2012/05/16/hubble-space-telescope-observations-of-an-outer-field-in-omega-centauri-a-definitive-helium-abundance/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:41:40 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cluster center]]></category>
		<category><![CDATA[cluster member]]></category>
		<category><![CDATA[differential]]></category>
		<category><![CDATA[globular cluster]]></category>
		<category><![CDATA[helium abundance]]></category>
		<category><![CDATA[high quality]]></category>
		<category><![CDATA[hubble space telescope]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[main sequence]]></category>
		<category><![CDATA[omega centauri]]></category>
		<category><![CDATA[proper motion]]></category>
		<category><![CDATA[sequence]]></category>
		<category><![CDATA[stellar model]]></category>
		<category><![CDATA[telescope observations]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/hubble-space-telescope-observations-of-an-outer-field-in-omega-centauri-a-definitive-helium-abundance/</guid>
		<description><![CDATA[We revisit the problem of the split main sequence (MS) of the globular cluster omega Centauri, and report the results of two-epoch Hubble Space Telescope observations of an outer field, for which proper motions give us a pure sample of cluster members, and an improved separation of the two branches of the main sequence. Using [...]]]></description>
			<content:encoded><![CDATA[<p>We revisit the problem of the split main sequence (MS) of the globular cluster omega Centauri, and report the results of two-epoch Hubble Space Telescope observations of an outer field, for which proper motions give us a pure sample of cluster members, and an improved separation of the two branches of the main sequence. Using a new set of stellar models covering a grid of values of helium and metallicity, we find that the best possible estimate of the helium abundance of the bluer branch of the MS is Y = 0.39 +/- 0.02. For the cluster center we apply new techniques to old observations: we use indices of photometric quality to select a high-quality sample of stars, which we also correct for differential reddening. We then superpose the color-magnitude diagram of the outer field on that of the cluster center, and suggest a connection of the bluer branch of the MS with one of the more prominent among the many sequences in the subgiant region. We also report a group of undoubted cluster members that are well to the red of the lower MS.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/hubble-space-telescope-observations-of-an-outer-field-in-omega-centauri-a-definitive-helium-abundance/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>What turns galaxies off? The different morphologies of star-forming and quiescent galaxies since z~2 from CANDELS [Replacement]</title>
		<link>http://voxcharta.org/2012/05/16/what-turns-galaxies-off-the-different-morphologies-of-star-forming-and-quiescent-galaxies-since-z2-from-candels-replacement/</link>
		<comments>http://voxcharta.org/2012/05/16/what-turns-galaxies-off-the-different-morphologies-of-star-forming-and-quiescent-galaxies-since-z2-from-candels-replacement/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:39:43 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[candels]]></category>
		<category><![CDATA[digital sky survey]]></category>
		<category><![CDATA[dramatic increase]]></category>
		<category><![CDATA[galactic structure]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[galaxy structure]]></category>
		<category><![CDATA[mass star]]></category>
		<category><![CDATA[multicycle]]></category>
		<category><![CDATA[number density]]></category>
		<category><![CDATA[optical color]]></category>
		<category><![CDATA[present day]]></category>
		<category><![CDATA[rest frame]]></category>
		<category><![CDATA[sloan digital]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[stellar surface]]></category>
		<category><![CDATA[surface density]]></category>
		<category><![CDATA[time span]]></category>
		<category><![CDATA[velocity dispersion]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/what-turns-galaxies-off-the-different-morphologies-of-star-forming-and-quiescent-galaxies-since-z2-from-candels-replacement/</guid>
		<description><![CDATA[We use HST/WFC3 imaging from the CANDELS Multicycle Treasury Survey, in conjunction with the Sloan Digital Sky Survey, to explore the evolution of galactic structure for galaxies with stellar masses &#62;3e10M_sun from z=2.2 to the present epoch, a time span of 10Gyr. We explore the relationship between rest-frame optical color, stellar mass, star formation activity [...]]]></description>
			<content:encoded><![CDATA[<p>We use HST/WFC3 imaging from the CANDELS Multicycle Treasury Survey, in conjunction with the Sloan Digital Sky Survey, to explore the evolution of galactic structure for galaxies with stellar masses &gt;3e10M_sun from z=2.2 to the present epoch, a time span of 10Gyr. We explore the relationship between rest-frame optical color, stellar mass, star formation activity and galaxy structure. We confirm the dramatic increase from z=2.2 to the present day in the number density of non-star-forming galaxies above 3e10M_sun reported by others. We further find that the vast majority of these quiescent systems have concentrated light profiles, as parametrized by the Sersic index, and the population of concentrated galaxies grows similarly rapidly. We examine the joint distribution of star formation activity, Sersic index, stellar mass, inferred velocity dispersion, and stellar surface density. Quiescence correlates poorly with stellar mass at all z1.3, and somewhat less well at lower redshifts. Yet, there is significant scatter between quiescence and galaxy structure: while the vast majority of quiescent galaxies have prominent bulges, many of them have significant disks, and a number of bulge-dominated galaxies have significant star formation. Noting the rarity of quiescent galaxies without prominent bulges, we argue that a prominent bulge (and perhaps, by association, a supermassive black hole) is an important condition for quenching star formation on galactic scales over the last 10Gyr, in qualitative agreement with the AGN feedback paradigm.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/what-turns-galaxies-off-the-different-morphologies-of-star-forming-and-quiescent-galaxies-since-z2-from-candels-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>On the Stability of Super Earth Atmospheres [Replacement]</title>
		<link>http://voxcharta.org/2012/05/16/on-the-stability-of-super-earth-atmospheres-replacement/</link>
		<comments>http://voxcharta.org/2012/05/16/on-the-stability-of-super-earth-atmospheres-replacement/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:36:41 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[advection]]></category>
		<category><![CDATA[atmosphere]]></category>
		<category><![CDATA[condensation]]></category>
		<category><![CDATA[constituent]]></category>
		<category><![CDATA[dataset]]></category>
		<category><![CDATA[dual effect]]></category>
		<category><![CDATA[exoplanet]]></category>
		<category><![CDATA[g star]]></category>
		<category><![CDATA[gas phase]]></category>
		<category><![CDATA[habitable zone]]></category>
		<category><![CDATA[k star]]></category>
		<category><![CDATA[kepler]]></category>
		<category><![CDATA[major axis]]></category>
		<category><![CDATA[molecular weight]]></category>
		<category><![CDATA[nightside]]></category>
		<category><![CDATA[parameter space]]></category>
		<category><![CDATA[solid surface]]></category>
		<category><![CDATA[super earth]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/on-the-stability-of-super-earth-atmospheres-replacement/</guid>
		<description><![CDATA[We investigate the stability of super Earth atmospheres around M stars using a 7-parameter, analytical framework. We construct stability diagrams in the parameter space of exoplanetary radius versus semi-major axis and elucidate the regions in which the atmospheres are stable against the condensation of their major constituents, out of the gas phase, on their permanent [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate the stability of super Earth atmospheres around M stars using a 7-parameter, analytical framework. We construct stability diagrams in the parameter space of exoplanetary radius versus semi-major axis and elucidate the regions in which the atmospheres are stable against the condensation of their major constituents, out of the gas phase, on their permanent nightside hemispheres. We find that super Earth atmospheres which are nitrogen-dominated (&#8220;Earth-like&#8221;) occupy a smaller region of allowed parameter space, compared to hydrogen-dominated atmospheres, because of the dual effects of diminished advection and enhanced radiative cooling. Furthermore, some super Earths which reside within the habitable zones of M stars may not possess stable atmospheres, depending on the mean molecular weight and infrared photospheric pressure of their atmospheres. We apply our stability diagrams to GJ 436b and GJ 1214b, and demonstrate that atmospheric compositions with high mean molecular weights are disfavoured if these exoplanets possess solid surfaces and shallow atmospheres. Finally, we construct stability diagrams tailored to the Kepler dataset, for G and K stars, and predict that about half of the exoplanet candidates are expected to habour stable atmospheres if Earth-like conditions are assumed. We include 55 Cancri e and CoRoT-7b in our stability diagram for G stars.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/on-the-stability-of-super-earth-atmospheres-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A new low magnetic field magnetar: the 2011 outburst of Swift J1822.3-1606 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/16/a-new-low-magnetic-field-magnetar-the-2011-outburst-of-swift-j1822-3-1606-replacement/</link>
		<comments>http://voxcharta.org/2012/05/16/a-new-low-magnetic-field-magnetar-the-2011-outburst-of-swift-j1822-3-1606-replacement/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:34:53 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[dipolar]]></category>
		<category><![CDATA[gbt]]></category>
		<category><![CDATA[gran telescopio canarias]]></category>
		<category><![CDATA[green bank telescope]]></category>
		<category><![CDATA[kyr]]></category>
		<category><![CDATA[magnetar]]></category>
		<category><![CDATA[optical emission]]></category>
		<category><![CDATA[order of magnitude]]></category>
		<category><![CDATA[outburst]]></category>
		<category><![CDATA[quiescent state]]></category>
		<category><![CDATA[Ray Bursts]]></category>
		<category><![CDATA[rosat observations]]></category>
		<category><![CDATA[rxte]]></category>
		<category><![CDATA[spectral evolution]]></category>
		<category><![CDATA[suzaku]]></category>
		<category><![CDATA[thermal evolution]]></category>
		<category><![CDATA[time span]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xmm newton]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/a-new-low-magnetic-field-magnetar-the-2011-outburst-of-swift-j1822-3-1606-replacement/</guid>
		<description><![CDATA[We report on the long term X-ray monitoring with Swift, RXTE, Suzaku, Chandra and XMM-Newton of the outburst of the newly discovered magnetar Swift J1822.3-1606 (SGR 1822-1606), from the first observations soon after the detection of the short X-ray bursts which led to its discovery, through the first stages of its outburst decay (covering the [...]]]></description>
			<content:encoded><![CDATA[<p>We report on the long term X-ray monitoring with Swift, RXTE, Suzaku, Chandra and XMM-Newton of the outburst of the newly discovered magnetar Swift J1822.3-1606 (SGR 1822-1606), from the first observations soon after the detection of the short X-ray bursts which led to its discovery, through the first stages of its outburst decay (covering the time-span from July 2011, until end of April 2012). We also report on archival ROSAT observations which witnessed the source during its likely quiescent state, and on upper limits on Swift J1822.3-1606&#8217;s radio-pulsed and optical emission during outburst, with the Green Bank Telescope (GBT) and the Gran Telescopio Canarias (GTC), respectively. Our X-ray timing analysis finds the source rotating with a period of P=8.43772016(2) s and a period derivative \dot{P}=8.3(2)x10^{-14} s s^{-1} , which entails an inferred dipolar surface magnetic field of B~2.7&#215;10^{13} G at the equator. This measurement makes Swift J1822.3-1606 the second lowest magnetic field magnetar (after SGR 0418+5729; Rea et al. 2010). Following the flux and spectral evolution from the beginning of the outburst, we find that the flux decreased by about an order of magnitude, with a subtle softening of the spectrum, both typical of the outburst decay of magnetars. By modeling the secular thermal evolution of Swift J1822.3-1606, we find that the observed timing properties of the source, as well as its quiescent X-ray luminosity, can be reproduced if it was born with a poloidal and crustal toroidal fields of B_{p}~1.5&#215;10^{14} G and B_{tor}~7&#215;10^{14} G, respectively, and if its current age is ~550 kyr.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/a-new-low-magnetic-field-magnetar-the-2011-outburst-of-swift-j1822-3-1606-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>The Absence of Ex-Companions in Type Ia Supernova Remnants</title>
		<link>http://voxcharta.org/2012/05/15/the-absence-of-ex-companions-in-type-ia-supernova-remnants/</link>
		<comments>http://voxcharta.org/2012/05/15/the-absence-of-ex-companions-in-type-ia-supernova-remnants/#comments</comments>
		<pubDate>Wed, 16 May 2012 01:04:33 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[100 000 years]]></category>
		<category><![CDATA[absence]]></category>
		<category><![CDATA[acceleration]]></category>
		<category><![CDATA[angular momentum]]></category>
		<category><![CDATA[companion]]></category>
		<category><![CDATA[companion star]]></category>
		<category><![CDATA[deep imaging]]></category>
		<category><![CDATA[exact nature]]></category>
		<category><![CDATA[explosion images]]></category>
		<category><![CDATA[large magellanic cloud]]></category>
		<category><![CDATA[natures]]></category>
		<category><![CDATA[probes]]></category>
		<category><![CDATA[progenitor]]></category>
		<category><![CDATA[remnant]]></category>
		<category><![CDATA[SNe]]></category>
		<category><![CDATA[supernova remnant]]></category>
		<category><![CDATA[systematic uncertainty]]></category>
		<category><![CDATA[type ia]]></category>
		<category><![CDATA[white dwarf]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/the-absence-of-ex-companions-in-type-ia-supernova-remnants/</guid>
		<description><![CDATA[Type Ia supernovae (SNe Ia) play important roles in our study of the expansion and acceleration of the Universe, but because we do not know the exact nature or natures of the progenitors, there is a systematic uncertainty that must be resolved if SNe Ia are to become more precise cosmic probes. No progenitor system [...]]]></description>
			<content:encoded><![CDATA[<p>Type Ia supernovae (SNe Ia) play important roles in our study of the expansion and acceleration of the Universe, but because we do not know the exact nature or natures of the progenitors, there is a systematic uncertainty that must be resolved if SNe Ia are to become more precise cosmic probes. No progenitor system has ever been identified either in the pre- or post-explosion images of a Ia event. There have been recent claims for and against the detection of ex-companion stars in several SNe Ia remnants. These studies, however, usually ignore the angular momentum gain of the progenitor white dwarf, which leads to a spin-up phase and a subsequent spin-down phase before explosion. For spin-down timescales greater than 100,000 years, the donor star could be too dim to detect by the time of explosion. Here we revisit the current limits on ex-companion stars to SNR 0509-67.5, a 400 year old remnant in the Large Magellanic Cloud. If the effects of possible angular momentum gain on the white dwarf are included, a wide range of single-degenerate progenitor models are allowed for this remnant. We demonstrate that the current absence of evidence for ex-companion stars in this remnant, as well as other SNe Ia remnants, does not necessarily provide the evidence of absence for ex-companions. We discuss potential ways to identify such ex-companion stars through deep imaging observations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/the-absence-of-ex-companions-in-type-ia-supernova-remnants/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Maximally Star-Forming Galactic Disks II. Vertically-Resolved Hydrodynamic Simulations of Starburst Regulation</title>
		<link>http://voxcharta.org/2012/05/15/maximally-star-forming-galactic-disks-ii-vertically-resolved-hydrodynamic-simulations-of-starburst-regulation/</link>
		<comments>http://voxcharta.org/2012/05/15/maximally-star-forming-galactic-disks-ii-vertically-resolved-hydrodynamic-simulations-of-starburst-regulation/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:56:45 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[angular velocity]]></category>
		<category><![CDATA[dense gas]]></category>
		<category><![CDATA[density environments]]></category>
		<category><![CDATA[dispersion]]></category>
		<category><![CDATA[free fall time]]></category>
		<category><![CDATA[galactic center]]></category>
		<category><![CDATA[galactic disk]]></category>
		<category><![CDATA[gas velocity]]></category>
		<category><![CDATA[high density]]></category>
		<category><![CDATA[momentum flux]]></category>
		<category><![CDATA[relevant quantity]]></category>
		<category><![CDATA[replenishment]]></category>
		<category><![CDATA[self regulation]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[steady state]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[supersonic turbulence]]></category>
		<category><![CDATA[surface density]]></category>
		<category><![CDATA[thicknesses]]></category>
		<category><![CDATA[vertical slices]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/maximally-star-forming-galactic-disks-ii-vertically-resolved-hydrodynamic-simulations-of-starburst-regulation/</guid>
		<description><![CDATA[We explore the self-regulation of star formation using a large suite of high resolution hydrodynamic simulations, focusing on molecule-dominated regions (galactic centers and [U]LIRGS) where feedback from star formation drives highly supersonic turbulence. In equilibrium the total midplane pressure, dominated by turbulence, must balance the vertical weight of the ISM. Under self-regulation, the momentum flux [...]]]></description>
			<content:encoded><![CDATA[<p>We explore the self-regulation of star formation using a large suite of high resolution hydrodynamic simulations, focusing on molecule-dominated regions (galactic centers and [U]LIRGS) where feedback from star formation drives highly supersonic turbulence. In equilibrium the total midplane pressure, dominated by turbulence, must balance the vertical weight of the ISM. Under self-regulation, the momentum flux injected by feedback evolves until it matches the vertical weight. We test this flux balance in simulations spanning a range of parameters, including surface density $\Sigma$, momentum injected per stellar mass formed ($p_*/m_*$), and angular velocity. The simulations are 2D radial-vertical slices, including both self-gravity and an external potential that confines gas to the disk midplane. After the simulations reach a steady state in all relevant quantities, including the star formation rate $\Sigma_{SFR}$, there is remarkably good agreement between the vertical weight, the turbulent pressure, and the momentum injection rate from supernovae. Gas velocity dispersions and disk thicknesses increase with $p_*/m_*$. The efficiency of star formation per free-fall time at the mid-plane density is insensitive to the local conditions and to the star formation prescription in very dense gas. We measure efficiencies $\sim$0.004-0.01, consistent with low and approximately constant efficiencies inferred from observations. For $\Sigma\in$(100&#8211;1000) \msunpc, we find $\Sigma_{SFR}\in$(0.1&#8211;4) \sfrunits, generally following a $\Sigma_{SFR}\propto \Sigma^2$ relationship. The measured relationships agree very well with vertical equilibrium and with turbulent energy replenishment by feedback within a vertical crossing time. These results, along with the observed $\Sigma_{SFR}-\Sigma$ relation in high density environments, provide strong evidence for the self-regulation of star formation.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/maximally-star-forming-galactic-disks-ii-vertically-resolved-hydrodynamic-simulations-of-starburst-regulation/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Slicing The Monoceros Overdensity with Suprime-Cam</title>
		<link>http://voxcharta.org/2012/05/15/slicing-the-monoceros-overdensity-with-suprime-cam/</link>
		<comments>http://voxcharta.org/2012/05/15/slicing-the-monoceros-overdensity-with-suprime-cam/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:54:45 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[deep imaging]]></category>
		<category><![CDATA[deg]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[density profile]]></category>
		<category><![CDATA[disc model]]></category>
		<category><![CDATA[distance]]></category>
		<category><![CDATA[galactic latitude]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[latitude]]></category>
		<category><![CDATA[longitude]]></category>
		<category><![CDATA[longitude range]]></category>
		<category><![CDATA[match]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[monoceros]]></category>
		<category><![CDATA[nearby star]]></category>
		<category><![CDATA[stripes]]></category>
		<category><![CDATA[subaru]]></category>
		<category><![CDATA[subaru telescope]]></category>
		<category><![CDATA[suprime]]></category>
		<category><![CDATA[tidal stream]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/slicing-the-monoceros-overdensity-with-suprime-cam/</guid>
		<description><![CDATA[We derive distance, density and metallicity distribution of the stellar Monoceros Overdensity (MO) in the outer Milky Way, based on deep imaging with the Subaru Telescope. We applied CMD fitting techniques in three stripes at galactic longitudes: l=130 deg, 150 deg, 170 deg; and galactic latitudes: +15 &#60; b [deg] &#60; +25 . The MO [...]]]></description>
			<content:encoded><![CDATA[<p>We derive distance, density and metallicity distribution of the stellar Monoceros Overdensity (MO) in the outer Milky Way, based on deep imaging with the Subaru Telescope. We applied CMD fitting techniques in three stripes at galactic longitudes: l=130 deg, 150 deg, 170 deg; and galactic latitudes: +15 &lt; b [deg] &lt; +25 . The MO appears as a wall of stars at a heliocentric distance of ~ 10.1\pm0.5 kpc across the observed longitude range with no distance change. The MO stars are more metal rich ([Fe/H] ~ -1.0) than the nearby stars at the same latitude. These data are used to test three different models for the origin of the MO: a perturbed disc model, which predicts a significant drop in density adjacent to the MO that is not seen; a basic flared disc model, which can give a good match to the density profile but the MO metallicity implies the disc is too metal rich to source the MO stars; and a tidal stream model, which bracket the distances and densities we derive for the MO, suggesting that a model can be found that would fully fit the MO data. Further data and modeling will be required to confirm or rule out the MO feature as a stream or as a flaring of the disc.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/slicing-the-monoceros-overdensity-with-suprime-cam/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Chandra Observations of the Nuclear Star Cluster and Ultraluminous X-ray Sources in NGC 2139</title>
		<link>http://voxcharta.org/2012/05/15/chandra-observations-of-the-nuclear-star-cluster-and-ultraluminous-x-ray-sources-in-ngc-2139/</link>
		<comments>http://voxcharta.org/2012/05/15/chandra-observations-of-the-nuclear-star-cluster-and-ultraluminous-x-ray-sources-in-ngc-2139/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:52:24 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[chandra observation]]></category>
		<category><![CDATA[chronometer]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[galaxy ngc]]></category>
		<category><![CDATA[hubble space telescope]]></category>
		<category><![CDATA[hubble space telescope images]]></category>
		<category><![CDATA[optical counterpart]]></category>
		<category><![CDATA[ray sources]]></category>
		<category><![CDATA[source population]]></category>
		<category><![CDATA[space telescope images]]></category>
		<category><![CDATA[star cluster]]></category>
		<category><![CDATA[star formation history]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[upper bound]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/chandra-observations-of-the-nuclear-star-cluster-and-ultraluminous-x-ray-sources-in-ngc-2139/</guid>
		<description><![CDATA[We report Chandra observations of the Scd galaxy NGC 2139, which is known to host a recently formed (10^7.6 yrs) nuclear star cluster. The star cluster is undetected in X-rays, with an upper bound on 0.5-7 keV luminosity of L_X &#60; 7.1 x 10^37 erg/s. This bound implies a bolometric accretion luminosity  10^39 erg/s. [...]]]></description>
			<content:encoded><![CDATA[<p>We report Chandra observations of the Scd galaxy NGC 2139, which is known to host a recently formed (10^7.6 yrs) nuclear star cluster. The star cluster is undetected in X-rays, with an upper bound on 0.5-7 keV luminosity of L_X &lt; 7.1 x 10^37 erg/s. This bound implies a bolometric accretion luminosity  10^39 erg/s. We use archival Hubble Space Telescope images to identify candidate optical counterparts for seven Chandra sources, which in most cases have optical luminosities and spatial profiles consistent with star clusters. Compared with other galaxies, the number of luminous X-ray sources in NGC 2139 is larger by a factor of 4 &#8211; 10 than expected based on its present star formation rate and stellar mass. This finding can be understood if NGC 2139 has concluded a burst of star formation in the recent past, and suggests that this galaxy could be important for testing the use of X-ray source populations as a chronometer of star formation history.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/chandra-observations-of-the-nuclear-star-cluster-and-ultraluminous-x-ray-sources-in-ngc-2139/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Resolving the Circumstellar Disk Around the Massive Protostar Driving the HH 80-81 Jet</title>
		<link>http://voxcharta.org/2012/05/15/resolving-the-circumstellar-disk-around-the-massive-protostar-driving-the-hh-80-81-jet/</link>
		<comments>http://voxcharta.org/2012/05/15/resolving-the-circumstellar-disk-around-the-massive-protostar-driving-the-hh-80-81-jet/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:46:17 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion disk]]></category>
		<category><![CDATA[continuum emission]]></category>
		<category><![CDATA[dust emission]]></category>
		<category><![CDATA[high angular resolution]]></category>
		<category><![CDATA[ira]]></category>
		<category><![CDATA[micron]]></category>
		<category><![CDATA[molecule]]></category>
		<category><![CDATA[morphology]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[protostar]]></category>
		<category><![CDATA[radio jet]]></category>
		<category><![CDATA[radius]]></category>
		<category><![CDATA[resolution observations]]></category>
		<category><![CDATA[resolutions]]></category>
		<category><![CDATA[scales]]></category>
		<category><![CDATA[submillimeter array]]></category>
		<category><![CDATA[submillimeter observations]]></category>
		<category><![CDATA[subtraction]]></category>
		<category><![CDATA[sulfur oxide]]></category>
		<category><![CDATA[very large array]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/resolving-the-circumstellar-disk-around-the-massive-protostar-driving-the-hh-80-81-jet/</guid>
		<description><![CDATA[We present new high-angular resolution observations toward the driving source of the HH 80-81 jet (IRAS 18162-2048). Continuum emission was observed with the Very Large Array at 7 mm and 1.3 cm, and with the Submillimeter Array at 860 microns, with angular resolutions of ~0&#8243;1 and ~0&#8243;8 respectively. Submillimeter observations of the sulfur oxide (SO) [...]]]></description>
			<content:encoded><![CDATA[<p>We present new high-angular resolution observations toward the driving source of the HH 80-81 jet (IRAS 18162-2048). Continuum emission was observed with the Very Large Array at 7 mm and 1.3 cm, and with the Submillimeter Array at 860 microns, with angular resolutions of ~0&#8243;1 and ~0&#8243;8 respectively. Submillimeter observations of the sulfur oxide (SO) molecule are reported as well. At 1.3 cm the emission traces the well-known radio jet, while at 7 mm the continuum morphology is quadrupolar and seems to be produced by a combination of free-free and dust emission. An elongated structure perpendicular to the jet remains in the 7 mm image after subtraction of the free-free contribution. This structure is interpreted as a compact accretion disk of ~200 AU radius. Our interpretation is favored by the presence of rotation in our SO observations observed at larger scales. The observations presented here add to the small list of cases where the hundred-AU scale emission from a circumstellar disk around a massive protostar has been resolved.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/resolving-the-circumstellar-disk-around-the-massive-protostar-driving-the-hh-80-81-jet/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Galaxy And Mass Assembly (GAMA): Galaxy environments and star formation rate variations</title>
		<link>http://voxcharta.org/2012/05/15/galaxy-and-mass-assembly-gama-galaxy-environments-and-star-formation-rate-variations/</link>
		<comments>http://voxcharta.org/2012/05/15/galaxy-and-mass-assembly-gama-galaxy-environments-and-star-formation-rate-variations/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:43:18 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[dependence]]></category>
		<category><![CDATA[environmental effect]]></category>
		<category><![CDATA[environments]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[ewh]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[galaxy population]]></category>
		<category><![CDATA[independent volume]]></category>
		<category><![CDATA[mass and density]]></category>
		<category><![CDATA[morphology]]></category>
		<category><![CDATA[observation]]></category>
		<category><![CDATA[rate variation]]></category>
		<category><![CDATA[relationship]]></category>
		<category><![CDATA[sfr]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[timescale]]></category>
		<category><![CDATA[type star]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/galaxy-and-mass-assembly-gama-galaxy-environments-and-star-formation-rate-variations/</guid>
		<description><![CDATA[We present a detailed investigation into the effects of galaxy environment on their star formation rates (SFR) using galaxies observed in the Galaxy and Mass Assembly Survey (GAMA). We use three independent volume-limited samples of galaxies within z &#60; 0.2 and Mr &#60; -17.8. We investigate the known SFR-density relationship and explore in detail the [...]]]></description>
			<content:encoded><![CDATA[<p>We present a detailed investigation into the effects of galaxy environment on their star formation rates (SFR) using galaxies observed in the Galaxy and Mass Assembly Survey (GAMA). We use three independent volume-limited samples of galaxies within z &lt; 0.2 and Mr &lt; -17.8. We investigate the known SFR-density relationship and explore in detail the dependence of SFR on stellar mass and density. We show that the SFR-density trend is only visible when we include the passive galaxy population along with the star-forming population. This SFR-density relation is absent when we consider only the star-forming population of galaxies, consistent with previous work. While there is a strong dependence of the EWH?a on density we find, as in previous studies, that these trends are largely due to the passive galaxy population and this relationship is absent when considering a &quot;star-forming&quot; sample of galaxies. We find that stellar mass has the strongest influence on SFR and EWH?a with the environment having no significant effect on the star-formation properties of the star forming population. We also show that the SFR-density relationship is absent for both early and late-type star-forming galaxies. We conclude that the stellar mass has the largest impact on the current SFR of a galaxy, and any environmental effect is not detectable. The observation that the trends with density are due to the changing morphology fraction with density implies that the timescales must be very short for any quenching of the SFR in infalling galaxies. Alternatively galaxies may in fact undergo predominantly in-situ evolution where the infall and quenching of galaxies from the field into dense environments is not the dominant evolutionary mode.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/galaxy-and-mass-assembly-gama-galaxy-environments-and-star-formation-rate-variations/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Dark gas in the Solar neighnorhood from extinction data</title>
		<link>http://voxcharta.org/2012/05/15/dark-gas-in-the-solar-neighnorhood-from-extinction-data/</link>
		<comments>http://voxcharta.org/2012/05/15/dark-gas-in-the-solar-neighnorhood-from-extinction-data/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:42:22 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[aquila]]></category>
		<category><![CDATA[atomic gas]]></category>
		<category><![CDATA[cepheus]]></category>
		<category><![CDATA[cm 2]]></category>
		<category><![CDATA[co emission]]></category>
		<category><![CDATA[co measurements]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[conversion factor]]></category>
		<category><![CDATA[density ratio]]></category>
		<category><![CDATA[extinction data]]></category>
		<category><![CDATA[gamma ray data]]></category>
		<category><![CDATA[gas column]]></category>
		<category><![CDATA[linear combination]]></category>
		<category><![CDATA[magellanic cloud]]></category>
		<category><![CDATA[mass fraction]]></category>
		<category><![CDATA[ophiuchus]]></category>
		<category><![CDATA[outer galaxy]]></category>
		<category><![CDATA[solar neighborhood]]></category>
		<category><![CDATA[theoretical model]]></category>
		<category><![CDATA[tracers]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/dark-gas-in-the-solar-neighnorhood-from-extinction-data/</guid>
		<description><![CDATA[When modeling infrared or gamma-ray data as a linear combination of observed gas tracers, an excess of emission has been pointed out with respect to expectations from known neutral and atomic gas as traced by HI and CO measurements respectively. This excess could result from an additional gas component. This gas, called &#8220;dark-gas&#8221; (DG) has [...]]]></description>
			<content:encoded><![CDATA[<p>When modeling infrared or gamma-ray data as a linear combination of observed gas tracers, an excess of emission has been pointed out with respect to expectations from known neutral and atomic gas as traced by HI and CO measurements respectively. This excess could result from an additional gas component. This gas, called &#8220;dark-gas&#8221; (DG) has been observed in our Galaxy, as well as in the Magellanic Clouds. In this paper, we investigate for the first time the correlation between visible extinction (Av) data and the gas tracers on large scales in the solar neighborhood. Our work focuses on the solar neighborhood ($|b|&gt;10\degr$), as well as the inner and outer Galaxy and on four individual regions: Taurus, Orion, Cepheus-Polaris and Aquila-Ophiuchus. Thanks to the recent production of an all-sky Av map, we first perform the correlation between Av and HI and CO emission over the most diffuse regions, to derive the optimal (Av/NH)^(ref) ratio. We then iterate the analysis over the entire regions to estimate the CO-to-H2 conversion factor as well as the DG mass fraction. The average extinction to gas column density ratio in the solar neighborhood is found to be (Av/NH)^(ref)=6.53 10^(-22) mag. cm^2, with significant differences between the inner and outer Galaxy. We derive an average XCO value of 1.67 10^(20) H2 cm^(-2)/(K km s^(-1)). In the solar neighborhood, the gas mass in the dark component is found to be 19% relative to that in the atomic component and 164$%$ relative to the one traced by CO. These results are compatible with the recent analysis using Planck data within the uncertainties of our measurements. We estimate the fraction of dark gas to the total molecular gas to be 0.62 in the solar neighborhood. The HI-to-H2 and H2-to-CO transitions appear for Av $\simeq$0.2 and Av$\simeq1.5$, respectively, in agreement with theoretical models of dark-H2 gas.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/dark-gas-in-the-solar-neighnorhood-from-extinction-data/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>User Guide for the Discrete Dipole Approximation Code DDSCAT 7.2 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/15/user-guide-for-the-discrete-dipole-approximation-code-ddscat-7-2-replacement-2/</link>
		<comments>http://voxcharta.org/2012/05/15/user-guide-for-the-discrete-dipole-approximation-code-ddscat-7-2-replacement-2/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:34:05 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accurate calculation]]></category>
		<category><![CDATA[arbitrary geometry]]></category>
		<category><![CDATA[dipole approximation]]></category>
		<category><![CDATA[dust particle]]></category>
		<category><![CDATA[electromagnetic wave]]></category>
		<category><![CDATA[ellipsoid]]></category>
		<category><![CDATA[field calculations]]></category>
		<category><![CDATA[incident wave]]></category>
		<category><![CDATA[intel math kernel]]></category>
		<category><![CDATA[intel math kernel library]]></category>
		<category><![CDATA[lambda 25]]></category>
		<category><![CDATA[math kernel library]]></category>
		<category><![CDATA[periodic arrays]]></category>
		<category><![CDATA[periodic structure]]></category>
		<category><![CDATA[rectangular solids]]></category>
		<category><![CDATA[rectangular volume]]></category>
		<category><![CDATA[size parameter]]></category>
		<category><![CDATA[target material]]></category>
		<category><![CDATA[target unit]]></category>
		<category><![CDATA[unit cells]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/user-guide-for-the-discrete-dipole-approximation-code-ddscat-7-2-replacement-2/</guid>
		<description><![CDATA[DDSCAT 7.2 is a freely available open-source Fortran-90 software package applying the discrete dipole approximation (DDA) to calculate scattering and absorption of electromagnetic waves by targets with arbitrary geometries and complex refractive index. The targets may be isolated entities (e.g., dust particles), but may also be 1-d or 2-d periodic arrays of &#8220;target unit cells&#8221;, [...]]]></description>
			<content:encoded><![CDATA[<p>DDSCAT 7.2 is a freely available open-source Fortran-90 software package applying the discrete dipole approximation (DDA) to calculate scattering and absorption of electromagnetic waves by targets with arbitrary geometries and complex refractive index. The targets may be isolated entities (e.g., dust particles), but may also be 1-d or 2-d periodic arrays of &#8220;target unit cells&#8221;, which can be used to study absorption, scattering, and electric fields around arrays of nanostructures.   The DDA approximates the target by an array of polarizable points. The theory of the DDA and its implementation in DDSCAT is presented in Draine (1988) and Draine &amp; Flatau (1994), and its extension to periodic structures in Draine &amp; Flatau (2008). Efficient near-field calculations are enabled following Flatau &amp; Draine (2012). DDSCAT 7.2 allows accurate calculations of electromagnetic scattering from targets with size parameters 2*pi*aeff/lambda &lt; 25 provided the refractive index m is not large compared to unity (|m-1| &lt; 2). DDSCAT 7.2 includes support for MPI, OpenMP, and the Intel Math Kernel Library (MKL).   DDSCAT 7.2 supports calculations for a variety of target geometries (e.g., ellipsoids, regular tetrahedra, rectangular solids, finite cylinders, hexagonal prisms, etc.). Target materials may be both inhomogeneous and anisotropic. It is straightforward for the user to import new target geometries into the code. DDSCAT 7.2 calculates total cross sections for absorption and scattering and selected elements of the Mueller scattering intensity matrix for specified orientation of the target relative to the incident wave, and for specified scattering directions. DDSCAT 7.2 calculates E throughout a user-specified rectangular volume containing the target. A Fortran-90 code READNF to read E and P from files created by DDSCAT 7.2 is included in the distribution.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/user-guide-for-the-discrete-dipole-approximation-code-ddscat-7-2-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Protostellar disk formation and transport of angular momentum during magnetized core collapse [Replacement]</title>
		<link>http://voxcharta.org/2012/05/15/protostellar-disk-formation-and-transport-of-angular-momentum-during-magnetized-core-collapse-replacement/</link>
		<comments>http://voxcharta.org/2012/05/15/protostellar-disk-formation-and-transport-of-angular-momentum-during-magnetized-core-collapse-replacement/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:33:17 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[amr]]></category>
		<category><![CDATA[angular momentum]]></category>
		<category><![CDATA[cavity]]></category>
		<category><![CDATA[core collapse]]></category>
		<category><![CDATA[critical value]]></category>
		<category><![CDATA[dense core]]></category>
		<category><![CDATA[disk formation]]></category>
		<category><![CDATA[field intensity]]></category>
		<category><![CDATA[fragmentation]]></category>
		<category><![CDATA[gravitational collapse]]></category>
		<category><![CDATA[initial configuration]]></category>
		<category><![CDATA[initial core]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[mhd simulation]]></category>
		<category><![CDATA[outflow]]></category>
		<category><![CDATA[rotation axis]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[theoretical study]]></category>
		<category><![CDATA[ubiquity]]></category>
		<category><![CDATA[variance]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/protostellar-disk-formation-and-transport-of-angular-momentum-during-magnetized-core-collapse-replacement/</guid>
		<description><![CDATA[Theoretical studies of collapsing clouds have found that even a relatively weak magnetic field (B) may prevent the formation of disks and their fragmentation. However, most previous studies have been limited to cases where B and the rotation axis of the cloud are aligned. We study the transport of angular momentum, and its effects on [...]]]></description>
			<content:encoded><![CDATA[<p>Theoretical studies of collapsing clouds have found that even a relatively weak magnetic field (B) may prevent the formation of disks and their fragmentation. However, most previous studies have been limited to cases where B and the rotation axis of the cloud are aligned. We study the transport of angular momentum, and its effects on disk formation, for non-aligned initial configurations and a range magnetic intensities. We perform 3D AMR MHD simulations of magnetically supercritical collapsing dense cores using the code Ramses. We compute the contributions of the processes transporting angular momentum (J), in the envelope and the region of the disk. We clearly define what could be defined as centrifugally supported disks and study their properties. At variance with earlier analyses, we show that the transport of J acts less efficiently in collapsing cores with non-aligned rotation axis and B. Analytically, this result can be understood by taking into account the bending of field lines occurring during the gravitational collapse. For the transport of J, we conclude that magnetic braking in the mean direction of B tends to dominate over both the gravitational and outflow transport of J. We find that massive disks, containing at least 10% of the initial core mass, can form during the earliest stages of star formation even for mass-to-flux ratios as small as 3 to 5 times the critical value. At higher field intensities, the early formation of massive disks is prevented. Given the ubiquity of Class I disks, and because the early formation of massive disks can take place at moderate magnetic intensities, we speculate that for stronger fields, disks will form later, when most of the envelope will have been accreted. In addition, we speculate that some observed early massive disks may actually be outflow cavities, mistaken for disks by projection effects. (Abridged version of the abstract.)</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/protostellar-disk-formation-and-transport-of-angular-momentum-during-magnetized-core-collapse-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>The velocity dispersion and mass function of the outer halo globular cluster Palomar 4</title>
		<link>http://voxcharta.org/2012/05/14/the-velocity-dispersion-and-mass-function-of-the-outer-halo-globular-cluster-palomar-4/</link>
		<comments>http://voxcharta.org/2012/05/14/the-velocity-dispersion-and-mass-function-of-the-outer-halo-globular-cluster-palomar-4/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:55:08 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[broad band]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[hst wfpc2]]></category>
		<category><![CDATA[keck ii telescope]]></category>
		<category><![CDATA[line of sight]]></category>
		<category><![CDATA[lris]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[mass function]]></category>
		<category><![CDATA[mass range]]></category>
		<category><![CDATA[member stars]]></category>
		<category><![CDATA[outer halo]]></category>
		<category><![CDATA[palomar]]></category>
		<category><![CDATA[precise line]]></category>
		<category><![CDATA[radial velocity]]></category>
		<category><![CDATA[resolution imaging]]></category>
		<category><![CDATA[spectrograph]]></category>
		<category><![CDATA[spectrometer]]></category>
		<category><![CDATA[surface brightness]]></category>
		<category><![CDATA[velocity dispersion]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/the-velocity-dispersion-and-mass-function-of-the-outer-halo-globular-cluster-palomar-4/</guid>
		<description><![CDATA[We obtained precise line-of-sight radial velocities of 23 member stars of the remote halo globular cluster Palomar 4 (Pal 4) using the High Resolution Echelle Spectrograph (HIRES) at the Keck I telescope. We also measured the mass function of the cluster down to a limiting magnitude of V~28 mag using archival HST/WFPC2 imaging. We derived [...]]]></description>
			<content:encoded><![CDATA[<p>We obtained precise line-of-sight radial velocities of 23 member stars of the remote halo globular cluster Palomar 4 (Pal 4) using the High Resolution Echelle Spectrograph (HIRES) at the Keck I telescope. We also measured the mass function of the cluster down to a limiting magnitude of V~28 mag using archival HST/WFPC2 imaging. We derived the cluster&#8217;s surface brightness profile based on the WFPC2 data and on broad-band imaging with the Low-Resolution Imaging Spectrometer (LRIS) at the Keck II telescope. We find a mean cluster velocity of 72.55+/-0.22 km/s and a velocity dispersion of 0.87+/-0.18 km/s. The global mass function of the cluster, in the mass range 0.55&lt;=M&lt;=0.85 M_solar, is shallower than a Kroupa mass function and the cluster is significantly depleted in low-mass stars in its center compared to its outskirts. Since the relaxation time of Pal 4 is of the order of a Hubble time, this points to primordial mass segregation in this cluster. Extrapolating the measured mass function towards lower-mass stars and including the contribution of compact remnants, we derive a total cluster mass of 29800 M_solar. For this mass, the measured velocity dispersion is consistent with the expectations of Newtonian dynamics and below the prediction of Modified Newtonian Dynamics (MOND). Pal 4 adds to the growing body of evidence that the dynamics of star clusters in the outer Galactic halo can hardly be explained by MOND.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/the-velocity-dispersion-and-mass-function-of-the-outer-halo-globular-cluster-palomar-4/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>A wide-area view of the Phoenix dwarf galaxy from VLT/FORS imaging</title>
		<link>http://voxcharta.org/2012/05/14/a-wide-area-view-of-the-phoenix-dwarf-galaxy-from-vltfors-imaging/</link>
		<comments>http://voxcharta.org/2012/05/14/a-wide-area-view-of-the-phoenix-dwarf-galaxy-from-vltfors-imaging/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:53:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[center of the galaxy]]></category>
		<category><![CDATA[colour magnitude diagram]]></category>
		<category><![CDATA[density profile]]></category>
		<category><![CDATA[dwarf galaxy]]></category>
		<category><![CDATA[dwarf irregulars]]></category>
		<category><![CDATA[dwarf spheroidals]]></category>
		<category><![CDATA[galaxy one]]></category>
		<category><![CDATA[giant branch]]></category>
		<category><![CDATA[gyr]]></category>
		<category><![CDATA[horizontal branch]]></category>
		<category><![CDATA[luminosity function]]></category>
		<category><![CDATA[number density]]></category>
		<category><![CDATA[optical center]]></category>
		<category><![CDATA[photometry]]></category>
		<category><![CDATA[spatial distribution]]></category>
		<category><![CDATA[spatial variation]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[type galaxy]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/a-wide-area-view-of-the-phoenix-dwarf-galaxy-from-vltfors-imaging/</guid>
		<description><![CDATA[We present results from a wide-area photometric survey of the Phoenix dwarf galaxy, one of the rare dwarf irregular/ dwarf spheroidal transition type galaxies (dTs) of the Local Group (LG). These objects offer the opportunity to study the existence of possible evolutionary links between the late- and early- type LG dwarf galaxies, since the properties [...]]]></description>
			<content:encoded><![CDATA[<p>We present results from a wide-area photometric survey of the Phoenix dwarf galaxy, one of the rare dwarf irregular/ dwarf spheroidal transition type galaxies (dTs) of the Local Group (LG). These objects offer the opportunity to study the existence of possible evolutionary links between the late- and early- type LG dwarf galaxies, since the properties of dTs suggest that they may be dwarf irregulars in the process of transforming into dwarf spheroidals. Using FORS at the VLT we have acquired VI photometry of Phoenix. The data reach a S/N~10 just below the horizontal branch of the system and consist of a mosaic of images that covers an area of 26&#8242; x 26&#8242; centered on the coordinates of the optical center of the galaxy. Examination of the colour-magnitude diagram and luminosity function revealed the presence of a bump above the red clump, consistent with being a red giant branch bump. The deep photometry combined with the large area covered allows us to put on a secure ground the determination of the overall structural properties of the galaxy and to derive the spatial distribution of stars in different evolutionary phases and age ranges, from 0.1 Gyr to the oldest stars. The best-fitting profile to the overall stellar population is a Sersic profile of Sersic radius R_S = 1.82&#8242;+-0.06&#8242; and m=0.83+-0.03. We confirm that the spatial distribution of stars is found to become more and more centrally concentrated the younger the stellar population, as reported in previous studies. This is similar to the stellar population gradients found for close-by Milky Way dwarf spheroidal galaxies. We quantify such spatial variations by analyzing the surface number density profiles of stellar populations in different age ranges; [Abridged]</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/a-wide-area-view-of-the-phoenix-dwarf-galaxy-from-vltfors-imaging/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Formation of Galactic Pseudo-bulges via Gas Rich Major Mergers</title>
		<link>http://voxcharta.org/2012/05/14/formation-of-galactic-pseudo-bulges-via-gas-rich-major-mergers/</link>
		<comments>http://voxcharta.org/2012/05/14/formation-of-galactic-pseudo-bulges-via-gas-rich-major-mergers/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:51:23 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bulge]]></category>
		<category><![CDATA[coalescence process]]></category>
		<category><![CDATA[disk galaxy]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[giant disk]]></category>
		<category><![CDATA[mass resolution]]></category>
		<category><![CDATA[merger]]></category>
		<category><![CDATA[numerical simulation]]></category>
		<category><![CDATA[remnant]]></category>
		<category><![CDATA[rotation]]></category>
		<category><![CDATA[stellar component]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/formation-of-galactic-pseudo-bulges-via-gas-rich-major-mergers/</guid>
		<description><![CDATA[It is widely accepted that within the framework of LCDM a significant fraction of giant-disk galaxies has recently experienced a violent galactic merger. We present numerical simulations of such major mergers of gas-rich pure disk galaxies, and focus on the innermost stellar component (bulge) of the disk remnants. The simulations have high spatial and mass [...]]]></description>
			<content:encoded><![CDATA[<p>It is widely accepted that within the framework of LCDM a significant fraction of giant-disk galaxies has recently experienced a violent galactic merger. We present numerical simulations of such major mergers of gas-rich pure disk galaxies, and focus on the innermost stellar component (bulge) of the disk remnants. The simulations have high spatial and mass resolutions, and resolve regions deep enough to allow bulge classification according to standard kinematical and structural characteristics. In agreement with recent studies we find that these bulges are dominated by stars formed in the final coalescence process. In contrast to the common interpretation of such components as classical bulges (i.e. similar to intermediate luminosity ellipticals), we find they are supported by highly coherent rotations and have Sersic indices n&lt;2, a result leading to their classification as pseudo-bulges. Pseudo-bulge formation by gas rich major mergers of pure disks is a novel mode of pseudo-bulge formation; It complements pseudo-bulge growth by secular evolution, and it could help explain the high fractions of classically bulge-less giant disk galaxies, and pseudo-bulges found in giant Sc galaxies.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>An HST Imaging Survey of Low-Mass Stars in the Chamaeleon I Star Forming region</title>
		<link>http://voxcharta.org/2012/05/14/an-hst-imaging-survey-of-low-mass-stars-in-the-chamaeleon-i-star-forming-region/</link>
		<comments>http://voxcharta.org/2012/05/14/an-hst-imaging-survey-of-low-mass-stars-in-the-chamaeleon-i-star-forming-region/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:51:04 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion rates]]></category>
		<category><![CDATA[alpha 2]]></category>
		<category><![CDATA[chamaeleon]]></category>
		<category><![CDATA[disk parameters]]></category>
		<category><![CDATA[fitting tool]]></category>
		<category><![CDATA[hst imaging]]></category>
		<category><![CDATA[mass loss]]></category>
		<category><![CDATA[mass star]]></category>
		<category><![CDATA[mm data]]></category>
		<category><![CDATA[narrow band filters]]></category>
		<category><![CDATA[optical data]]></category>
		<category><![CDATA[outlier]]></category>
		<category><![CDATA[photometry]]></category>
		<category><![CDATA[region images]]></category>
		<category><![CDATA[spectral energy distribution]]></category>
		<category><![CDATA[spectral index]]></category>
		<category><![CDATA[t tauri]]></category>
		<category><![CDATA[tauri stars]]></category>
		<category><![CDATA[v band]]></category>
		<category><![CDATA[wfpc2 observations]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/an-hst-imaging-survey-of-low-mass-stars-in-the-chamaeleon-i-star-forming-region/</guid>
		<description><![CDATA[We present new HST/WFPC2 observations of 20 fields centered around T Tauri stars in the Chamaeleon I star forming region. Images have been obtained in the F631N ([OI]6300A), F656N (Ha) and F673N ([SII]6716A+6731A) narrow-band filters, plus the Johnson V-band equivalent F547M filter. We detect 31 T Tauri stars falling within our fields. We discuss the [...]]]></description>
			<content:encoded><![CDATA[<p>We present new HST/WFPC2 observations of 20 fields centered around T Tauri stars in the Chamaeleon I star forming region. Images have been obtained in the F631N ([OI]6300A), F656N (Ha) and F673N ([SII]6716A+6731A) narrow-band filters, plus the Johnson V-band equivalent F547M filter. We detect 31 T Tauri stars falling within our fields. We discuss the optical morphology of 10 sources showing evidence of either binarity, circumstellar material, or mass loss. We supplement our photometry with a compilation of optical, infrared and sub-millimeter data from the literature, together with new sub-mm data for three objects, to build the Spectral Energy Distributions (SED) of 19 single sources. Using an SED model fitting tool, we self-consistently estimate a number of stellar and disk parameters, while mass accretion rates are directly derived from our Ha photometry. We find that bolometric luminosities derived from dereddened optical data tend to be underestimated in systems with high alpha(2-24} IR spectral index, suggesting that disks seen nearly edge-on may occasionally be interpreted as low luminosity (and therefore more evolved) sources. On the other hand, the same alpha(2-24) spectral index, a tracer of the amount of dust in the warmer layers of the circumstellar disks, and the mass accretion rate appear to decay with the isocronal stellar age, suggesting that the observed age spread (~0.5-5 Myr) within the cluster is real. Our sample contains a few outliers that may have dissipated their circumstellar disks on shorter time-scale.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/an-hst-imaging-survey-of-low-mass-stars-in-the-chamaeleon-i-star-forming-region/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Astrophysical and Structural Parameters of the Open Clusters NGC 6866, NGC 7062, and NGC 2360</title>
		<link>http://voxcharta.org/2012/05/14/astrophysical-and-structural-parameters-of-the-open-clusters-ngc-6866-ngc-7062-and-ngc-2360/</link>
		<comments>http://voxcharta.org/2012/05/14/astrophysical-and-structural-parameters-of-the-open-clusters-ngc-6866-ngc-7062-and-ngc-2360/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:48:27 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[beta]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[cluster member]]></category>
		<category><![CDATA[density profile]]></category>
		<category><![CDATA[field star]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[giant molecular cloud]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[longevity]]></category>
		<category><![CDATA[mass function]]></category>
		<category><![CDATA[msun]]></category>
		<category><![CDATA[NGC]]></category>
		<category><![CDATA[open cluster]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[probability]]></category>
		<category><![CDATA[quadrant]]></category>
		<category><![CDATA[radii]]></category>
		<category><![CDATA[slope]]></category>
		<category><![CDATA[ubv]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/astrophysical-and-structural-parameters-of-the-open-clusters-ngc-6866-ngc-7062-and-ngc-2360/</guid>
		<description><![CDATA[We derive astrophysical and structural parameters of the poorly studied open clusters NGC 6866, NGC 7062, and NGC 2360 based on filtered 2MASS (J, J -H) diagrams, and stellar radial density profiles. The field star decontamination technique is utilised for selecting high-probability cluster members. The E(B -V) reddening values of the three clusters derived from [...]]]></description>
			<content:encoded><![CDATA[<p>We derive astrophysical and structural parameters of the poorly studied open clusters NGC 6866, NGC 7062, and NGC 2360 based on filtered 2MASS (J, J -H) diagrams, and stellar radial density profiles. The field star decontamination technique is utilised for selecting high-probability cluster members. The E(B -V) reddening values of the three clusters derived from 2MASS JHKs agree with those inferred from UBV and uvby-{\beta} photometries. We find that the core mass function slopes are flatter than the halo&#8217;s for the three clusters. The large core and cluster radii of NGC 6866 and NGC 2360 indicate an expanded core, which may suggest the presence of stellar mass black-holes. NGC 2360 is located in the third quadrant (l = 229.80), where Giant Molecular Clouds are scarce that, together with its relatively large mass (~ 1800 msun), might explain its longevity(~ 1.8Gyr) in the Galaxy.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/astrophysical-and-structural-parameters-of-the-open-clusters-ngc-6866-ngc-7062-and-ngc-2360/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Formation of Stellar Cusps in Galactic Nuclei</title>
		<link>http://voxcharta.org/2012/05/14/the-formation-of-stellar-cusps-in-galactic-nuclei/</link>
		<comments>http://voxcharta.org/2012/05/14/the-formation-of-stellar-cusps-in-galactic-nuclei/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:47:35 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cusp]]></category>
		<category><![CDATA[disruption]]></category>
		<category><![CDATA[dynamical evolution]]></category>
		<category><![CDATA[galactic center]]></category>
		<category><![CDATA[galactic nuclei]]></category>
		<category><![CDATA[galactic nucleus]]></category>
		<category><![CDATA[massive black hole]]></category>
		<category><![CDATA[mechanisms]]></category>
		<category><![CDATA[observational signature]]></category>
		<category><![CDATA[planck]]></category>
		<category><![CDATA[segregation]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[stellar cluster]]></category>
		<category><![CDATA[stellar collisions]]></category>
		<category><![CDATA[stellar evolution]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/the-formation-of-stellar-cusps-in-galactic-nuclei/</guid>
		<description><![CDATA[The dynamics of galactic nuclei can be affected by several mechanisms. Among these are stellar evolution, stellar collisions, mass segregation, and tidal disruptions of stars due to the central black hole. In this presentation I will address how each of these affects the stellar cusp and the resulting observational signatures. Using a set of dynamically [...]]]></description>
			<content:encoded><![CDATA[<p>The dynamics of galactic nuclei can be affected by several mechanisms. Among these are stellar evolution, stellar collisions, mass segregation, and tidal disruptions of stars due to the central black hole. In this presentation I will address how each of these affects the stellar cusp and the resulting observational signatures. Using a set of dynamically evolving Fokker-Planck simulations I present the dynamical evolution a nuclear stellar cluster and the growth of the central massive black hole within the Galactic Nucleus. In addition to the Galactic Center I explore a wide variety of galactic nuclei and their resulting stellar cusps.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/the-formation-of-stellar-cusps-in-galactic-nuclei/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A Near-Infrared Survey of the Inner Galactic Plane for Wolf-Rayet Stars II. Going Fainter: 72 More New WR Stars [Replacement]</title>
		<link>http://voxcharta.org/2012/05/14/a-near-infrared-survey-of-the-inner-galactic-plane-for-wolf-rayet-stars-ii-going-fainter-72-more-new-wr-stars-replacement/</link>
		<comments>http://voxcharta.org/2012/05/14/a-near-infrared-survey-of-the-inner-galactic-plane-for-wolf-rayet-stars-ii-going-fainter-72-more-new-wr-stars-replacement/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:36:48 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[band spectra]]></category>
		<category><![CDATA[distant spiral]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[few degrees]]></category>
		<category><![CDATA[follow ups]]></category>
		<category><![CDATA[galactic center]]></category>
		<category><![CDATA[galactic longitude]]></category>
		<category><![CDATA[galactic plane]]></category>
		<category><![CDATA[image analysis]]></category>
		<category><![CDATA[infrared survey]]></category>
		<category><![CDATA[k band]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[narrow band imaging]]></category>
		<category><![CDATA[spectroscopic parallax]]></category>
		<category><![CDATA[spiral arm]]></category>
		<category><![CDATA[square degree]]></category>
		<category><![CDATA[star candidates]]></category>
		<category><![CDATA[ups]]></category>
		<category><![CDATA[wr stars]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/a-near-infrared-survey-of-the-inner-galactic-plane-for-wolf-rayet-stars-ii-going-fainter-72-more-new-wr-stars-replacement/</guid>
		<description><![CDATA[We are continuing a J, K and narrow-band imaging survey of 300 square degrees of the plane of the Galaxy, searching for new Wolf-Rayet stars. Our survey spans 150 degrees in Galactic longitude and reaches 1 degree above and below the Galactic plane. The survey has a useful limiting magnitude of K = 15 over [...]]]></description>
			<content:encoded><![CDATA[<p>We are continuing a J, K and narrow-band imaging survey of 300 square degrees of the plane of the Galaxy, searching for new Wolf-Rayet stars. Our survey spans 150 degrees in Galactic longitude and reaches 1 degree above and below the Galactic plane. The survey has a useful limiting magnitude of K = 15 over most of the observed Galactic plane, and K = 14 (due to severe crowding) within a few degrees of the Galactic center. Thousands of emission line candidates have been detected. In spectrographic follow-ups of 146 relatively bright WR star candidates we have re-examined 11 previously known WC and WN stars and discovered 72 new WR stars, 17 of type WN and 55 of type WC. Our latest image analysis pipeline now picks out WR stars with a 57% success rate. Star subtype assignments have been confirmed with K band spectra, and distances approximated using the method of spectroscopic parallax. Some of the new WR stars are amongst the most distant known in our Galaxy. The distribution of these new WR stars is beginning to trace the locations of massive stars along the distant spiral arms of the Milky Way.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/a-near-infrared-survey-of-the-inner-galactic-plane-for-wolf-rayet-stars-ii-going-fainter-72-more-new-wr-stars-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>MaGICC Disks: Matching Observed Galaxy Relationships Over a Wide Stellar Mass Range [Replacement]</title>
		<link>http://voxcharta.org/2012/05/14/magicc-disks-matching-observed-galaxy-relationships-over-a-wide-stellar-mass-range-replacement-2/</link>
		<comments>http://voxcharta.org/2012/05/14/magicc-disks-matching-observed-galaxy-relationships-over-a-wide-stellar-mass-range-replacement-2/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:35:16 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorption line]]></category>
		<category><![CDATA[baryonic]]></category>
		<category><![CDATA[core]]></category>
		<category><![CDATA[cosmological context]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[dependence]]></category>
		<category><![CDATA[disc galaxies]]></category>
		<category><![CDATA[galaxy properties]]></category>
		<category><![CDATA[interplay]]></category>
		<category><![CDATA[key role]]></category>
		<category><![CDATA[large scale]]></category>
		<category><![CDATA[mass range]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[physical model]]></category>
		<category><![CDATA[rotation curves]]></category>
		<category><![CDATA[rotation velocity]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[surface brightness]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/magicc-disks-matching-observed-galaxy-relationships-over-a-wide-stellar-mass-range-replacement-2/</guid>
		<description><![CDATA[We use the same physical model to simulate four galaxies that match the relation between stellar and total mass, over a mass range that includes the vast majority of disc galaxies. The resultant galaxies, part of the Making Galaxies in a Cosmological Context (MaGICC) program, also match observed relations between luminosity, rotation velocity, size, colour, [...]]]></description>
			<content:encoded><![CDATA[<p>We use the same physical model to simulate four galaxies that match the relation between stellar and total mass, over a mass range that includes the vast majority of disc galaxies. The resultant galaxies, part of the Making Galaxies in a Cosmological Context (MaGICC) program, also match observed relations between luminosity, rotation velocity, size, colour, star formation rate, HI mass, baryonic mass, and metallicity. Radiation from massive stars and supernova energy regulate star formation and drive outflows, balancing the complex interplay between cooling gas, star formation, large scale outflows, and recycling of gas in a manner which correctly scales with the mass of the galaxy. Outflows also play a key role in simulating galaxies with exponential surface brightness profiles, flat rotation curves and dark matter cores. Our study implies that large scale outflows are the primary driver of the dependence of disc galaxy properties on mass. We show that the amount of outflows invoked in our model is required to meet the constraints provided by observations of OVI absorption lines in the circum-galactic-media of local galaxies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/magicc-disks-matching-observed-galaxy-relationships-over-a-wide-stellar-mass-range-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Initial data release of the Kepler-INT Survey [Replacement]</title>
		<link>http://voxcharta.org/2012/05/14/initial-data-release-of-the-kepler-int-survey-replacement/</link>
		<comments>http://voxcharta.org/2012/05/14/initial-data-release-of-the-kepler-int-survey-replacement/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:34:20 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[broadband filters]]></category>
		<category><![CDATA[enormous impact]]></category>
		<category><![CDATA[first data]]></category>
		<category><![CDATA[galactic plane]]></category>
		<category><![CDATA[initial data]]></category>
		<category><![CDATA[intensive search]]></category>
		<category><![CDATA[isaac newton]]></category>
		<category><![CDATA[isaac newton telescope]]></category>
		<category><![CDATA[island of la palma]]></category>
		<category><![CDATA[kepler mission]]></category>
		<category><![CDATA[kic]]></category>
		<category><![CDATA[la palma]]></category>
		<category><![CDATA[optical survey]]></category>
		<category><![CDATA[photometric calibration]]></category>
		<category><![CDATA[photometry]]></category>
		<category><![CDATA[release concerns]]></category>
		<category><![CDATA[stellar variability]]></category>
		<category><![CDATA[target]]></category>
		<category><![CDATA[transiting planet]]></category>
		<category><![CDATA[vega system]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/initial-data-release-of-the-kepler-int-survey-replacement/</guid>
		<description><![CDATA[This paper describes the first data release of the Kepler-INT Survey (KIS), that covers a 116 deg2 region of the Cygnus and Lyra constellations. The Kepler field is the target of the most intensive search for transiting planets to date. Despite the fact that the Kepler mission provides superior time series photometry, with an enormous [...]]]></description>
			<content:encoded><![CDATA[<p>This paper describes the first data release of the Kepler-INT Survey (KIS), that covers a 116 deg2 region of the Cygnus and Lyra constellations. The Kepler field is the target of the most intensive search for transiting planets to date. Despite the fact that the Kepler mission provides superior time series photometry, with an enormous impact on all areas of stellar variability, its field lacks optical photometry complete to the confusion limit of the Kepler instrument necessary for selecting various classes of targets. For this reason, we follow the observing strategy and data reduction method used in the IPHAS and UVEX galactic plane surveys in order to produce a deep optical survey of the Kepler field. This initial release concerns data taken between May and August 2011, using the Isaac Newton Telescope on the island of La Palma. Four broadband filters were used, U, g, r, i, as well as one narrowband one, Halpha, reaching down to a 10-sigma limit of around 20th mag in the Vega system. Observations covering around 50 deg2, thus about half of the field, passed our quality control thresholds and constitute this first data release. We derive a global photometric calibration by placing the KIS magnitudes as close as possible to the Kepler Input Catalog (KIC) photometry. The initial data release catalogue containing around 6 million sources from all the good photometric fields is available for download from the KIS webpage, as well as via MAST.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/initial-data-release-of-the-kepler-int-survey-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Structure of dynamical condensation fronts in the interstellar medium [Replacement]</title>
		<link>http://voxcharta.org/2012/05/14/structure-of-dynamical-condensation-fronts-in-the-interstellar-medium-replacement/</link>
		<comments>http://voxcharta.org/2012/05/14/structure-of-dynamical-condensation-fronts-in-the-interstellar-medium-replacement/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:33:46 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cloud formation]]></category>
		<category><![CDATA[cnm]]></category>
		<category><![CDATA[condensation]]></category>
		<category><![CDATA[diffuse gas]]></category>
		<category><![CDATA[geometry]]></category>
		<category><![CDATA[heat conduction]]></category>
		<category><![CDATA[interstellar medium]]></category>
		<category><![CDATA[mass flux]]></category>
		<category><![CDATA[molecular cloud]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[remarkable property]]></category>
		<category><![CDATA[shock]]></category>
		<category><![CDATA[thermal equilibrium]]></category>
		<category><![CDATA[transition]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/structure-of-dynamical-condensation-fronts-in-the-interstellar-medium-replacement/</guid>
		<description><![CDATA[In this paper, we investigate the structure of condensation fronts from warm diffuse gas to cold neutral medium (CNM) under the plane parallel geometry. The solutions have two parameters, the pressure of the CNM and the mass flux across the transition front, and their ranges are much wider than previously thought. First, we consider the [...]]]></description>
			<content:encoded><![CDATA[<p>In this paper, we investigate the structure of condensation fronts from warm diffuse gas to cold neutral medium (CNM) under the plane parallel geometry. The solutions have two parameters, the pressure of the CNM and the mass flux across the transition front, and their ranges are much wider than previously thought. First, we consider the pressure range where the three phases, the CNM, the unstable phase, and the warm neutral medium, can coexist in the pressure equilibrium. In a wide range of the mass flux, we find solutions connecting the CNM and the unstable phase. Moreover, we find solutions in larger pressure range where there is only one thermal equilibrium state or the CNM. These solutions can be realized in shock-compressed regions that are promising sites of molecular cloud formation. We also find remarkable properties in our solutions. Heat conduction becomes less important with increasing mass flux, and the thickness of the transition layer is characterized by the cooling length instead of the Field length.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/structure-of-dynamical-condensation-fronts-in-the-interstellar-medium-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Radiative and Momentum Based Mechanical AGN Feedback in a 3-Dimensional Galaxy Evolution Code [Replacement]</title>
		<link>http://voxcharta.org/2012/05/14/radiative-and-momentum-based-mechanical-agn-feedback-in-a-3-dimensional-galaxy-evolution-code-replacement/</link>
		<comments>http://voxcharta.org/2012/05/14/radiative-and-momentum-based-mechanical-agn-feedback-in-a-3-dimensional-galaxy-evolution-code-replacement/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:32:37 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[analytic results]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[bondi]]></category>
		<category><![CDATA[di matteo]]></category>
		<category><![CDATA[feedback model]]></category>
		<category><![CDATA[fluctuation]]></category>
		<category><![CDATA[galaxy evolution]]></category>
		<category><![CDATA[host galaxy]]></category>
		<category><![CDATA[isolated galaxies]]></category>
		<category><![CDATA[mechanical energy]]></category>
		<category><![CDATA[new model]]></category>
		<category><![CDATA[radiative]]></category>
		<category><![CDATA[ray radiation]]></category>
		<category><![CDATA[sph simulation]]></category>
		<category><![CDATA[thermal feedback]]></category>
		<category><![CDATA[wind velocity]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/radiative-and-momentum-based-mechanical-agn-feedback-in-a-3-dimensional-galaxy-evolution-code-replacement/</guid>
		<description><![CDATA[We study the growth of black holes (BHs) in galaxies using three-dimensional smoothed particle hydrodynamic (SPH) simulations with new implementations of the momentum mechanical feedback, and restriction of accreted elements to those that are gravitationally bound to the BH. We also include the feedback from the X-ray radiation emitted by the black hole, which heats [...]]]></description>
			<content:encoded><![CDATA[<p>We study the growth of black holes (BHs) in galaxies using three-dimensional smoothed particle hydrodynamic (SPH) simulations with new implementations of the momentum mechanical feedback, and restriction of accreted elements to those that are gravitationally bound to the BH. We also include the feedback from the X-ray radiation emitted by the black hole, which heats the surrounding gas in the host galaxies, and adds radial momentum to the fluid. We perform simulations of isolated galaxies and merging galaxies and test various feedback models with the new treatment of the Bondi radius criterion. We find that overall the black hole growth is similar to what has been obtained by earlier workers using the Springel, Di Matteo, &amp; Hernquist algorithms. However, the outflowing wind velocities and mechanical energy emitted by winds are considerably higher (v_w ~ 1000-3000 km/s) compared to the standard thermal feedback model (v_w ~ 50-100 km/s). While the thermal feedback model emits only 0.1 % of BH released energy in winds, the momentum feedback model emits more than 30 % of the total energy released by the BH in winds. In the momentum feedback model, the degree of fluctuation in both radiant and wind output is considerably larger than in the standard treatments. We check that the new model of the BH mass accretion agrees with analytic results for the standard Bondi problem.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/radiative-and-momentum-based-mechanical-agn-feedback-in-a-3-dimensional-galaxy-evolution-code-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>High-Velocity Outflows Without AGN Feedback: Eddington-Limited Star Formation in Compact Massive Galaxies</title>
		<link>http://voxcharta.org/2012/05/13/high-velocity-outflows-without-agn-feedback-eddington-limited-star-formation-in-compact-massive-galaxies/</link>
		<comments>http://voxcharta.org/2012/05/13/high-velocity-outflows-without-agn-feedback-eddington-limited-star-formation-in-compact-massive-galaxies/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:55:25 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[dust grains]]></category>
		<category><![CDATA[eddington limit]]></category>
		<category><![CDATA[galactic nucleus]]></category>
		<category><![CDATA[high velocity]]></category>
		<category><![CDATA[hubble space telescope]]></category>
		<category><![CDATA[infrared photometry]]></category>
		<category><![CDATA[infrared survey]]></category>
		<category><![CDATA[massive galaxy]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[msun]]></category>
		<category><![CDATA[radiation pressure]]></category>
		<category><![CDATA[sfr]]></category>
		<category><![CDATA[sigma]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[starburst]]></category>
		<category><![CDATA[stellar wind]]></category>
		<category><![CDATA[supernovae]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/high-velocity-outflows-without-agn-feedback-eddington-limited-star-formation-in-compact-massive-galaxies/</guid>
		<description><![CDATA[We present the discovery of compact, obscured star formation in galaxies at z 0.6 that exhibit &#62;1000 km/s outflows. Using optical morphologies from the Hubble Space Telescope and infrared photometry from the Wide-field Infrared Survey Explorer, we estimate star formation rate (SFR) surface densities that approach Sigma_SFR 3000 Msun/yr/kpc^2, comparable to the Eddington limit from [...]]]></description>
			<content:encoded><![CDATA[<p>We present the discovery of compact, obscured star formation in galaxies at z 0.6 that exhibit &gt;1000 km/s outflows. Using optical morphologies from the Hubble Space Telescope and infrared photometry from the Wide-field Infrared Survey Explorer, we estimate star formation rate (SFR) surface densities that approach Sigma_SFR 3000 Msun/yr/kpc^2, comparable to the Eddington limit from radiation pressure on dust grains. We argue that feedback associated with a compact starburst in the form of radiation pressure from massive stars and ram pressure from supernovae and stellar winds is sufficient to produce the high-velocity outflows we observe, without the need to invoke feedback from an active galactic nucleus.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/high-velocity-outflows-without-agn-feedback-eddington-limited-star-formation-in-compact-massive-galaxies/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Origin of the Virgo Stellar Substructure</title>
		<link>http://voxcharta.org/2012/05/13/the-origin-of-the-virgo-stellar-substructure/</link>
		<comments>http://voxcharta.org/2012/05/13/the-origin-of-the-virgo-stellar-substructure/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:54:10 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[body simulation]]></category>
		<category><![CDATA[delta mu delta]]></category>
		<category><![CDATA[dimensional space]]></category>
		<category><![CDATA[dwarf galaxy]]></category>
		<category><![CDATA[galactic center]]></category>
		<category><![CDATA[gsr]]></category>
		<category><![CDATA[locus]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[pisces]]></category>
		<category><![CDATA[progenitor]]></category>
		<category><![CDATA[proper motion]]></category>
		<category><![CDATA[radial velocity]]></category>
		<category><![CDATA[remnant]]></category>
		<category><![CDATA[segue 1]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[substructure]]></category>
		<category><![CDATA[tidal debris]]></category>
		<category><![CDATA[tidal disruption]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/the-origin-of-the-virgo-stellar-substructure/</guid>
		<description><![CDATA[We present three-dimensional space velocities of stars selected to be consistent with membership in the Virgo stellar substructure. Candidates were selected from SA 103, a single 40&#215;40 arcmin field from our proper motion (PM) survey in Kapteyn&#8217;s Selected Areas (SAs), based on the PMs, SDSS photometry, and follow-up spectroscopy of 215 stars. The signature of [...]]]></description>
			<content:encoded><![CDATA[<p>We present three-dimensional space velocities of stars selected to be consistent with membership in the Virgo stellar substructure. Candidates were selected from SA 103, a single 40&#215;40 arcmin field from our proper motion (PM) survey in Kapteyn&#8217;s Selected Areas (SAs), based on the PMs, SDSS photometry, and follow-up spectroscopy of 215 stars. The signature of the Virgo substructure is clear in the SDSS color-magnitude diagram (CMD) centered on SA 103, and 16 stars are identified that have high Galactocentric-frame radial velocities (V_GSR &gt; 50 km/s) and lie near the CMD locus of Virgo. The implied distance to the Virgo substructure from the candidates is 14+/-3 kpc. We derive mean kinematics from these 16 stars, finding a radial velocity V_GSR = 153+/-22 km/s and proper motions (mu_alpha*cos(delta), mu_delta) = (-5.24, -0.91)+/-(0.43, 0.46) mas/yr. From the mean kinematics of these members, we determine that the Virgo progenitor was on an eccentric (e ~ 0.8) orbit that recently passed near the Galactic center (pericentric distance R_p ~ 6 kpc). This destructive orbit is consistent with the idea that the substructure(s) in Virgo originated in the tidal disruption of a Milky Way satellite. N-body simulations suggest that the entire cloud-like Virgo substructure (encompassing the &#8220;Virgo Overdensity&#8221; and the &#8220;Virgo Stellar Stream&#8221;) is likely the tidal debris remnant from a recently-disrupted massive (~10^9 M_sun) dwarf galaxy. The model also suggests that some other known stellar overdensities in the Milky Way halo (e.g., the Pisces Overdensity and debris near NGC 2419 and SEGUE 1) are explained by the disruption of the Virgo progenitor.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/the-origin-of-the-virgo-stellar-substructure/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Residual Cooling and Persistent Star Formation amid AGN Feedback in Abell 2597</title>
		<link>http://voxcharta.org/2012/05/13/residual-cooling-and-persistent-star-formation-amid-agn-feedback-in-abell-2597/</link>
		<comments>http://voxcharta.org/2012/05/13/residual-cooling-and-persistent-star-formation-amid-agn-feedback-in-abell-2597/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:53:54 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abell]]></category>
		<category><![CDATA[bcg]]></category>
		<category><![CDATA[chandra observation]]></category>
		<category><![CDATA[chandra x ray]]></category>
		<category><![CDATA[cluster galaxy]]></category>
		<category><![CDATA[cold dust]]></category>
		<category><![CDATA[cold gas]]></category>
		<category><![CDATA[cooling flow]]></category>
		<category><![CDATA[dominant contributor]]></category>
		<category><![CDATA[filament]]></category>
		<category><![CDATA[fuv]]></category>
		<category><![CDATA[galactic nucleus]]></category>
		<category><![CDATA[herschel]]></category>
		<category><![CDATA[kiloparsec]]></category>
		<category><![CDATA[previous results]]></category>
		<category><![CDATA[radio lobes]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[thermal instability]]></category>
		<category><![CDATA[time profile]]></category>
		<category><![CDATA[young stars]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/residual-cooling-and-persistent-star-formation-amid-agn-feedback-in-abell-2597/</guid>
		<description><![CDATA[New Chandra X-ray and Herschel FIR observations enable a multiwavelength study of active galactic nucleus (AGN) heating and intracluster medium (ICM) cooling in the brightest cluster galaxy of Abell 2597. The new Chandra observations reveal the central &#60; 30 kiloparsec X-ray cavity network to be more extensive than previously thought, and associated with enough enthalpy [...]]]></description>
			<content:encoded><![CDATA[<p>New Chandra X-ray and Herschel FIR observations enable a multiwavelength study of active galactic nucleus (AGN) heating and intracluster medium (ICM) cooling in the brightest cluster galaxy of Abell 2597. The new Chandra observations reveal the central &lt; 30 kiloparsec X-ray cavity network to be more extensive than previously thought, and associated with enough enthalpy to theoretically inhibit the inferred classical cooling flow. Nevertheless, we present new evidence, consistent with previous results, that a moderately strong residual cooling flow is persisting at 4%-8% of the classically predicted rates in a spatially structured manner amid the feedback-driven excavation of the X-ray cavity network. New Herschel observations are used to estimate warm and cold dust masses, a lower-limit gas-to-dust ratio, and a star formation rate consistent with previous measurements. The cooling time profile of the ambient X-ray atmosphere is used to map the locations of the observational star formation entropy threshold as well as the theoretical thermal instability threshold. Both lie just outside the &lt; 30 kpc central region permeated by X-ray cavities, and star formation as well as ionized and molecular gas lie interior to both. The young stars are distributed in an elongated region that is aligned with the radio lobes, and their estimated ages are both younger and older than the X-ray cavity network, suggesting both jet-triggered as well as persistent star formation over the current AGN feedback episode. Bright X-ray knots that are coincident with extended Ly-alpha and FUV continuum filaments motivate a discussion of structured cooling from the ambient hot atmosphere along a projected axis that is perpendicular to X-ray cavity and radio axis. We conclude that the cooling ICM is the dominant contributor of the cold gas reservoir fueling star formation and AGN activity in the Abell 2597 BCG.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/residual-cooling-and-persistent-star-formation-amid-agn-feedback-in-abell-2597/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Multiphase Signatures of AGN Feedback in Abell 2597</title>
		<link>http://voxcharta.org/2012/05/13/multiphase-signatures-of-agn-feedback-in-abell-2597/</link>
		<comments>http://voxcharta.org/2012/05/13/multiphase-signatures-of-agn-feedback-in-abell-2597/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:53:32 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bcg]]></category>
		<category><![CDATA[caveat]]></category>
		<category><![CDATA[cavity]]></category>
		<category><![CDATA[chandra x ray]]></category>
		<category><![CDATA[cluster abell]]></category>
		<category><![CDATA[cluster galaxy]]></category>
		<category><![CDATA[cold gas]]></category>
		<category><![CDATA[core cluster]]></category>
		<category><![CDATA[excess gas]]></category>
		<category><![CDATA[filament]]></category>
		<category><![CDATA[galactic nucleus]]></category>
		<category><![CDATA[inner edge]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[observational evidence]]></category>
		<category><![CDATA[radio data]]></category>
		<category><![CDATA[radio source]]></category>
		<category><![CDATA[ray observations]]></category>
		<category><![CDATA[spatial correlation]]></category>
		<category><![CDATA[spectral analysis]]></category>
		<category><![CDATA[spectral maps]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/multiphase-signatures-of-agn-feedback-in-abell-2597/</guid>
		<description><![CDATA[We present new Chandra X-ray observations of the brightest cluster galaxy (BCG) in the cool core cluster Abell 2597. The data reveal an extensive kpc-scale X-ray cavity network as well as a 15 kpc filament of soft-excess gas exhibiting strong spatial correlation with archival VLA radio data. In addition to several possible scenarios, multiwavelength evidence [...]]]></description>
			<content:encoded><![CDATA[<p>We present new Chandra X-ray observations of the brightest cluster galaxy (BCG) in the cool core cluster Abell 2597. The data reveal an extensive kpc-scale X-ray cavity network as well as a 15 kpc filament of soft-excess gas exhibiting strong spatial correlation with archival VLA radio data. In addition to several possible scenarios, multiwavelength evidence may suggest that the filament is associated with multiphase (10^3 &#8211; 10^7 K) gas that has been entrained and dredged-up by the propagating radio source. Stemming from a full spectral analysis, we also present profiles and 2D spectral maps of modeled X-ray temperature, entropy, pressure, and metal abundance. The maps reveal an arc of hot gas which in projection borders the inner edge of a large X-ray cavity. Although limited by strong caveats, we suggest that the hot arc may be (a) due to a compressed rim of cold gas pushed outward by the radio bubble or (b) morphologically and energetically consistent with cavity-driven active galactic nucleus (AGN) heating models invoked to quench cooling flows, in which the enthalpy of a buoyant X-ray cavity is locally thermalized as ambient gas rushes to refill its wake. If confirmed, this would be the first observational evidence for this model.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/multiphase-signatures-of-agn-feedback-in-abell-2597/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Chemical Abundances of the Milky Way Thick Disk and Stellar Halo I.: Implications of [alpha/Fe] for Star Formation Histories in Their Progenitors</title>
		<link>http://voxcharta.org/2012/05/13/chemical-abundances-of-the-milky-way-thick-disk-and-stellar-halo-i-implications-of-alphafe-for-star-formation-histories-in-their-progenitors/</link>
		<comments>http://voxcharta.org/2012/05/13/chemical-abundances-of-the-milky-way-thick-disk-and-stellar-halo-i-implications-of-alphafe-for-star-formation-histories-in-their-progenitors/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:48:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abundance]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[progenitor]]></category>
		<category><![CDATA[star formation history]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/chemical-abundances-of-the-milky-way-thick-disk-and-stellar-halo-i-implications-of-alphafe-for-star-formation-histories-in-their-progenitors/</guid>
		<description><![CDATA[We present the abundance analysis of 97 nearby metal-poor (-3.3&#60;[Fe/H]&#60;-0.5) stars having kinematics characteristics of the Milky Way (MW) thick disk, inner, and outer stellar halos. The high-resolution, high-signal-to-noise optical spectra for the sample stars have been obtained with the High Dispersion Spectrograph mounted on the Subaru Telescope. Abundances of Fe, Mg, Si, Ca and [...]]]></description>
			<content:encoded><![CDATA[<p>We present the abundance analysis of 97 nearby metal-poor (-3.3&lt;[Fe/H]&lt;-0.5) stars having kinematics characteristics of the Milky Way (MW) thick disk, inner, and outer stellar halos. The high-resolution, high-signal-to-noise optical spectra for the sample stars have been obtained with the High Dispersion Spectrograph mounted on the Subaru Telescope. Abundances of Fe, Mg, Si, Ca and Ti have been derived using a one-dimensional LTE abundance analysis code with Kurucz NEWODF model atmospheres. By assigning membership of the sample stars to the thick disk, inner or outer halo components based on their orbital parameters, we examine abundance ratios as a function of [Fe/H] and kinematics for the three subsamples in wide metallicity and orbital parameter ranges.   We show that, in the metallicity range of -1.5&lt;[Fe/H]-2$. These results favor the scenarios that the MW thick disk formed through rapid chemical enrichment primarily through Type II supernovae of massive stars, while the stellar halo has formed at least in part via accretion of progenitor stellar systems having been chemically enriched with different timescales.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/chemical-abundances-of-the-milky-way-thick-disk-and-stellar-halo-i-implications-of-alphafe-for-star-formation-histories-in-their-progenitors/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Astronomical Evidence for the Rapid Growth of Millimeter Sized Particles in Protoplanetary Disks</title>
		<link>http://voxcharta.org/2012/05/13/astronomical-evidence-for-the-rapid-growth-of-millimeter-sized-particles-in-protoplanetary-disks/</link>
		<comments>http://voxcharta.org/2012/05/13/astronomical-evidence-for-the-rapid-growth-of-millimeter-sized-particles-in-protoplanetary-disks/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:43:55 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astronomical evidence]]></category>
		<category><![CDATA[contrasts]]></category>
		<category><![CDATA[disk evolution]]></category>
		<category><![CDATA[dust grains]]></category>
		<category><![CDATA[infrared observation]]></category>
		<category><![CDATA[lifetime]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[millimeter wavelength]]></category>
		<category><![CDATA[occurrence]]></category>
		<category><![CDATA[planets]]></category>
		<category><![CDATA[radial velocity]]></category>
		<category><![CDATA[rapid growth]]></category>
		<category><![CDATA[sized particles]]></category>
		<category><![CDATA[statistic]]></category>
		<category><![CDATA[statistical result]]></category>
		<category><![CDATA[survey]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/astronomical-evidence-for-the-rapid-growth-of-millimeter-sized-particles-in-protoplanetary-disks/</guid>
		<description><![CDATA[I summarize recent surveys of protoplanetary disks at millimeter wavelengths and show that the distribution of luminosity, equivalent to the mass in small dust grains, declines rapidly. This contrasts with statistics on the lifetime of disks from infrared observations and the high occurrence of planets from radial velocity and transit surveys. I suggest that these [...]]]></description>
			<content:encoded><![CDATA[<p>I summarize recent surveys of protoplanetary disks at millimeter wavelengths and show that the distribution of luminosity, equivalent to the mass in small dust grains, declines rapidly. This contrasts with statistics on the lifetime of disks from infrared observations and the high occurrence of planets from radial velocity and transit surveys. I suggest that these disparate results can be reconciled if most of the dust in a disk is locked up in millimeter and larger sized particles within about 2 Myr. This general statistical result on disk evolution agrees with detailed modeling of a small number of individual disks and with cosmochemical measurements of chondrule ages.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/astronomical-evidence-for-the-rapid-growth-of-millimeter-sized-particles-in-protoplanetary-disks/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Light Element Abundance Distribution in NGC 5128 from Planetary Nebulae</title>
		<link>http://voxcharta.org/2012/05/13/the-light-element-abundance-distribution-in-ngc-5128-from-planetary-nebulae/</link>
		<comments>http://voxcharta.org/2012/05/13/the-light-element-abundance-distribution-in-ngc-5128-from-planetary-nebulae/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:43:27 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[angstrom]]></category>
		<category><![CDATA[central star]]></category>
		<category><![CDATA[element abundance]]></category>
		<category><![CDATA[element oxygen]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[light element]]></category>
		<category><![CDATA[line ratio]]></category>
		<category><![CDATA[luminosity function]]></category>
		<category><![CDATA[photoionization model]]></category>
		<category><![CDATA[photometric studies]]></category>
		<category><![CDATA[planetary nebulae]]></category>
		<category><![CDATA[progenitor]]></category>
		<category><![CDATA[radial gradient]]></category>
		<category><![CDATA[slit spectra]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[vlt]]></category>
		<category><![CDATA[wavelength range]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/the-light-element-abundance-distribution-in-ngc-5128-from-planetary-nebulae/</guid>
		<description><![CDATA[The light element abundance pattern from many planetary nebulae (PNe) covering the upper 4 mag. of the [O III] luminosity function was observed with ESO VLT FORS1 multi-slit. Spectra of 51 PNe over the wavelength range 3500-7500 Angstrom were obtained in three fields at 4, 8 and 17 kpc, for a distance of 3.8 Mpc. [...]]]></description>
			<content:encoded><![CDATA[<p>The light element abundance pattern from many planetary nebulae (PNe) covering the upper 4 mag. of the [O III] luminosity function was observed with ESO VLT FORS1 multi-slit. Spectra of 51 PNe over the wavelength range 3500-7500 Angstrom were obtained in three fields at 4, 8 and 17 kpc, for a distance of 3.8 Mpc. Emission line ratios are entirely typical of PN such as in the Milky Way. The temperature sensitive [O III]4363A line was weakly detected in 10 PNe, both [O II] and [O III] lines were detected in 30 PNe, and only the bright [O III]5007A line in 7 PN. Cloudy photoionization models were run to match the spectra by a spherical, constant density nebula ionized by a black body central star. He, N, O and Ne abundances with respect to H were determined and, for brighter PNe, S and Ar; central star luminosities and temperatures are also derived. For 40 PNe with Cloudy models, from the upper 2 mag. of the luminosity function, the most reliably estimated element, oxygen, has a mean 12+log(O/H) of 8.52. No obvious radial gradient is apparent in O/H over a range 2-20 kpc. Comparison of the PN abundances with the stellar population, from the spectra of the integrated starlight on the multi-slits and photometric studies, suggests [Fe/H]=-0.4 and [O/Fe]=0.25. The masses of the PN central stars in NGC 5128 from model tracks imply an epoch of formation more recent than for the minority young population from colour-magnitude studies. The PNe progenitors may belong to the young tail of a recent, minor, star formation episode or derive from other evolutionary channels.[Abridged]</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/the-light-element-abundance-distribution-in-ngc-5128-from-planetary-nebulae/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Integral Field Spectroscopy Of The Brightest Knots Of Hh 223 In L723</title>
		<link>http://voxcharta.org/2012/05/13/integral-field-spectroscopy-of-the-brightest-knots-of-hh-223-in-l723/</link>
		<comments>http://voxcharta.org/2012/05/13/integral-field-spectroscopy-of-the-brightest-knots-of-hh-223-in-l723/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:42:34 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[band image]]></category>
		<category><![CDATA[electron density]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[emission properties]]></category>
		<category><![CDATA[field spectroscopy]]></category>
		<category><![CDATA[integral field]]></category>
		<category><![CDATA[integral system]]></category>
		<category><![CDATA[intensity maps]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[line ratio]]></category>
		<category><![CDATA[nii]]></category>
		<category><![CDATA[optical counterpart]]></category>
		<category><![CDATA[outflow]]></category>
		<category><![CDATA[proper motion]]></category>
		<category><![CDATA[radial velocity]]></category>
		<category><![CDATA[radial velocity field]]></category>
		<category><![CDATA[ratio maps]]></category>
		<category><![CDATA[spatial sampling]]></category>
		<category><![CDATA[spectral range]]></category>
		<category><![CDATA[wht]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/integral-field-spectroscopy-of-the-brightest-knots-of-hh-223-in-l723/</guid>
		<description><![CDATA[HH 223 is the optical counterpart of a larger scale H2 outflow, driven by the protostellar source VLA 2A, in L723. Its poorly collimated and rather chaotic morphology suggested the Integral Field Spectroscopy (IFS) as an appropriate option to map the emission for deriving the physical conditions and the kinematics. Here we present new results [...]]]></description>
			<content:encoded><![CDATA[<p>HH 223 is the optical counterpart of a larger scale H2 outflow, driven by the protostellar source VLA 2A, in L723. Its poorly collimated and rather chaotic morphology suggested the Integral Field Spectroscopy (IFS) as an appropriate option to map the emission for deriving the physical conditions and the kinematics. Here we present new results based on the IFS observations made with the INTEGRAL system at the WHT. The brightest knots of HH 223 (\sim16 arcsec, 0.02 pc at a distance of 300 pc) were mapped with a single pointing in the spectral range 6200-7700 A. We obtained the emission-line intensity maps for Halpha, [NII] 6584 A and [SII] 6716, 6731 A, and explored the distribution of the excitation and electron density from [NII]/Halpha, [SII]/Halpha, and [SII] 6716/6731 line-ratio maps. Maps of the radial velocity field were obtained. We analysed the 3D-kinematics by combining the knot radial velocities, derived from IFS data, with the knot proper motions derived from multi-epoch, narrow-band images. The intensity maps built from IFS data reproduced well the morphology found in the narrow-band images. We checked the results obtained from previous long-slit observations with those derived from IFS spectra extracted with a similar spatial sampling. At the positions intersected by the slit, the physical conditions and kinematics derived from IFS are compatible with those derived from long-slit data. In contrast, significant discrepancies were found when the results from long-slit data were compared with the ones derived from IFS spectra extracted at positions shifted a few arcsec from those intersected by the slit. This clearly revealed IFS observations as the best choice to get a reliable picture of the HH emission properties.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/integral-field-spectroscopy-of-the-brightest-knots-of-hh-223-in-l723/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>On Galaxies and Homology</title>
		<link>http://voxcharta.org/2012/05/13/on-galaxies-and-homology/</link>
		<comments>http://voxcharta.org/2012/05/13/on-galaxies-and-homology/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:41:40 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[ambiguity]]></category>
		<category><![CDATA[anisotropy]]></category>
		<category><![CDATA[baryonic matter]]></category>
		<category><![CDATA[component galaxies]]></category>
		<category><![CDATA[constants]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[different concepts]]></category>
		<category><![CDATA[galaxy merger]]></category>
		<category><![CDATA[half mass]]></category>
		<category><![CDATA[kinematic structure]]></category>
		<category><![CDATA[mass radius]]></category>
		<category><![CDATA[multi component]]></category>
		<category><![CDATA[quantities]]></category>
		<category><![CDATA[relationship]]></category>
		<category><![CDATA[remnant]]></category>
		<category><![CDATA[respects]]></category>
		<category><![CDATA[sole source]]></category>
		<category><![CDATA[variation]]></category>
		<category><![CDATA[velocity dispersion]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/on-galaxies-and-homology/</guid>
		<description><![CDATA[The definition of homology for single-component galaxies is clear, but for multi-component (luminous and dark matter) galaxies there is some ambiguity. We attempt to clarify the situation by carefully separating the different concepts of homology that have been used to date. We argue that the most useful definition is that a set of galaxies is [...]]]></description>
			<content:encoded><![CDATA[<p>The definition of homology for single-component galaxies is clear, but for multi-component (luminous and dark matter) galaxies there is some ambiguity. We attempt to clarify the situation by carefully separating the different concepts of homology that have been used to date. We argue that the most useful definition is that a set of galaxies is homologous if they are the same in all respects up to a set of three dimensional scaling constants which may differ from one galaxy to the next. Noting that we are free to choose the dimensional constants, we find that a set of hydrodynamic simulated galaxy merger remnants is significantly closer to homologous when the dimensional length constant is taken to be the radius containing equal amounts of dark and baryonic matter rather than the usual observationally motivated choice of the baryonic half-mass radius. Once the correct dimensional scaling constants are used, the stellar velocity dispersion anisotropy is essentially the sole source of the variation in the kinematic structure of these simulated merger remnants. In order to facilitate the use of these scaling constants to analyse observed galaxies, we calculated the relationship between our preferred dimensional scaling constants and the typical observationally accessible quantities.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/on-galaxies-and-homology/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A High Resolution Study of the HI-H2 Transition across the Perseus Molecular Cloud [Replacement]</title>
		<link>http://voxcharta.org/2012/05/13/a-high-resolution-study-of-the-hi-h2-transition-across-the-perseus-molecular-cloud-replacement/</link>
		<comments>http://voxcharta.org/2012/05/13/a-high-resolution-study-of-the-hi-h2-transition-across-the-perseus-molecular-cloud-replacement/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:36:44 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[arecibo]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[extinction]]></category>
		<category><![CDATA[fundamental principle]]></category>
		<category><![CDATA[giant molecular cloud]]></category>
		<category><![CDATA[h2 surface]]></category>
		<category><![CDATA[hi data]]></category>
		<category><![CDATA[hi survey]]></category>
		<category><![CDATA[infrared data]]></category>
		<category><![CDATA[internal radiation]]></category>
		<category><![CDATA[ira]]></category>
		<category><![CDATA[l band]]></category>
		<category><![CDATA[photodissociation]]></category>
		<category><![CDATA[radiation field]]></category>
		<category><![CDATA[sigma]]></category>
		<category><![CDATA[spatial variation]]></category>
		<category><![CDATA[surface density]]></category>
		<category><![CDATA[timescale]]></category>
		<category><![CDATA[v band]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/a-high-resolution-study-of-the-hi-h2-transition-across-the-perseus-molecular-cloud-replacement/</guid>
		<description><![CDATA[To investigate the fundamental principles of H2 formation in a giant molecular cloud (GMC), we derive the HI and H2 surface density (Sigma_HI and Sigma_H2) images of the Perseus molecular cloud on sub-pc scales (~0.4 pc). We use the far-infrared data from the Improved Reprocessing of the IRAS Survey and the V-band extinction image provided [...]]]></description>
			<content:encoded><![CDATA[<p>To investigate the fundamental principles of H2 formation in a giant molecular cloud (GMC), we derive the HI and H2 surface density (Sigma_HI and Sigma_H2) images of the Perseus molecular cloud on sub-pc scales (~0.4 pc). We use the far-infrared data from the Improved Reprocessing of the IRAS Survey and the V-band extinction image provided by the COMPLETE Survey to estimate the dust column density image of Perseus. In combination with the HI data from the Galactic Arecibo L-band Feed Array HI Survey and an estimate of the local dust-to-gas ratio, we then derive the Sigma_H2 distribution across Perseus. We find a relatively uniform Sigma_HI ~ 6-8 Msun pc^-2 for both dark and star-forming regions, suggesting a minimum HI surface density required to shield H2 against photodissociation. As a result, a remarkably tight and consistent relation is found between Sigma_H2/Sigma_HI and Sigma_HI+Sigma_H2. The transition between the HI- and H2-dominated regions occurs at N(HI)+2N(H2) ~ (8-14) x 10^20 cm^-2. Our findings are consistent with predictions for H2 formation in equilibrium, suggesting that turbulence may not be of primary importance for H2 formation. However, the importance of a warm neutral medium for H2 shielding, an internal radiation field, and the timescale of H2 formation still remain as open questions. We also compare H2 and CO distributions and estimate the fraction of &#8220;CO-dark&#8221; gas, f_DG ~ 0.3. While significant spatial variations of f_DG are found, we do not find a clear correlation with the mean V-band extinction.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/a-high-resolution-study-of-the-hi-h2-transition-across-the-perseus-molecular-cloud-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Cosmological X-ray Scattering from Intergalactic Dust [Replacement]</title>
		<link>http://voxcharta.org/2012/05/13/cosmological-x-ray-scattering-from-intergalactic-dust-replacement/</link>
		<comments>http://voxcharta.org/2012/05/13/cosmological-x-ray-scattering-from-intergalactic-dust-replacement/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:35:08 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[clump]]></category>
		<category><![CDATA[cosmic history]]></category>
		<category><![CDATA[cosmological context]]></category>
		<category><![CDATA[cosmological distances]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[dust grains]]></category>
		<category><![CDATA[energy parameters]]></category>
		<category><![CDATA[grain size]]></category>
		<category><![CDATA[metallicity]]></category>
		<category><![CDATA[petric]]></category>
		<category><![CDATA[photon energy]]></category>
		<category><![CDATA[point source]]></category>
		<category><![CDATA[power law distribution]]></category>
		<category><![CDATA[ray point]]></category>
		<category><![CDATA[relative contribution]]></category>
		<category><![CDATA[size constraint]]></category>
		<category><![CDATA[soft x]]></category>
		<category><![CDATA[surface brightness]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/cosmological-x-ray-scattering-from-intergalactic-dust-replacement/</guid>
		<description><![CDATA[High resolution X-ray imaging offers a unique opportunity to probe the nature of dust in the z ~&#60; 2 universe. Dust grains 0.1- 1 um in size will scatter soft X-rays, producing a diffuse &#34;halo&#34; image around an X-ray point source, with a brightness ~ few % confined to an arcminute-sized region. We derive the [...]]]></description>
			<content:encoded><![CDATA[<p>High resolution X-ray imaging offers a unique opportunity to probe the nature of dust in the z ~&lt; 2 universe. Dust grains 0.1- 1 um in size will scatter soft X-rays, producing a diffuse &quot;halo&quot; image around an X-ray point source, with a brightness ~ few % confined to an arcminute-sized region. We derive the formulae for scattering in a cosmological context and calculate the surface brightness of the scattering halo due to (i) an IGM uniformly enriched (Omega_ d ~ 10^-5) by a power-law distribution of grain sizes, and (ii) a DLA-type (N_H ~ 10^21 cm^-2) dust screen at cosmological distances. The morphology of the surface brightness profile can distinguish between the two scenarios above, place size constraints on dusty clumps, and constrain the homogeneity of the IGM. Thus X-ray scattering can gauge the relative contribution of the first stars, dwarf galaxies, and galactic outflows to the cosmic metallicity budget and cosmic history of dust. We show that, because the amount of intergalactic scattering is overestimated for photon energies &lt; 1 keV, the non-detection of an X-ray scattering halo by Petric et al. (2006) is consistent with `grey&#039; intergalactic dust grains (Omega_d ~ 10^-5$) when the data is restricted to the 1-8 keV band. We also calculate the systematic offset in magnitude, delta m ~ 0.01, for such a population of graphite grains, which would affect the type of supernova survey ideal for measuring dark energy parameters within ~ 1% precision.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/cosmological-x-ray-scattering-from-intergalactic-dust-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Triggered star formation surrounding Wolf-Rayet star HD 211853 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/13/triggered-star-formation-surrounding-wolf-rayet-star-hd-211853-replacement/</link>
		<comments>http://voxcharta.org/2012/05/13/triggered-star-formation-surrounding-wolf-rayet-star-hd-211853-replacement/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:34:43 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[core]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[fragmentation]]></category>
		<category><![CDATA[gravitational collapse]]></category>
		<category><![CDATA[hi emission]]></category>
		<category><![CDATA[infrared emission]]></category>
		<category><![CDATA[ionized gas]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[large scale]]></category>
		<category><![CDATA[molecular emission]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[radiation]]></category>
		<category><![CDATA[radio]]></category>
		<category><![CDATA[sequential star formation]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[star hd]]></category>
		<category><![CDATA[stellar object]]></category>
		<category><![CDATA[wolf]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/triggered-star-formation-surrounding-wolf-rayet-star-hd-211853-replacement/</guid>
		<description><![CDATA[The environment surrounding Wolf-Rayet star HD 211853 is studied in molecular emission, infrared emission, as well as radio and HI emission. The molecular ring consists of well-separated cores, which have a volume density of 10$^{3}$ cm$^{-3}$ and kinematic temperature $\sim$20 K. Most of the cores are under gravitational collapse due to external pressure from the [...]]]></description>
			<content:encoded><![CDATA[<p>The environment surrounding Wolf-Rayet star HD 211853 is studied in molecular emission, infrared emission, as well as radio and HI emission. The molecular ring consists of well-separated cores, which have a volume density of 10$^{3}$ cm$^{-3}$ and kinematic temperature $\sim$20 K. Most of the cores are under gravitational collapse due to external pressure from the surrounding ionized gas. From SED modeling towards the young stellar objects (YSOs), sequential star formation is revealed on a large scale in space spreading from the Wolf-Rayet star to the molecular ring. A small scale sequential star formation is revealed towards core A, which harbors a very young star cluster. Triggered star formations is thus suggested. The presence of PDR, the fragmentation of the molecular ring, the collapse of the cores, the large scale sequential star formation indicate the &#8220;Collect and Collapse&#8221; process functions in this region. The star forming activities in core A seem to be affected by the &#8220;Radiation-Driven Implosion&#8221; (RDI) process.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/triggered-star-formation-surrounding-wolf-rayet-star-hd-211853-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>On the Spectroscopic Classes of Novae in M33 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/13/on-the-spectroscopic-classes-of-novae-in-m33-replacement/</link>
		<comments>http://voxcharta.org/2012/05/13/on-the-spectroscopic-classes-of-novae-in-m33-replacement/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:33:27 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[11a]]></category>
		<category><![CDATA[12a]]></category>
		<category><![CDATA[decline]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[hybrid classes]]></category>
		<category><![CDATA[initial results]]></category>
		<category><![CDATA[m31]]></category>
		<category><![CDATA[m33]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[novae]]></category>
		<category><![CDATA[spectroscopic data]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[white dwarf]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/on-the-spectroscopic-classes-of-novae-in-m33-replacement/</guid>
		<description><![CDATA[We report the initial results from an ongoing multi-year spectroscopic survey of novae in M33. The survey resulted in the spectroscopic classification of six novae (M33N 2006-09a, 2007-09a, 2009-01a, 2010-10a, 2010-11a, and 2011-12a) and a determination of rates of decline (t_2 times) for four of them (2006-09a, 2007-09a, 2009-01a, and 2010-10a). When these data are [...]]]></description>
			<content:encoded><![CDATA[<p>We report the initial results from an ongoing multi-year spectroscopic survey of novae in M33. The survey resulted in the spectroscopic classification of six novae (M33N 2006-09a, 2007-09a, 2009-01a, 2010-10a, 2010-11a, and 2011-12a) and a determination of rates of decline (t_2 times) for four of them (2006-09a, 2007-09a, 2009-01a, and 2010-10a). When these data are combined with existing spectroscopic data for two additional M33 novae (2003-09a and 2008-02a) we find that 5 of the 8 novae with available spectroscopic class appear to be members of either the He/N or Fe IIb (hybrid) classes, with only two clear members of the Fe II spectroscopic class. This initial finding is very different from what would be expected based on the results for M31 and the Galaxy where Fe II novae dominate, and the He/N and Fe IIb classes together make up only ~20% of the total. It is plausible that the increased fraction of He/N and Fe IIb novae observed in M33 thus far may be the result of the younger stellar population that dominates this galaxy, which is expected to produce novae that harbor generally more massive white dwarfs than those typically associated with novae in M31 or the Milky Way.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/on-the-spectroscopic-classes-of-novae-in-m33-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Close encounters of the protostellar kind in IC 1396N [Replacement]</title>
		<link>http://voxcharta.org/2012/05/13/close-encounters-of-the-protostellar-kind-in-ic-1396n-replacement/</link>
		<comments>http://voxcharta.org/2012/05/13/close-encounters-of-the-protostellar-kind-in-ic-1396n-replacement/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:31:29 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[continuum]]></category>
		<category><![CDATA[emission features]]></category>
		<category><![CDATA[globule]]></category>
		<category><![CDATA[hydrogen emission]]></category>
		<category><![CDATA[line emission]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[micron]]></category>
		<category><![CDATA[molecular hydrogen]]></category>
		<category><![CDATA[pdbi]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[sky]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/close-encounters-of-the-protostellar-kind-in-ic-1396n-replacement/</guid>
		<description><![CDATA[We have mapped in the 2.7 mm continuum and 12CO with the PdBI the IR-dark &#8220;tail&#8221; that crosses the IC 1396N globule from south to north, and is the most extincted part of this cloud. These observations have allowed us to distinguish all possible associations of molecular hydrogen emission features by revealing the presence of [...]]]></description>
			<content:encoded><![CDATA[<p>We have mapped in the 2.7 mm continuum and 12CO with the PdBI the IR-dark &#8220;tail&#8221; that crosses the IC 1396N globule from south to north, and is the most extincted part of this cloud. These observations have allowed us to distinguish all possible associations of molecular hydrogen emission features by revealing the presence of two well-collimated low-mass protostellar outflows at the northern part of the globule. The outflows are located almost in the plane of the sky and are colliding with each other towards the position of a strong 2.12 microns H2 line emission feature.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/close-encounters-of-the-protostellar-kind-in-ic-1396n-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Is the observed high-frequency radio luminosity distribution of QSOs bimodal?</title>
		<link>http://voxcharta.org/2012/05/10/is-the-observed-high-frequency-radio-luminosity-distribution-of-qsos-bimodal/</link>
		<comments>http://voxcharta.org/2012/05/10/is-the-observed-high-frequency-radio-luminosity-distribution-of-qsos-bimodal/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:39:55 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[AGN]]></category>
		<category><![CDATA[bimodal distribution]]></category>
		<category><![CDATA[continuous distribution]]></category>
		<category><![CDATA[formation rates]]></category>
		<category><![CDATA[galaxy survey]]></category>
		<category><![CDATA[high frequency radio]]></category>
		<category><![CDATA[literature]]></category>
		<category><![CDATA[lobes]]></category>
		<category><![CDATA[luminosity distribution]]></category>
		<category><![CDATA[population]]></category>
		<category><![CDATA[previous results]]></category>
		<category><![CDATA[probes]]></category>
		<category><![CDATA[radio emission]]></category>
		<category><![CDATA[radio frequency]]></category>
		<category><![CDATA[sigma]]></category>
		<category><![CDATA[solar mass]]></category>
		<category><![CDATA[star formation processes]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/is-the-observed-high-frequency-radio-luminosity-distribution-of-qsos-bimodal/</guid>
		<description><![CDATA[The distribution of QSO radio luminosities has long been debated in the literature. Some argue that it is a bimodal distribution, implying that there are two separate QSO populations (normally referred to as &#8216;radio-loud&#8217; and &#8216;radio-quiet&#8217;), while others claim it forms a more continuous distribution characteristic of a single population. We use deep observations at [...]]]></description>
			<content:encoded><![CDATA[<p>The distribution of QSO radio luminosities has long been debated in the literature. Some argue that it is a bimodal distribution, implying that there are two separate QSO populations (normally referred to as &#8216;radio-loud&#8217; and &#8216;radio-quiet&#8217;), while others claim it forms a more continuous distribution characteristic of a single population. We use deep observations at 20 GHz to investigate whether the distribution is bimodal at high radio frequencies. Carrying out this study at high radio frequencies has an advantage over previous studies as the radio emission comes predominantly from the core of the AGN, hence probes the most recent activity. Studies carried out at lower frequencies are dominated by the large scale lobes where the emission is built up over longer timescales (10^7-10^8 yrs), thereby confusing the sample. Our sample comprises 874 X-ray selected QSOs that were observed as part of the 6dF Galaxy Survey. Of these, 40% were detected down to a 3 sigma detection limit of 0.2-0.5 mJy.   No evidence of bimodality is seen in either the 20 GHz luminosity distribution or in the distribution of the R_20 parameter: the ratio of the radio to optical luminosities traditionally used to classify objects as being either radio-loud or radio-quiet. Previous results have claimed that at low radio luminosities, star formation processes can dominate the radio emission observed in QSOs. We attempt to investigate these claims by stacking the undetected sources at 20 GHz and discuss the limitations in carrying out this analysis. However, if the radio emission was solely due to star formation processes, we calculate that this corresponds to star formation rates ranging from ~10 solar masses/yr to ~2300 solar masses/yr.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/is-the-observed-high-frequency-radio-luminosity-distribution-of-qsos-bimodal/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Close encounters of the protostellar kind in IC 1396N</title>
		<link>http://voxcharta.org/2012/05/10/close-encounters-of-the-protostellar-kind-in-ic-1396n/</link>
		<comments>http://voxcharta.org/2012/05/10/close-encounters-of-the-protostellar-kind-in-ic-1396n/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:39:03 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[continuum]]></category>
		<category><![CDATA[emission features]]></category>
		<category><![CDATA[globule]]></category>
		<category><![CDATA[hydrogen emission]]></category>
		<category><![CDATA[line emission]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[micron]]></category>
		<category><![CDATA[molecular hydrogen]]></category>
		<category><![CDATA[pdbi]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[sky]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/close-encounters-of-the-protostellar-kind-in-ic-1396n/</guid>
		<description><![CDATA[We have mapped in the 2.7 mm continuum and 12CO with the PdBI the IR-dark &#8220;tail&#8221; that crosses the IC 1396N globule from south to north, and is the most extincted part of this cloud. These observations have allowed us to distinguish all possible associations of molecular hydrogen emission features by revealing the presence of [...]]]></description>
			<content:encoded><![CDATA[<p>We have mapped in the 2.7 mm continuum and 12CO with the PdBI the IR-dark &#8220;tail&#8221; that crosses the IC 1396N globule from south to north, and is the most extincted part of this cloud. These observations have allowed us to distinguish all possible associations of molecular hydrogen emission features by revealing the presence of two well-collimated low-mass protostellar outflows at the northern part of the globule. The outflows are located almost in the plane of the sky and are colliding with each other towards the position of a strong 2.12 microns H2 line emission feature.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/close-encounters-of-the-protostellar-kind-in-ic-1396n/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Tracers of Discs and Winds around Intermediate and High Mass Young Stellar Objects</title>
		<link>http://voxcharta.org/2012/05/10/tracers-of-discs-and-winds-around-intermediate-and-high-mass-young-stellar-objects/</link>
		<comments>http://voxcharta.org/2012/05/10/tracers-of-discs-and-winds-around-intermediate-and-high-mass-young-stellar-objects/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:37:37 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorption]]></category>
		<category><![CDATA[accretion disc]]></category>
		<category><![CDATA[circumstellar environment]]></category>
		<category><![CDATA[dense material]]></category>
		<category><![CDATA[disc model]]></category>
		<category><![CDATA[doppler]]></category>
		<category><![CDATA[electron]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[high speed]]></category>
		<category><![CDATA[inner regions]]></category>
		<category><![CDATA[mass range]]></category>
		<category><![CDATA[mass star]]></category>
		<category><![CDATA[outflow]]></category>
		<category><![CDATA[similarity]]></category>
		<category><![CDATA[speed motion]]></category>
		<category><![CDATA[stellar object]]></category>
		<category><![CDATA[stellar wind]]></category>
		<category><![CDATA[tracers]]></category>
		<category><![CDATA[transition]]></category>
		<category><![CDATA[wings]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/tracers-of-discs-and-winds-around-intermediate-and-high-mass-young-stellar-objects/</guid>
		<description><![CDATA[We present a study of the kinematical properties of a small sample of nearby near-infrared bright massive and intermediate mass young stellar objects using emission lines sensitive to discs and winds. We show for the first time that the broad ($\sim500$kms$^{-1}$) symmetric line wings on the HI Brackett series lines are due to Stark broadening [...]]]></description>
			<content:encoded><![CDATA[<p>We present a study of the kinematical properties of a small sample of nearby near-infrared bright massive and intermediate mass young stellar objects using emission lines sensitive to discs and winds. We show for the first time that the broad ($\sim500$kms$^{-1}$) symmetric line wings on the HI Brackett series lines are due to Stark broadening or electron scattering, rather than pure Doppler broadening due to high speed motion. The results are consistent with the presence of a very dense circumstellar environment. In addition, many of these lines show evidence for weak line self-absorption, suggestive of a wind or disc-wind origin for that part of the absorbing material. The weakness of the self-absorption suggests a large opening angle for such an outflow. We also study the fluorescent 1.688$\mu$m FeII line, which is sensitive to dense material. We fitted a Keplerian disc model to this line, and find reasonable fits in all bar one case, in agreement with previous finding for classical Be stars that fluorescent iron transitions are reasonable disc tracers. Overall the picture is one in which these stars still have accretion discs, with a very dense inner circumstellar environment which may be tracing either the inner regions of a disc, or of a stellar wind, and in which ionised outflow is also present. The similarity with lower mass stars is striking, suggesting that at least in this mass range they form in a similar fashion.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/tracers-of-discs-and-winds-around-intermediate-and-high-mass-young-stellar-objects/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Pulsar Spin&#8211;Velocity Alignment: Further Results and Discussion</title>
		<link>http://voxcharta.org/2012/05/10/pulsar-spin-velocity-alignment-further-results-and-discussion/</link>
		<comments>http://voxcharta.org/2012/05/10/pulsar-spin-velocity-alignment-further-results-and-discussion/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:37:19 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[alignment]]></category>
		<category><![CDATA[angle]]></category>
		<category><![CDATA[axis]]></category>
		<category><![CDATA[confidence]]></category>
		<category><![CDATA[offsets]]></category>
		<category><![CDATA[polarisation]]></category>
		<category><![CDATA[proper motion]]></category>
		<category><![CDATA[pulsars]]></category>
		<category><![CDATA[sigma]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[vector]]></category>
		<category><![CDATA[velocities]]></category>
		<category><![CDATA[velocity distribution]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/pulsar-spin-velocity-alignment-further-results-and-discussion/</guid>
		<description><![CDATA[The reported alignment between the projected spin-axes and proper motion directions of pulsars is revisited in the light of new data from Jodrell Bank and Effelsberg. The present investigation uses 54 pulsars, the largest to date sample of pulsars with proper-motion and absolute polarisation, to study this effect. Our study has found strong evidence for [...]]]></description>
			<content:encoded><![CDATA[<p>The reported alignment between the projected spin-axes and proper motion directions of pulsars is revisited in the light of new data from Jodrell Bank and Effelsberg. The present investigation uses 54 pulsars, the largest to date sample of pulsars with proper-motion and absolute polarisation, to study this effect. Our study has found strong evidence for pulsar spin-velocity alignment, excluding that those two vectors are completely uncorrelated, with &gt;99% confidence. Although we cannot exclude the possibility of orthogonal spin-velocity configurations, comparison of the data with simulations shows that the scenario of aligned vectors is more likely than that of the orthogonal case. Moreover, we have determined the spread of velocities that a spin-aligned and spin-orthogonal distribution of kicks must have to produce the observed distribution of spin-velocity angle offsets. If the observed distribution of spin-velocity offset angles is the result of spin-aligned kicks, then we find that the distribution of kick-velocity directions must be broad with {\sigma}_v~30\degree if the orthogonal-kick scenario is assumed, then the velocity distribution is much narrower with {\sigma}_v&lt;10\degree. Finally, in contrast to previous studies, we have performed robustness tests on our data, in order to determine whether our conclusions are the result of a statistical and/or systematic bias. The conclusion of a correlation between the spin and velocity vectors is independent of a bias introduced by subsets in the total sample. Moreover, we estimate that the observed alignment is robust to within 10% systematic uncertainties on the determination of the spin-axis direction from polarisation data.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/pulsar-spin-velocity-alignment-further-results-and-discussion/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Investigating the stellar system&#8217;s life-time and the evolution of their mass function using N-body simulation</title>
		<link>http://voxcharta.org/2012/05/10/investigating-the-stellar-systems-life-time-and-the-evolution-of-their-mass-function-using-n-body-simulation/</link>
		<comments>http://voxcharta.org/2012/05/10/investigating-the-stellar-systems-life-time-and-the-evolution-of-their-mass-function-using-n-body-simulation/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:37:00 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[body relaxation]]></category>
		<category><![CDATA[body simulation]]></category>
		<category><![CDATA[dissolution]]></category>
		<category><![CDATA[dynamical evolution]]></category>
		<category><![CDATA[half mass]]></category>
		<category><![CDATA[initial parameters]]></category>
		<category><![CDATA[life time]]></category>
		<category><![CDATA[linear relation]]></category>
		<category><![CDATA[mass function]]></category>
		<category><![CDATA[mass radius]]></category>
		<category><![CDATA[mass star]]></category>
		<category><![CDATA[relaxation time]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[slope]]></category>
		<category><![CDATA[star cluster]]></category>
		<category><![CDATA[stellar cluster]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[stellar system]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/investigating-the-stellar-systems-life-time-and-the-evolution-of-their-mass-function-using-n-body-simulation/</guid>
		<description><![CDATA[In this thesis we study several aspects of dynamical evolution of stellar clusters. The results of more than 200 simulations of single-mass star clusters with different initial total mass, half-mass radius and galactocentric distance, are reported. Recent studies of star clusters show a linear relation between a star cluster&#8217;s dissolution time and its two-body relaxation [...]]]></description>
			<content:encoded><![CDATA[<p>In this thesis we study several aspects of dynamical evolution of stellar clusters. The results of more than 200 simulations of single-mass star clusters with different initial total mass, half-mass radius and galactocentric distance, are reported. Recent studies of star clusters show a linear relation between a star cluster&#8217;s dissolution time and its two-body relaxation time in logarithmic scale. We found that the single-mass star clusters do not show such a linear relation. We present new modified initial parameters to obtain a linear relation for single-mass star clusters. Also the evolution of multi-mass clusters and their lifetime, in the presence of the Galaxy is investigated. We simulate about 90 multi-mass star clusters with the Nbody6 code. These clusters have different initial total mass, half-mass radius and galactocentric distance. Finally we investigate the evolution of the stellar mass function and show that the slopes of the mass functions decrease with time. In addition we study the effect of galactocentric distance of star clusters on the evolution of the mass function.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/investigating-the-stellar-systems-life-time-and-the-evolution-of-their-mass-function-using-n-body-simulation/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Evolving Gravitationally Unstable Disks Over Cosmic Time: Implications For Thick Disk Formation [Replacement]</title>
		<link>http://voxcharta.org/2012/05/10/evolving-gravitationally-unstable-disks-over-cosmic-time-implications-for-thick-disk-formation-replacement/</link>
		<comments>http://voxcharta.org/2012/05/10/evolving-gravitationally-unstable-disks-over-cosmic-time-implications-for-thick-disk-formation-replacement/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:34:25 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[cosmic time]]></category>
		<category><![CDATA[disk formation]]></category>
		<category><![CDATA[disk galaxy]]></category>
		<category><![CDATA[dispersion]]></category>
		<category><![CDATA[energetics]]></category>
		<category><![CDATA[gravitational instability]]></category>
		<category><![CDATA[high velocity]]></category>
		<category><![CDATA[matter of minutes]]></category>
		<category><![CDATA[metallicity]]></category>
		<category><![CDATA[simulation code]]></category>
		<category><![CDATA[solar neighborhood]]></category>
		<category><![CDATA[spiral structure]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[thin disk]]></category>
		<category><![CDATA[Turbulence]]></category>
		<category><![CDATA[velocity dispersion]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/evolving-gravitationally-unstable-disks-over-cosmic-time-implications-for-thick-disk-formation-replacement/</guid>
		<description><![CDATA[Observations of disk galaxies at z~2 have demonstrated that turbulence driven by gravitational instability can dominate the energetics of the disk. We present a 1D simulation code, which we have made publicly available, that economically evolves these galaxies from z~2 to z~0 on a single CPU in a matter of minutes, tracking column density, metallicity, [...]]]></description>
			<content:encoded><![CDATA[<p>Observations of disk galaxies at z~2 have demonstrated that turbulence driven by gravitational instability can dominate the energetics of the disk. We present a 1D simulation code, which we have made publicly available, that economically evolves these galaxies from z~2 to z~0 on a single CPU in a matter of minutes, tracking column density, metallicity, and velocity dispersions of gaseous and multiple stellar components. We include an H$_2$ regulated star formation law and the effects of stellar heating by transient spiral structure. We use this code to demonstrate a possible explanation for the existence of a thin and thick disk stellar population and the age-velocity dispersion correlation of stars in the solar neighborhood: the high velocity dispersion of gas in disks at z~2 decreases along with the cosmological accretion rate, while at lower redshift, the dynamically colder gas forms the low velocity dispersion stars of the thin disk.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/evolving-gravitationally-unstable-disks-over-cosmic-time-implications-for-thick-disk-formation-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Tidal Tails of Minor Mergers: Star Formation Efficiency in the Western Tail of NGC 2782 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/10/tidal-tails-of-minor-mergers-star-formation-efficiency-in-the-western-tail-of-ngc-2782-replacement/</link>
		<comments>http://voxcharta.org/2012/05/10/tidal-tails-of-minor-mergers-star-formation-efficiency-in-the-western-tail-of-ngc-2782-replacement/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:31:23 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[dense region]]></category>
		<category><![CDATA[disk galaxy]]></category>
		<category><![CDATA[galaxy evolution explorer]]></category>
		<category><![CDATA[gas density]]></category>
		<category><![CDATA[global star formation]]></category>
		<category><![CDATA[kiloparsec]]></category>
		<category><![CDATA[mass ratio]]></category>
		<category><![CDATA[mass star]]></category>
		<category><![CDATA[metallicity]]></category>
		<category><![CDATA[myr]]></category>
		<category><![CDATA[narrowband]]></category>
		<category><![CDATA[orders of magnitude]]></category>
		<category><![CDATA[sfr]]></category>
		<category><![CDATA[spiral ngc]]></category>
		<category><![CDATA[star cluster]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[tidal debris]]></category>
		<category><![CDATA[tidal tail]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/tidal-tails-of-minor-mergers-star-formation-efficiency-in-the-western-tail-of-ngc-2782-replacement/</guid>
		<description><![CDATA[While major mergers and their tidal debris are well studied, they are less common than minor mergers (mass ratios &#60; 0.3). The peculiar spiral NGC 2782 is the result of a merger between two disk galaxies with a mass ratio of ~4:1 occurring ~200 Myr ago. This merger produced a molecular and H I-rich, optically [...]]]></description>
			<content:encoded><![CDATA[<p>While major mergers and their tidal debris are well studied, they are less common than minor mergers (mass ratios &lt; 0.3). The peculiar spiral NGC 2782 is the result of a merger between two disk galaxies with a mass ratio of ~4:1 occurring ~200 Myr ago. This merger produced a molecular and H I-rich, optically bright eastern tail and an H I-rich, optically faint western tail. Non-detection of CO in the western tail by Braine et al. suggested that star formation had not yet begun to occur in that tidal tail. However, deep H{\alpha} narrowband images show evidence of recent star formation in the western tail. Across the entire western tail, we find the global star formation rate per unit area ({\Sigma}SFR) to be several orders of magnitude less than expected from the total gas density. Together with extended FUV+NUV emission from Galaxy Evolution Explorer along the tail, this indicates a low global star formation efficiency in the tidal tail producing lower mass star clusters. The H II region that we observed has a local (few-kiloparsec scale) {\Sigma}SFR from H{\alpha} that is less than that expected from the total gas density, which is consistent with other observations of tidal debris. The star formation efficiency of this H II region inferred from the total gas density is low, but normal when inferred from the molecular gas density. These results suggest the presence of a very small, locally dense region in the western tail of NGC 2782 or of a low-metallicity and/or low-pressure star-forming region.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/tidal-tails-of-minor-mergers-star-formation-efficiency-in-the-western-tail-of-ngc-2782-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Deep Silicate absorption features in Compton-thick AGN predominantly arise due to dust in the host galaxy</title>
		<link>http://voxcharta.org/2012/05/09/deep-silicate-absorption-features-in-compton-thick-agn-predominantly-arise-due-to-dust-in-the-host-galaxy/</link>
		<comments>http://voxcharta.org/2012/05/09/deep-silicate-absorption-features-in-compton-thick-agn-predominantly-arise-due-to-dust-in-the-host-galaxy/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:48:12 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorption feature]]></category>
		<category><![CDATA[AGN]]></category>
		<category><![CDATA[cm 2]]></category>
		<category><![CDATA[compton]]></category>
		<category><![CDATA[dust extinction]]></category>
		<category><![CDATA[hard energy]]></category>
		<category><![CDATA[host galaxy]]></category>
		<category><![CDATA[infrared spectrograph]]></category>
		<category><![CDATA[irs]]></category>
		<category><![CDATA[keV]]></category>
		<category><![CDATA[Lambda]]></category>
		<category><![CDATA[obs]]></category>
		<category><![CDATA[silicate]]></category>
		<category><![CDATA[spectral measurement]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/deep-silicate-absorption-features-in-compton-thick-agn-predominantly-arise-due-to-dust-in-the-host-galaxy/</guid>
		<description><![CDATA[We explore the origin of mid-infrared (mid-IR) dust extinction in all 20 nearby (z  1.5 x 10^24 cm^-2) AGN with hard energy (E &#62; 10 keV) X-ray spectral measurements. We accurately measure the silicate absorption features at lambda~9.7um in archival low-resolution (R~57-127) Spitzer Infrared Spectrograph (IRS) spectroscopy, and show that only a minority (~45%) [...]]]></description>
			<content:encoded><![CDATA[<p>We explore the origin of mid-infrared (mid-IR) dust extinction in all 20 nearby (z  1.5 x 10^24 cm^-2) AGN with hard energy (E &gt; 10 keV) X-ray spectral measurements. We accurately measure the silicate absorption features at lambda~9.7um in archival low-resolution (R~57-127) Spitzer Infrared Spectrograph (IRS) spectroscopy, and show that only a minority (~45%) of nearby Compton-thick AGN have strong Si-absorption features (S_9.7 = ln(f_{int}/f_{obs}) &gt; 0.5) which would indicate significant dust attenuation. The majority (~60%) are star-formation dominated (AGN:SB&lt;0.5) at mid-IR wavelengths and lack the spectral signatures of AGN activity at optical wavelengths, most likely because the AGN emission-lines are optically-extinguished. Those Compton-thick AGN hosted in low-inclination angle galaxies exhibit a narrow-range in Si-absorption (S_9.7 ~ 0-0.3), which is consistent with that predicted by clumpy-torus models. However, on the basis of the IR spectra and additional lines of evidence, we conclude that the dominant contribution to the observed mid-IR dust extinction is dust located in the host galaxy (i.e., due to disturbed morphologies; dust-lanes; galaxy inclination angles) and not necessarily a compact obscuring torus surrounding the central engine.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/deep-silicate-absorption-features-in-compton-thick-agn-predominantly-arise-due-to-dust-in-the-host-galaxy/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Mass Measurements of Black Holes in X-Ray Transients: Is There a Mass Gap?</title>
		<link>http://voxcharta.org/2012/05/09/mass-measurements-of-black-holes-in-x-ray-transients-is-there-a-mass-gap/</link>
		<comments>http://voxcharta.org/2012/05/09/mass-measurements-of-black-holes-in-x-ray-transients-is-there-a-mass-gap/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:47:13 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[careful examination]]></category>
		<category><![CDATA[donor]]></category>
		<category><![CDATA[gap]]></category>
		<category><![CDATA[hole mass]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[mass distribution]]></category>
		<category><![CDATA[mass gap]]></category>
		<category><![CDATA[mass measurement]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[odot]]></category>
		<category><![CDATA[orbital inclination]]></category>
		<category><![CDATA[paucity]]></category>
		<category><![CDATA[soft x]]></category>
		<category><![CDATA[systematic error]]></category>
		<category><![CDATA[transients]]></category>
		<category><![CDATA[typical data]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/mass-measurements-of-black-holes-in-x-ray-transients-is-there-a-mass-gap/</guid>
		<description><![CDATA[We explore possible systematic errors in the mass measurements of stellar mass black holes. We find that significant errors can arise from the assumption of zero or constant emission from the accretion flow, which is commonly used when determining orbital inclination by modelling ellipsoidal variations. For A0620-00, the system with the best available data, we [...]]]></description>
			<content:encoded><![CDATA[<p>We explore possible systematic errors in the mass measurements of stellar mass black holes. We find that significant errors can arise from the assumption of zero or constant emission from the accretion flow, which is commonly used when determining orbital inclination by modelling ellipsoidal variations. For A0620-00, the system with the best available data, we show that typical data sets and analysis procedures can lead to systematic underestimates of the inclination by ten degrees or more. A careful examination of the available data for the 15 other X-ray transients with low-mass donors suggests that this effect may significantly reduce the black hole mass estimates in several other cases, most notably that of GRO J0422+32. With these revisions, our analysis of the black hole mass distribution in soft X-ray transients does not suggest any &#8220;mass gap&#8221; between the low end of the distribution and the maximum theoretical neutron star mass, as has been identified in previous studies. Nevertheless, we find that the mass distribution retains other previously identified characteristics, namely a peak around 8M\odot, a paucity of sources with masses below 5M\odot, and a sharp drop-off above 10M\odot.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/mass-measurements-of-black-holes-in-x-ray-transients-is-there-a-mass-gap/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Redshift Evolution of the Relation between Stellar Mass, Star Formation Rate, and Gas Metallicity of Galaxies</title>
		<link>http://voxcharta.org/2012/05/09/the-redshift-evolution-of-the-relation-between-stellar-mass-star-formation-rate-and-gas-metallicity-of-galaxies/</link>
		<comments>http://voxcharta.org/2012/05/09/the-redshift-evolution-of-the-relation-between-stellar-mass-star-formation-rate-and-gas-metallicity-of-galaxies/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:44:22 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[digital sky survey]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[mass star]]></category>
		<category><![CDATA[metallicity]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[redshift galaxies]]></category>
		<category><![CDATA[sfr]]></category>
		<category><![CDATA[sky survey data]]></category>
		<category><![CDATA[sloan digital]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[stellar mass]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/the-redshift-evolution-of-the-relation-between-stellar-mass-star-formation-rate-and-gas-metallicity-of-galaxies/</guid>
		<description><![CDATA[We investigate the relation between stellar mass ($M_\star$), star formation rate (SFR), and metallicity of galaxies, so called the fundamental metallicity relation, in the galaxy sample of Sloan Digital Sky Survey Data Release 7. We separate the galaxies into narrow redshift bins and compare the relation at different redshifts, and find statistically significant ($&#62; 99$%) [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate the relation between stellar mass ($M_\star$), star formation rate (SFR), and metallicity of galaxies, so called the fundamental metallicity relation, in the galaxy sample of Sloan Digital Sky Survey Data Release 7. We separate the galaxies into narrow redshift bins and compare the relation at different redshifts, and find statistically significant ($&gt; 99$%) evolution which is not explained solely by the effect of fiber covering fraction. In the current sample of low redshift galaxies, galaxies with different $M_\star$, and SFR are sampled from different redshifts. The separation of the intrinsic relation from the redshift evolution effect is a crucial issue to understand evolution of galaxies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/the-redshift-evolution-of-the-relation-between-stellar-mass-star-formation-rate-and-gas-metallicity-of-galaxies/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Flow Through Campylotic Media [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/09/flow-through-campylotic-media-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/09/flow-through-campylotic-media-cross-listing/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:44:04 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[critical value]]></category>
		<category><![CDATA[curved space]]></category>
		<category><![CDATA[fluid flow]]></category>
		<category><![CDATA[functional expressions]]></category>
		<category><![CDATA[interference]]></category>
		<category><![CDATA[kinetic model]]></category>
		<category><![CDATA[perturbation]]></category>
		<category><![CDATA[ricci curvature]]></category>
		<category><![CDATA[spatial extent]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/flow-through-campylotic-media-cross-listing/</guid>
		<description><![CDATA[We have found that the relation between the flow through campylotic (generically curved) media, consisting of randomly located curvature perturbations, and the average Ricci scalar of the system exhibits two distinct functional expressions (hysteresis), depending on whether the typical spatial extent of the curvature perturbation lies above or below the critical value maximizing the overall [...]]]></description>
			<content:encoded><![CDATA[<p>We have found that the relation between the flow through campylotic (generically curved) media, consisting of randomly located curvature perturbations, and the average Ricci scalar of the system exhibits two distinct functional expressions (hysteresis), depending on whether the typical spatial extent of the curvature perturbation lies above or below the critical value maximizing the overall Ricci curvature. Furthermore, the flow through such systems as a function of the number of curvature perturbations presents a sublinear behavior for large concentrations due to the interference between curvature perturbations that, consequently, produces a less curved space. For the purpose of this study, we have developed and validated a lattice kinetic model capable of describing fluid flow in arbitrarily curved manifolds, which allows to deal with highly complex spaces in a very compact and efficient way.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/flow-through-campylotic-media-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>High Resolution IR Observations of the Starburst Ring in NGC 7552 &#8212; One Ring to Rule Them All?</title>
		<link>http://voxcharta.org/2012/05/09/high-resolution-ir-observations-of-the-starburst-ring-in-ngc-7552-one-ring-to-rule-them-all/</link>
		<comments>http://voxcharta.org/2012/05/09/high-resolution-ir-observations-of-the-starburst-ring-in-ngc-7552-one-ring-to-rule-them-all/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:42:57 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[angular resolution]]></category>
		<category><![CDATA[cluster formation]]></category>
		<category><![CDATA[continuous inflow]]></category>
		<category><![CDATA[fundamental limitation]]></category>
		<category><![CDATA[galactic bar]]></category>
		<category><![CDATA[galaxy ngc]]></category>
		<category><![CDATA[gas density]]></category>
		<category><![CDATA[hst observation]]></category>
		<category><![CDATA[integral field]]></category>
		<category><![CDATA[massive cluster]]></category>
		<category><![CDATA[myr]]></category>
		<category><![CDATA[pah]]></category>
		<category><![CDATA[ring galaxy]]></category>
		<category><![CDATA[sinfoni]]></category>
		<category><![CDATA[spatial scale]]></category>
		<category><![CDATA[starburst ring]]></category>
		<category><![CDATA[visir]]></category>
		<category><![CDATA[vlt]]></category>
		<category><![CDATA[wavelength]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/high-resolution-ir-observations-of-the-starburst-ring-in-ngc-7552-one-ring-to-rule-them-all/</guid>
		<description><![CDATA[We observed the ring galaxy NGC 7552 with the mid-infrared (MIR) instrument VISIR at an angular resolution of 0.3&#8243;- 0.4&#8243; and with the near-infrared (NIR) integral-field spectrograph SINFONI on the VLT, and complement these observations with data from ISO and Spitzer. The starburst ring is clearly detected at MIR wavelengths at the location of the [...]]]></description>
			<content:encoded><![CDATA[<p>We observed the ring galaxy NGC 7552 with the mid-infrared (MIR) instrument VISIR at an angular resolution of 0.3&#8243;- 0.4&#8243; and with the near-infrared (NIR) integral-field spectrograph SINFONI on the VLT, and complement these observations with data from ISO and Spitzer. The starburst ring is clearly detected at MIR wavelengths at the location of the dust-extincted, dark ring seen in HST observations. This &#8220;ring&#8221;, however, is a rather complex annular region of more than 100 parsec width. We find a large fraction of diffuse [Ne II] and PAH emission in the central region that is not associated with the MIR peaks on spatial scales of \sim30 pc. We do not detect MIR emission from the nucleus of NGC 7552, which is very prominent at optical and NIR continuum wavelengths. However, we have identified nine unresolved MIR peaks within the ring. The average extinction of these peaks is A(V)=7.4 and their total infrared luminosity is L(IR) = 2.1*10^10 Lo. The properties of these peaks are typical for MIR-selected massive clusters found in other galaxies. The ages of the MIR-selected clusters are in the range of 5.9\pm0.3 Myr. The age spread among the clusters of 0.8 Myr is small compared to the travel time of \sim5.6 Myr for half an orbit within the starburst ring. We find no strong evidence for a scenario where the continuous inflow of gas leads to the ongoing formation of massive clusters at the contact points between galactic bar and starburst ring. Instead, it appears more likely that the gas density build up more gradually over larger ring segments, and that the local physical conditions govern cluster formation. We note that the fundamental limitation on the accurate derivation of cluster age, mass and IMF slope is the lack of higher angular resolution.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/high-resolution-ir-observations-of-the-starburst-ring-in-ngc-7552-one-ring-to-rule-them-all/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Modeling the X-rays Resulting from High Velocity Clouds</title>
		<link>http://voxcharta.org/2012/05/09/modeling-the-x-rays-resulting-from-high-velocity-clouds/</link>
		<comments>http://voxcharta.org/2012/05/09/modeling-the-x-rays-resulting-from-high-velocity-clouds/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:41:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[enhancement]]></category>
		<category><![CDATA[environmental gas]]></category>
		<category><![CDATA[equilibrium]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[high velocity]]></category>
		<category><![CDATA[hydrodynamic]]></category>
		<category><![CDATA[magellanic stream]]></category>
		<category><![CDATA[magnetohydrodynamic simulation]]></category>
		<category><![CDATA[plasma]]></category>
		<category><![CDATA[productivity]]></category>
		<category><![CDATA[scenarios]]></category>
		<category><![CDATA[temperature]]></category>
		<category><![CDATA[velocity clouds]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xmm newton]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/modeling-the-x-rays-resulting-from-high-velocity-clouds/</guid>
		<description><![CDATA[With the goal of understanding why X-rays have been reported near some high velocity clouds, we perform detailed 3 dimensional hydrodynamic and magnetohydrodynamic simulations of clouds interacting with environmental gas like that in the Galaxy&#8217;s thick disk/halo or the Magellanic Stream. We examine 2 scenarios. In the first, clouds travel fast enough to shock-heat warm [...]]]></description>
			<content:encoded><![CDATA[<p>With the goal of understanding why X-rays have been reported near some high velocity clouds, we perform detailed 3 dimensional hydrodynamic and magnetohydrodynamic simulations of clouds interacting with environmental gas like that in the Galaxy&#8217;s thick disk/halo or the Magellanic Stream. We examine 2 scenarios. In the first, clouds travel fast enough to shock-heat warm environmental gas. In this scenario, the X-ray productivity depends strongly on the speed of the cloud and the radiative cooling rate. In order to shock-heat environmental gas to temperatures of &gt; or = 10^6 K, cloud speeds of &gt; or = 300 km/s are required. If cooling is quenched, then the shock-heated ambient gas is X-ray emissive, producing bright X-rays in the 1/4 keV band and some X-rays in the 3/4 keV band due to O VII and other ions. If, in contrast, the radiative cooling rate is similar to that of collisional ionizational equilibrium plasma with solar abundances, then the shocked gas is only mildly bright and for only about 1 Myr. The predicted count rates for the non-radiative case are bright enough to explain the count rate observed with XMM-Newton toward a Magellanic Stream cloud and some enhancement in the ROSAT 1/4 keV count rate toward Complex C, while the predicted count rates for the fully radiative case are not. In the second scenario, the clouds travel through and mix with hot ambient gas. The mixed zone can contain hot gas, but the hot portion of the mixed gas is not as bright as those from the shock-heating scenario.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/modeling-the-x-rays-resulting-from-high-velocity-clouds/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Properties and Spatial Distribution of Dust Emission in the Crab Nebula</title>
		<link>http://voxcharta.org/2012/05/09/properties-and-spatial-distribution-of-dust-emission-in-the-crab-nebula/</link>
		<comments>http://voxcharta.org/2012/05/09/properties-and-spatial-distribution-of-dust-emission-in-the-crab-nebula/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:38:51 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[amorphous carbon]]></category>
		<category><![CDATA[carbon grains]]></category>
		<category><![CDATA[continuum emission]]></category>
		<category><![CDATA[core collapse supernova]]></category>
		<category><![CDATA[crab nebula]]></category>
		<category><![CDATA[dust emission]]></category>
		<category><![CDATA[dust grains]]></category>
		<category><![CDATA[emission spectra]]></category>
		<category><![CDATA[filament]]></category>
		<category><![CDATA[infrared spectrograph]]></category>
		<category><![CDATA[ir spectra]]></category>
		<category><![CDATA[line emission]]></category>
		<category><![CDATA[silicate]]></category>
		<category><![CDATA[solar mass]]></category>
		<category><![CDATA[spatial distribution]]></category>
		<category><![CDATA[spitzer space telescope]]></category>
		<category><![CDATA[supernova remnant]]></category>
		<category><![CDATA[synchrotron nebula]]></category>
		<category><![CDATA[theoretical model]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/properties-and-spatial-distribution-of-dust-emission-in-the-crab-nebula/</guid>
		<description><![CDATA[Recent infrared (IR) observations of freshly-formed dust in supernova remnants (SNRs) have yielded significantly lower dust masses than predicted by theoretical models and measured from high redshift observations. The Crab Nebula&#8217;s pulsar wind is thought to be sweeping up freshly-formed supernova (SN) dust along with the ejected gas. The evidence for this dust was found [...]]]></description>
			<content:encoded><![CDATA[<p>Recent infrared (IR) observations of freshly-formed dust in supernova remnants (SNRs) have yielded significantly lower dust masses than predicted by theoretical models and measured from high redshift observations. The Crab Nebula&#8217;s pulsar wind is thought to be sweeping up freshly-formed supernova (SN) dust along with the ejected gas. The evidence for this dust was found in the form of an IR excess in the integrated spectrum of the Crab and in extinction against the synchrotron nebula that revealed the presence of dust in the filament cores. We present the first spatially resolved emission spectra of dust in the Crab Nebula acquired with the Infrared Spectrograph aboard the Spitzer Space Telescope. The IR spectra are dominated by synchrotron emission and show forbidden line emission from from S, Si, Ne, Ar, O, Fe, and Ni. We derived a synchrotron spectral map from the 3.6 and 4.5 microns images, and subtracted this contribution from our data to produce a map of the residual continuum emission from dust. The dust emission appears to be concentrated along the ejecta filaments and is well described by an amorphous carbon or silicate grain compositions. We find a dust temperature of 55+/- 4 K for silicates and 60 +/- 7 K for carbon grains. The total estimated dust mass is 0.0012-0.012 solar masses, well below the theoretical dust yield predicted for a core-collapse supernova. Our grain heating model implies that the dust grain radii are relatively small, unlike what is expected for dust grains formed in a Type IIP SN.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/properties-and-spatial-distribution-of-dust-emission-in-the-crab-nebula/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>On the origin of LS 5039 and PSR J1825-1446</title>
		<link>http://voxcharta.org/2012/05/09/on-the-origin-of-ls-5039-and-psr-j1825-1446/</link>
		<comments>http://voxcharta.org/2012/05/09/on-the-origin-of-ls-5039-and-psr-j1825-1446/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:38:21 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[ascension and declination]]></category>
		<category><![CDATA[characteristic age]]></category>
		<category><![CDATA[conclusion]]></category>
		<category><![CDATA[distance]]></category>
		<category><![CDATA[galactic rotation]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[high velocity]]></category>
		<category><![CDATA[kyr]]></category>
		<category><![CDATA[myr]]></category>
		<category><![CDATA[ob2]]></category>
		<category><![CDATA[optical observation]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[proper motion]]></category>
		<category><![CDATA[pulsar psr]]></category>
		<category><![CDATA[right ascension and declination]]></category>
		<category><![CDATA[snr]]></category>
		<category><![CDATA[supernova remnant]]></category>
		<category><![CDATA[synchronization]]></category>
		<category><![CDATA[trajectory]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/on-the-origin-of-ls-5039-and-psr-j1825-1446/</guid>
		<description><![CDATA[Context. The gamma-ray binary LS 5039 and the isolated pulsar PSR J1825-1446 were proposed to have been formed in the supernova remnant (SNR) G016.8-01.1. Aims. We aim to obtain the Galactic trajectory of LS 5039 and PSR J1825-1446 to find their origin in the Galaxy, and in particular to check their association with SNR G016.8-01.1 [...]]]></description>
			<content:encoded><![CDATA[<p>Context. The gamma-ray binary LS 5039 and the isolated pulsar PSR J1825-1446 were proposed to have been formed in the supernova remnant (SNR) G016.8-01.1. Aims. We aim to obtain the Galactic trajectory of LS 5039 and PSR J1825-1446 to find their origin in the Galaxy, and in particular to check their association with SNR G016.8-01.1 to restrict their age. Methods. By means of radio and optical observations we obtained the proper motion and the space velocity of the sources. Results. The proper motion of PSR J1825-1446 corresponds to a transverse space velocity of 690 km/s at a distance of 5 kpc. Its Galactic velocity at different distances is not compatible with the expected Galactic rotation. The velocity and characteristic age of PSR J1825-1446 make it incompatible with SNR G016.8-01.1. There are no clear OB associations or SNRs crossing the past trajectory of PSR J1825-1446. We estimate the age of the pulsar to be 80-245 kyr, which is compatible with its characteristic age. The proper motion of LS 5039 is 7.09 and -8.82 mas/yr in right ascension and declination, respectively. The association of LS 5039 with SNR G016.8-01.1 is unlikely, although we cannot to discard it. The system would have had to be formed in the association Ser OB2 (at 2.0 kpc) if the age of the system is 1.0-1.2 Myr, or in the association Sct OB3 (distance 1.5-2 kpc) for an age of 0.1-0.2 Myr. If the system were not formed close to Ser OB2, the pseudo-synchronization of the orbit would be unlikely. Conclusions. PSR J1825-1446 is a high-velocity isolated pulsar ejected from the Galaxy. The distance to LS 5039, which needs to be constrained by future astrometric missions such as Gaia, is a key parameter for restricting its origin and age.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/on-the-origin-of-ls-5039-and-psr-j1825-1446/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Radiative and Momentum Based Mechanical AGN Feedback in a 3-Dimensional Galaxy Evolution Code</title>
		<link>http://voxcharta.org/2012/05/09/radiative-and-momentum-based-mechanical-agn-feedback-in-a-3-dimensional-galaxy-evolution-code/</link>
		<comments>http://voxcharta.org/2012/05/09/radiative-and-momentum-based-mechanical-agn-feedback-in-a-3-dimensional-galaxy-evolution-code/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:38:12 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[analytic results]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[bondi]]></category>
		<category><![CDATA[di matteo]]></category>
		<category><![CDATA[feedback model]]></category>
		<category><![CDATA[fluctuation]]></category>
		<category><![CDATA[galaxy evolution]]></category>
		<category><![CDATA[host galaxy]]></category>
		<category><![CDATA[isolated galaxies]]></category>
		<category><![CDATA[mechanical energy]]></category>
		<category><![CDATA[new model]]></category>
		<category><![CDATA[radiative]]></category>
		<category><![CDATA[ray radiation]]></category>
		<category><![CDATA[sph simulation]]></category>
		<category><![CDATA[thermal feedback]]></category>
		<category><![CDATA[wind velocity]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/radiative-and-momentum-based-mechanical-agn-feedback-in-a-3-dimensional-galaxy-evolution-code/</guid>
		<description><![CDATA[We study the growth of black holes (BHs) in galaxies using three-dimensional smoothed particle hydrodynamic (SPH) simulations with new implementations of the momentum mechanical feedback, and restriction of accreted elements to those that are gravitationally bound to the BH. We also include the feedback from the X-ray radiation emitted bythe black hole, which heats the [...]]]></description>
			<content:encoded><![CDATA[<p>We study the growth of black holes (BHs) in galaxies using three-dimensional smoothed particle hydrodynamic (SPH) simulations with new implementations of the momentum mechanical feedback, and restriction of accreted elements to those that are gravitationally bound to the BH. We also include the feedback from the X-ray radiation emitted bythe black hole, which heats the surrounding gas in the host galaxies, and adds radial momentum to the fluid. We perform simulations of isolated galaxies and merging galaxies and test various feedback models with the new treatment of the Bondi radius criterion. We find that overall the black hole growth is similar to what has been obtained by earlier workers using the Springel, Di Matteo, &amp; Hernquist algorithms. However, the outflowing wind velocities and mechanical energy emitted by winds are considerably higher (v_w ~ 1000-3000 km/s) compared to the standard thermal feedback model (v_w ~ 50-100 km/s). While the thermal feedback model emits only 0.1 % of BH released energy in winds, the momentum feedback model emits more than 30 % of the total energy released by the BH in winds. In the momentum feedback model, the degree of fluctuation in both radiant and wind output is considerably larger than in the standard treatments. We check that the new model of the BH mass accretion agrees with analytic results for the standard Bondi problem.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/radiative-and-momentum-based-mechanical-agn-feedback-in-a-3-dimensional-galaxy-evolution-code/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>MaGICC Disks: Matching Observed Galaxy Relationships Over a Wide Stellar Mass Range [Replacement]</title>
		<link>http://voxcharta.org/2012/05/09/magicc-disks-matching-observed-galaxy-relationships-over-a-wide-stellar-mass-range-replacement/</link>
		<comments>http://voxcharta.org/2012/05/09/magicc-disks-matching-observed-galaxy-relationships-over-a-wide-stellar-mass-range-replacement/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:35:31 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorption line]]></category>
		<category><![CDATA[baryonic]]></category>
		<category><![CDATA[core]]></category>
		<category><![CDATA[cosmological context]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[dependence]]></category>
		<category><![CDATA[disc galaxies]]></category>
		<category><![CDATA[galaxy properties]]></category>
		<category><![CDATA[interplay]]></category>
		<category><![CDATA[key role]]></category>
		<category><![CDATA[large scale]]></category>
		<category><![CDATA[mass range]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[physical model]]></category>
		<category><![CDATA[rotation curves]]></category>
		<category><![CDATA[rotation velocity]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[surface brightness]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/magicc-disks-matching-observed-galaxy-relationships-over-a-wide-stellar-mass-range-replacement/</guid>
		<description><![CDATA[We use the same physical model to simulate four galaxies that match the relation between stellar and total mass, over a mass range that includes the vast majority of disc galaxies. The resultant galaxies, part of the Making Galaxies in a Cosmological Context (MaGICC) program, also match observed relations between luminosity, rotation velocity, size, colour, [...]]]></description>
			<content:encoded><![CDATA[<p>We use the same physical model to simulate four galaxies that match the relation between stellar and total mass, over a mass range that includes the vast majority of disc galaxies. The resultant galaxies, part of the Making Galaxies in a Cosmological Context (MaGICC) program, also match observed relations between luminosity, rotation velocity, size, colour, star formation rate, HI mass, baryonic mass, and metallicity. Radiation from massive stars and supernova energy regulate star formation and drive outflows, balancing the complex interplay between cooling gas, star formation, large scale outflows, and recycling of gas in a manner which correctly scales with the mass of the galaxy. Outflows also play a key role in simulating galaxies with exponential surface brightness profiles, flat rotation curves and dark matter cores. Our study implies that large scale outflows are the primary driver of the dependence of disc galaxy properties on mass. We show that the amount of outflows invoked in our model is required to meet the constraints provided by observations of OVI absorption lines in the circum-galactic-media of local galaxies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/magicc-disks-matching-observed-galaxy-relationships-over-a-wide-stellar-mass-range-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>New gamma ray signal from gravitationally boosted neutralinos at the galactic center [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/09/new-gamma-ray-signal-from-gravitationally-boosted-neutralinos-at-the-galactic-center-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/09/new-gamma-ray-signal-from-gravitationally-boosted-neutralinos-at-the-galactic-center-cross-listing/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:31:06 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[collision energy]]></category>
		<category><![CDATA[dark matter particles]]></category>
		<category><![CDATA[galactic center]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[massive black hole]]></category>
		<category><![CDATA[neutralino]]></category>
		<category><![CDATA[observability]]></category>
		<category><![CDATA[spectrum]]></category>
		<category><![CDATA[supersymmetric models]]></category>
		<category><![CDATA[tau lepton]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/new-gamma-ray-signal-from-gravitationally-boosted-neutralinos-at-the-galactic-center-cross-listing/</guid>
		<description><![CDATA[We discuss on the possibility that colliding dark matter particles in the form of neutralinos may be gravitationally boosted near the super-massive black hole at the galactic center so that they can have enough collision energy to annihilate into a stau pair. Since in some phenomenologically favored supersymmetric models the mass splitting between the neutralino [...]]]></description>
			<content:encoded><![CDATA[<p>We discuss on the possibility that colliding dark matter particles in the form of neutralinos may be gravitationally boosted near the super-massive black hole at the galactic center so that they can have enough collision energy to annihilate into a stau pair. Since in some phenomenologically favored supersymmetric models the mass splitting between the neutralino and the lightest stau, one of the two scalar superpartners of the tau lepton, is a few GeVs, this channel may be allowed. In addition, staus can only decay into a tau lepton and another neutralino. We calculate the gamma-ray spectrum and flux generated by the tau pair discussing the observability of the obtained features.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/new-gamma-ray-signal-from-gravitationally-boosted-neutralinos-at-the-galactic-center-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Inverse dynamical population synthesis: Constraining the initial conditions of young stellar clusters by studying their binary populations</title>
		<link>http://voxcharta.org/2012/05/08/inverse-dynamical-population-synthesis-constraining-the-initial-conditions-of-young-stellar-clusters-by-studying-their-binary-populations/</link>
		<comments>http://voxcharta.org/2012/05/08/inverse-dynamical-population-synthesis-constraining-the-initial-conditions-of-young-stellar-clusters-by-studying-their-binary-populations/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:47:17 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[binary properties]]></category>
		<category><![CDATA[binary star]]></category>
		<category><![CDATA[chamaeleon]]></category>
		<category><![CDATA[clump]]></category>
		<category><![CDATA[dynamical evolution]]></category>
		<category><![CDATA[ecl]]></category>
		<category><![CDATA[globular cluster]]></category>
		<category><![CDATA[half mass]]></category>
		<category><![CDATA[initial condition]]></category>
		<category><![CDATA[mass radius]]></category>
		<category><![CDATA[molecular cloud]]></category>
		<category><![CDATA[parameter distribution]]></category>
		<category><![CDATA[pc 3]]></category>
		<category><![CDATA[progenitor]]></category>
		<category><![CDATA[rho ophiuchus]]></category>
		<category><![CDATA[scorpius]]></category>
		<category><![CDATA[star cluster]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[stellar cluster]]></category>
		<category><![CDATA[stellar mass]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/inverse-dynamical-population-synthesis-constraining-the-initial-conditions-of-young-stellar-clusters-by-studying-their-binary-populations/</guid>
		<description><![CDATA[Binary populations in young star clusters show multiplicity fractions both lower and up to twice as high as those observed in the Galactic field. We follow the evolution of a population of binary stars in dense and loose star clusters starting with an invariant initial binary population and a formal multiplicity fraction of unity, and [...]]]></description>
			<content:encoded><![CDATA[<p>Binary populations in young star clusters show multiplicity fractions both lower and up to twice as high as those observed in the Galactic field. We follow the evolution of a population of binary stars in dense and loose star clusters starting with an invariant initial binary population and a formal multiplicity fraction of unity, and demonstrate that these models can explain the observed binary properties in Taurus, Rho-Ophiuchus, Chamaeleon, Orion, IC 348, Upper Scorpius A, Praesepe, and the Pleiades. The model needs to consider solely different birth densities for these regions. The evolved theoretical orbital-parameter distributions are highly probable parent distributions for the observed ones. We constrain the birth conditions (stellar mass, M_ecl, and half-mass radius, r_h) for the derived progenitors of the star clusters and the overall present-day binary fractions allowed by the present model. The results compare very well with properties of molecular cloud clumps on the verge of star formation. Combining these with previously and independently obtained constraints on the birth densities of globular clusters, we identify a weak stellar mass &#8212; half-mass radius correlation for cluster-forming cloud clumps, r_h / pc ~ (M_ecl / M_sun)^(0.13+-0.04). The ability of the model to reproduce the binary properties in all the investigated young objects, covering present-day densities from 1-10 stars pc^-3 (Taurus) to 2&#215;10^4 stars pc^-3 (Orion), suggests that environment-dependent dynamical evolution plays an important role in shaping the present-day properties of binary populations in star clusters, and that the initial binary properties may not vary dramatically between different environments.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/inverse-dynamical-population-synthesis-constraining-the-initial-conditions-of-young-stellar-clusters-by-studying-their-binary-populations/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Self-gravitating equilibrium models of dwarf galaxies and the minimum mass for star formation</title>
		<link>http://voxcharta.org/2012/05/08/self-gravitating-equilibrium-models-of-dwarf-galaxies-and-the-minimum-mass-for-star-formation/</link>
		<comments>http://voxcharta.org/2012/05/08/self-gravitating-equilibrium-models-of-dwarf-galaxies-and-the-minimum-mass-for-star-formation/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:44:40 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[alpha sigma]]></category>
		<category><![CDATA[baryon]]></category>
		<category><![CDATA[chemical evolution]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[dgs]]></category>
		<category><![CDATA[dwarf galaxy]]></category>
		<category><![CDATA[equilibrium model]]></category>
		<category><![CDATA[equilibrium system]]></category>
		<category><![CDATA[galaxy formation]]></category>
		<category><![CDATA[gas temperature]]></category>
		<category><![CDATA[gravitational potential]]></category>
		<category><![CDATA[hand models]]></category>
		<category><![CDATA[initial model]]></category>
		<category><![CDATA[minimum mass]]></category>
		<category><![CDATA[model galaxy]]></category>
		<category><![CDATA[momentum equation]]></category>
		<category><![CDATA[natural outcome]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[steady state]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/self-gravitating-equilibrium-models-of-dwarf-galaxies-and-the-minimum-mass-for-star-formation/</guid>
		<description><![CDATA[We construct a series of model galaxies in rotational equilibrium consisting of gas, stars, and a fixed dark matter (DM) halo and study how these equilibrium systems depend on the mass and form of the DM halo, gas temperature, non-thermal and rotation support against gravity, and also on the redshift of galaxy formation. For every [...]]]></description>
			<content:encoded><![CDATA[<p>We construct a series of model galaxies in rotational equilibrium consisting of gas, stars, and a fixed dark matter (DM) halo and study how these equilibrium systems depend on the mass and form of the DM halo, gas temperature, non-thermal and rotation support against gravity, and also on the redshift of galaxy formation. For every model galaxy we find the minimum gas mass M_g^min required to achieve a state in which star formation (SF) is allowed according to contemporary SF criteria. The obtained M_g^min&#8211;M_DM relations are compared against the baryon-to-DM mass relation M_b&#8211;M_DM inferred from the \LambdaCDM theory and WMAP4 data. Our aim is to construct realistic initial models of dwarf galaxies (DGs), which take into account the gas self-gravity and can be used as a basis to study the dynamical and chemical evolution of DGs. Rotating equilibria are found by solving numerically the steady-state momentum equation for the gas component in the combined gravitational potential of gas, stars, and DM halo using a forward substitution procedure. We find that for a given M_DM the value of M_g^min depends crucially on the gas temperature T_g, gas spin parameter \alpha, degree of non-thermal support \sigma_eff, and somewhat on the redshift for galaxy formation z_gf. Depending on the actual values of T_g, \alpha, \sigma_eff, and z_gf, model galaxies may have M_g^min that are either greater or smaller than M_b. Galaxies with M_DM \ga 10^9 M_sun are usually characterized by M_g^min \la M_b, implying that SF in such objects is a natural outcome as the required gas mass is consistent with what is available according to the \LambdaCDM theory. On the other hand, models with M_DM \la 10^9 M_sun are often characterized by M_g^min &gt;&gt; M_b, implying that they need much more gas than available to achieve a state in which SF is allowed. Abridged.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/self-gravitating-equilibrium-models-of-dwarf-galaxies-and-the-minimum-mass-for-star-formation/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Tidal Tails of Minor Mergers: Star Formation Efficiency in the Western Tail of NGC 2782</title>
		<link>http://voxcharta.org/2012/05/08/tidal-tails-of-minor-mergers-star-formation-efficiency-in-the-western-tail-of-ngc-2782/</link>
		<comments>http://voxcharta.org/2012/05/08/tidal-tails-of-minor-mergers-star-formation-efficiency-in-the-western-tail-of-ngc-2782/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:43:47 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[dense region]]></category>
		<category><![CDATA[disk galaxy]]></category>
		<category><![CDATA[galaxy evolution explorer]]></category>
		<category><![CDATA[gas density]]></category>
		<category><![CDATA[global star formation]]></category>
		<category><![CDATA[kiloparsec]]></category>
		<category><![CDATA[mass ratio]]></category>
		<category><![CDATA[mass star]]></category>
		<category><![CDATA[metallicity]]></category>
		<category><![CDATA[myr]]></category>
		<category><![CDATA[narrowband]]></category>
		<category><![CDATA[orders of magnitude]]></category>
		<category><![CDATA[sfr]]></category>
		<category><![CDATA[spiral ngc]]></category>
		<category><![CDATA[star cluster]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[tidal debris]]></category>
		<category><![CDATA[tidal tail]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/tidal-tails-of-minor-mergers-star-formation-efficiency-in-the-western-tail-of-ngc-2782/</guid>
		<description><![CDATA[While major mergers and their tidal debris are well studied, they are less common than minor mergers (mass ratios &#60; 0.3). The peculiar spiral NGC 2782 is the result of a merger between two disk galaxies with a mass ratio of ~4:1 occurring ~200 Myr ago. This merger produced a molecular and H I-rich, optically [...]]]></description>
			<content:encoded><![CDATA[<p>While major mergers and their tidal debris are well studied, they are less common than minor mergers (mass ratios &lt; 0.3). The peculiar spiral NGC 2782 is the result of a merger between two disk galaxies with a mass ratio of ~4:1 occurring ~200 Myr ago. This merger produced a molecular and H I-rich, optically bright eastern tail and an H I-rich, optically faint western tail. Non-detection of CO in the western tail by Braine et al. suggested that star formation had not yet begun to occur in that tidal tail. However, deep H{\alpha} narrowband images show evidence of recent star formation in the western tail. Across the entire western tail, we find the global star formation rate per unit area ({\Sigma}SFR) to be several orders of magnitude less than expected from the total gas density. Together with extended FUV+NUV emission from Galaxy Evolution Explorer along the tail, this indicates a low global star formation efficiency in the tidal tail producing lower mass star clusters. The H II region that we observed has a local (few-kiloparsec scale) {\Sigma}SFR from H{\alpha} that is less than that expected from the total gas density, which is consistent with other observations of tidal debris. The star formation efficiency of this H II region inferred from the total gas density is low, but normal when inferred from the molecular gas density. These results suggest the presence of a very small, locally dense region in the western tail of NGC 2782 or of a low-metallicity and/or low-pressure star-forming region.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/tidal-tails-of-minor-mergers-star-formation-efficiency-in-the-western-tail-of-ngc-2782/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Broad-band spectral analysis of the Galactic Ridge X-ray Emission</title>
		<link>http://voxcharta.org/2012/05/08/broad-band-spectral-analysis-of-the-galactic-ridge-x-ray-emission/</link>
		<comments>http://voxcharta.org/2012/05/08/broad-band-spectral-analysis-of-the-galactic-ridge-x-ray-emission/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:43:16 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[broad band]]></category>
		<category><![CDATA[chandra satellite]]></category>
		<category><![CDATA[faint point]]></category>
		<category><![CDATA[galactic bulge]]></category>
		<category><![CDATA[high spatial resolution]]></category>
		<category><![CDATA[keV]]></category>
		<category><![CDATA[number density]]></category>
		<category><![CDATA[plasma temperature]]></category>
		<category><![CDATA[point source]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[ray sources]]></category>
		<category><![CDATA[spectral analysis]]></category>
		<category><![CDATA[spectral components]]></category>
		<category><![CDATA[spectral model]]></category>
		<category><![CDATA[spectroscopic]]></category>
		<category><![CDATA[suzaku]]></category>
		<category><![CDATA[thermal emission]]></category>
		<category><![CDATA[white dwarf]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/broad-band-spectral-analysis-of-the-galactic-ridge-x-ray-emission/</guid>
		<description><![CDATA[Detailed spectral analysis of the Galactic X-ray background emission, or the Galactic Ridge X-ray Emission (GRXE), is presented. To study the origin of the emission, broad-band and high-quality GRXE spectra were produced from 18 pointing observations with Suzaku in the Galactic bulge region, with the total exposure of 1 Ms. The spectra were successfully fitted [...]]]></description>
			<content:encoded><![CDATA[<p>Detailed spectral analysis of the Galactic X-ray background emission, or the Galactic Ridge X-ray Emission (GRXE), is presented. To study the origin of the emission, broad-band and high-quality GRXE spectra were produced from 18 pointing observations with Suzaku in the Galactic bulge region, with the total exposure of 1 Ms. The spectra were successfully fitted by a sum of two major spectral components; a spectral model of magnetic accreting white dwarfs with a mass of 0.66 (0.59-0.75) solar, and a softer optically-thin thermal emission with a plasma temperature of 1.2-1.5 keV which is attributable to coronal X-ray sources.   When combined with previous studies which employed high spatial resolution of the Chandra satellite (e.g. Revnivtsev et al. 2009, Nature), the present spectroscopic result gives another strong support to a scenario that the GRXE is essentially an assembly of numerous discrete faint X-ray stars.   The detected GRXE flux in the hard X-ray band was used to estimate the number density of the unresolved hard X-ray sources. When integrated over a luminosity range of ~10^30-10^34 erg/s, the result is consistent with a value which was reported previously by directly resolving faint point sources.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/broad-band-spectral-analysis-of-the-galactic-ridge-x-ray-emission/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Complex Organic Molecules at High Spatial Resolution Toward Orion-KL II: Kinematics</title>
		<link>http://voxcharta.org/2012/05/08/complex-organic-molecules-at-high-spatial-resolution-toward-orion-kl-ii-kinematics/</link>
		<comments>http://voxcharta.org/2012/05/08/complex-organic-molecules-at-high-spatial-resolution-toward-orion-kl-ii-kinematics/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:42:46 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acetone]]></category>
		<category><![CDATA[beam size]]></category>
		<category><![CDATA[chemical processing]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[complex organic molecules]]></category>
		<category><![CDATA[dense region]]></category>
		<category><![CDATA[dynamic region]]></category>
		<category><![CDATA[ethyl]]></category>
		<category><![CDATA[formic acid]]></category>
		<category><![CDATA[gas phase]]></category>
		<category><![CDATA[high spatial resolution]]></category>
		<category><![CDATA[methanol]]></category>
		<category><![CDATA[methyl formate]]></category>
		<category><![CDATA[millimeter wave]]></category>
		<category><![CDATA[molecular images]]></category>
		<category><![CDATA[orion kl]]></category>
		<category><![CDATA[resolution image]]></category>
		<category><![CDATA[resolution observations]]></category>
		<category><![CDATA[sio]]></category>
		<category><![CDATA[spatial distribution]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/complex-organic-molecules-at-high-spatial-resolution-toward-orion-kl-ii-kinematics/</guid>
		<description><![CDATA[It has recently been suggested that chemical processing can shape the spatial distributions of complex molecules in the Orion-KL region and lead to the nitrogen-oxygen &#8220;chemical differentiation&#8221; seen in previous observations of this source. Orion-KL is a very dynamic region, and it is therefore also possible that physical conditions can shape the molecular distributions in [...]]]></description>
			<content:encoded><![CDATA[<p>It has recently been suggested that chemical processing can shape the spatial distributions of complex molecules in the Orion-KL region and lead to the nitrogen-oxygen &#8220;chemical differentiation&#8221; seen in previous observations of this source. Orion-KL is a very dynamic region, and it is therefore also possible that physical conditions can shape the molecular distributions in this source. Only high spatial resolution observations can provide the information needed to disentangle these effects. Here we present millimeter imaging studies of Orion-KL at various beam sizes using the Combined Array for Research in Millimeter-Wave Astronomy (CARMA). We compare molecular images with high spatial resolution images that trace the temperature, continuum column density, and kinematics of the source in order to investigate the effects of physical conditions on molecular distributions. These observations were conducted at \lambda = 3 mm and included transitions of ethyl cyanide [C2H5CN], methyl formate [HCOOCH3], formic acid [HCOOH], acetone [(CH3)2CO], SiO, and methanol [CH3OH]. We find differences in the molecular distributions as a function of each of these factors. These results indicate that acetone may be produced by chemical processing and is robust to large changes in physical conditions, while formic acid is readily destroyed by gas-phase processing in warm and dense regions. We also find that while the spatial distributions of ethyl cyanide and methyl formate are not distinct as is suggested by the concept of &#8220;chemical differentiation&#8221;, local physical conditions shape the small-scale emission structure for these species.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/complex-organic-molecules-at-high-spatial-resolution-toward-orion-kl-ii-kinematics/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Complex Organic Molecules at High Spatial Resolution Toward Orion-KL I: Spatial Scales</title>
		<link>http://voxcharta.org/2012/05/08/complex-organic-molecules-at-high-spatial-resolution-toward-orion-kl-i-spatial-scales/</link>
		<comments>http://voxcharta.org/2012/05/08/complex-organic-molecules-at-high-spatial-resolution-toward-orion-kl-i-spatial-scales/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:42:35 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[complex organic molecules]]></category>
		<category><![CDATA[high spatial resolution]]></category>
		<category><![CDATA[spatial scale]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/complex-organic-molecules-at-high-spatial-resolution-toward-orion-kl-i-spatial-scales/</guid>
		<description><![CDATA[Here we present high spatial resolution (&#60;1 arcsecond) observations of molecular emission in Orion-KL conducted using the Combined Array for Research in Millimeter-Wave Astronomy (CARMA). This work was motivated by recent millimeter continuum imaging studies of this region conducted at a similarly high spatial resolution, which revealed that the bulk of the emission arises from [...]]]></description>
			<content:encoded><![CDATA[<p>Here we present high spatial resolution (&lt;1 arcsecond) observations of molecular emission in Orion-KL conducted using the Combined Array for Research in Millimeter-Wave Astronomy (CARMA). This work was motivated by recent millimeter continuum imaging studies of this region conducted at a similarly high spatial resolution, which revealed that the bulk of the emission arises from numerous compact sources, rather than the larger-scale extended structures typically associated with the Orion Hot Core and Compact Ridge. Given that the spatial extent of molecular emission greatly affects the determination of molecular abundances, it is important to determine the true spatial scale for complex molecules in this region. Additionally, it has recently been suggested that the relative spatial distributions of complex molecules in a source might give insight into the chemical mechanisms that drive complex chemistry in star-forming regions. In order to begin to address these issues, this study seeks to determine the spatial distributions of ethyl cyanide [C2H5CN], dimethyl ether [(CH3)2O], methyl formate [HCOOCH3], formic acid [HCOOH], acetone [(CH3)2CO], SiO, methanol [CH3OH], and methyl cyanide [CH3CN] in Orion-KL at \lambda = 3 mm. We find that for all observed molecules, the molecular emission arises from multiple components of the cloud that include a range of spatial scales and physical conditions. Here we present the results of these observations and discuss the implications for studies of complex molecules in star-forming regions.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/complex-organic-molecules-at-high-spatial-resolution-toward-orion-kl-i-spatial-scales/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Isolated starless cores in IRDCs in the Hi-GAL survey</title>
		<link>http://voxcharta.org/2012/05/08/isolated-starless-cores-in-irdcs-in-the-hi-gal-survey/</link>
		<comments>http://voxcharta.org/2012/05/08/isolated-starless-cores-in-irdcs-in-the-hi-gal-survey/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:38:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[central density]]></category>
		<category><![CDATA[core]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[infrared dark clouds]]></category>
		<category><![CDATA[Monte Carlo]]></category>
		<category><![CDATA[physical parameter]]></category>
		<category><![CDATA[radiation field]]></category>
		<category><![CDATA[radiative transfer code]]></category>
		<category><![CDATA[wavelength]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/isolated-starless-cores-in-irdcs-in-the-hi-gal-survey/</guid>
		<description><![CDATA[In a previous paper we identified cores within infrared dark clouds (IRDCs). We regarded those without embedded sources as the least evolved, and labelled them starless. Here we identify the most isolated starless cores and model them using a three-dimensional, multi-wavelength, Monte Carlo, radiative transfer code. We derive the cores&#8217; physical parameters and discuss the [...]]]></description>
			<content:encoded><![CDATA[<p>In a previous paper we identified cores within infrared dark clouds (IRDCs). We regarded those without embedded sources as the least evolved, and labelled them starless. Here we identify the most isolated starless cores and model them using a three-dimensional, multi-wavelength, Monte Carlo, radiative transfer code. We derive the cores&#8217; physical parameters and discuss the relation between the mass, temperature, density, size and the surrounding interstellar radiation field (ISRF) for the cores. The masses of the cores were found not to correlate with their radial size or central density. The temperature at the surface of a core was seen to depend almost entirely on the level of the ISRF surrounding the core. No correlation was found between the temperature at the centre of a core and its local ISRF. This was seen to depend, instead, on the density and mass of the core.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/isolated-starless-cores-in-irdcs-in-the-hi-gal-survey/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The X-ray behaviour of Fermi/LAT pulsars</title>
		<link>http://voxcharta.org/2012/05/08/the-x-ray-behaviour-of-fermilat-pulsars/</link>
		<comments>http://voxcharta.org/2012/05/08/the-x-ray-behaviour-of-fermilat-pulsars/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:34:37 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[appendix]]></category>
		<category><![CDATA[chapter 3]]></category>
		<category><![CDATA[comprehension]]></category>
		<category><![CDATA[current status]]></category>
		<category><![CDATA[detailed description]]></category>
		<category><![CDATA[energetics]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[multiwavelength observations]]></category>
		<category><![CDATA[nebula]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[population]]></category>
		<category><![CDATA[proposal]]></category>
		<category><![CDATA[proprieties]]></category>
		<category><![CDATA[pulsars]]></category>
		<category><![CDATA[ray observations]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[synergy]]></category>
		<category><![CDATA[thesis]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[zoo]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/the-x-ray-behaviour-of-fermilat-pulsars/</guid>
		<description><![CDATA[More than 40 years after the discovery of Isolated Neutron Stars, the comprehension of their physics is still rather poor. This thesis is based on a program of multiwavelength observations of pulsars which yielded new and important pieces of information about the overall proprieties of this class of sources. The thesis is organized as follows: [...]]]></description>
			<content:encoded><![CDATA[<p>More than 40 years after the discovery of Isolated Neutron Stars, the comprehension of their physics is still rather poor. This thesis is based on a program of multiwavelength observations of pulsars which yielded new and important pieces of information about the overall proprieties of this class of sources. The thesis is organized as follows: &#8211; In chapter 1 we give a very brief overview of the current status of the understanding of Isolated Neutron Stars. We also talk about the Fermi revolution that occurred in the last three years, focusing on the Fermi contribution to the knowledge of neutron stars. Then, we describe the results led by the synergy between X-ray and gamma-ray bands. &#8211; In chapter 2 we report two of our published papers containing the surprising results we obtained for two different radio-quiet pulsars. Such neutron stars, J0007+7303 and J0357+3205, can be considered &#8220;extreme&#8221; in the Fermi pulsars&#8217; zoo due to their energetics and ages. Both the X-ray observations and analyses are very different so that they can be considered as the standing-up examples of all the following analyses. &#8211; In chapter 3 we describe the analysis we done in the X-ray band and briefly report the obtained spectra of each pulsar and its nebula, if present. Then, we study the X-ray and gamma-ray pulsars&#8217; luminosities as a function of their rotational energies and ages in order to find any relationship between these values and any difference between the two populations of radio-quiet and radio-loud pulsars. &#8211; In chapter 4 we report the &#8220;identity card&#8221; of all Fermi pulsars, the detailed description of the analyses done and results obtained for each pulsar. Finally, in appendix we report our accepted proposals of the most significative X-ray observations used in this thesis plus the article on the X-ray behaviour of Fermi/LAT pulsars we published on the Astrophyisical Journal.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/the-x-ray-behaviour-of-fermilat-pulsars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Early-type galaxies at z = 1.3. I. The Lynx supercluster: cluster and groups at z=1.3. Morphology and color-magnitude relation</title>
		<link>http://voxcharta.org/2012/05/08/early-type-galaxies-at-z-1-3-i-the-lynx-supercluster-cluster-and-groups-at-z1-3-morphology-and-color-magnitude-relation/</link>
		<comments>http://voxcharta.org/2012/05/08/early-type-galaxies-at-z-1-3-i-the-lynx-supercluster-cluster-and-groups-at-z1-3-morphology-and-color-magnitude-relation/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:33:52 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bulge]]></category>
		<category><![CDATA[classification method]]></category>
		<category><![CDATA[cluster]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[galaxy masses]]></category>
		<category><![CDATA[galaxy population]]></category>
		<category><![CDATA[group galaxies]]></category>
		<category><![CDATA[lynx]]></category>
		<category><![CDATA[magnitude relation]]></category>
		<category><![CDATA[morphological transformations]]></category>
		<category><![CDATA[morphology]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[remnant]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[type galaxy]]></category>
		<category><![CDATA[zero point]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/early-type-galaxies-at-z-1-3-i-the-lynx-supercluster-cluster-and-groups-at-z1-3-morphology-and-color-magnitude-relation/</guid>
		<description><![CDATA[We confirm the detection of 3 groups in the Lynx supercluster, at z~1.3, and give their redshifts and masses. We study the properties of the group galaxies as compared to the central clusters, RXJ0849+4452 and RXJ0848+4453, selecting 89 galaxies in the clusters and 74 galaxies in the groups. We morphologically classify galaxies by visual inspection, [...]]]></description>
			<content:encoded><![CDATA[<p>We confirm the detection of 3 groups in the Lynx supercluster, at z~1.3, and give their redshifts and masses. We study the properties of the group galaxies as compared to the central clusters, RXJ0849+4452 and RXJ0848+4453, selecting 89 galaxies in the clusters and 74 galaxies in the groups. We morphologically classify galaxies by visual inspection, noting that our early-type galaxy (ETG) sample would have been contaminated at the 30% -40% level by simple automated classification methods (e.g. based on Sersic index). In luminosity selected samples, both clusters and groups show high fractions of Sa galaxies. The ETG fractions never rise above ~50% in the clusters, which is low compared to the fractions observed in clusters at z~1. However, ETG plus Sa fractions are similar to those observed for ETGs in clusters at z~1. Bulge-dominated galaxies visually classified as Sas might also be ETGs with tidal features or merger remnants. They are mainly red and passive, and span a large range in luminosity. Their star formation seems to have been quenched before experiencing a morphological transformation. Because their fraction is smaller at lower redshifts, they might be the spiral population that evolves into ETGs. For mass-selected samples, the ETG fraction show no significant evolution with respect to local clusters, suggesting that morphological transformations occur at lower masses and densities. The ETG mass-size relation shows evolution towards smaller sizes at higher redshift in both clusters and groups, while the late-type mass-size relation matches that observed locally. The group ETG red sequence shows lower zero points and larger scatters than in clusters, both expected to be an indication of a younger galaxy population. The estimated age difference is small when compared to the difference in age at different galaxy masses.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/early-type-galaxies-at-z-1-3-i-the-lynx-supercluster-cluster-and-groups-at-z1-3-morphology-and-color-magnitude-relation/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Comparative study of variational chaos indicators and ODEs&#8217; numerical integrators [Replacement]</title>
		<link>http://voxcharta.org/2012/05/08/comparative-study-of-variational-chaos-indicators-and-odes-numerical-integrators-replacement-2/</link>
		<comments>http://voxcharta.org/2012/05/08/comparative-study-of-variational-chaos-indicators-and-odes-numerical-integrators-replacement-2/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:31:34 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[algorithm]]></category>
		<category><![CDATA[alignment]]></category>
		<category><![CDATA[comparative study]]></category>
		<category><![CDATA[complexity]]></category>
		<category><![CDATA[different systems]]></category>
		<category><![CDATA[differential]]></category>
		<category><![CDATA[exponential growth]]></category>
		<category><![CDATA[fli]]></category>
		<category><![CDATA[numerical integrator]]></category>
		<category><![CDATA[numerical technique]]></category>
		<category><![CDATA[oer]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[ordinary differential equation]]></category>
		<category><![CDATA[oscillator]]></category>
		<category><![CDATA[rli]]></category>
		<category><![CDATA[runge kutta]]></category>
		<category><![CDATA[sali]]></category>
		<category><![CDATA[taylor method]]></category>
		<category><![CDATA[work deals]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/comparative-study-of-variational-chaos-indicators-and-odes-numerical-integrators-replacement-2/</guid>
		<description><![CDATA[The reader can find in the literature a lot of different techniques to study the dynamics of a given system and also, many suitable numerical integrators to compute them. Notwithstanding the recent work of Maffione et al. (2011a) for mappings, a detailed comparison among the widespread indicators of chaos in a general system is still [...]]]></description>
			<content:encoded><![CDATA[<p>The reader can find in the literature a lot of different techniques to study the dynamics of a given system and also, many suitable numerical integrators to compute them. Notwithstanding the recent work of Maffione et al. (2011a) for mappings, a detailed comparison among the widespread indicators of chaos in a general system is still lacking. Such a comparison could lead to select the most efficient algorithms given a certain dynamical problem. Furthermore, in order to choose the appropriate numerical integrators to compute them, more comparative studies among numerical integrators are also needed.   This work deals with both problems. We first extend the work of Maffione et al. (2011) for mappings to the 2D H\&#8217;enon &amp; Heiles (1964) potential, and compare several variational indicators of chaos: the Lyapunov Indicator (LI); the Mean Exponential Growth Factor of Nearby Orbits (MEGNO); the Smaller Alignment Index (SALI) and its generalized version, the Generalized Alignment Index (GALI); the Fast Lyapunov Indicator (FLI) and its variant, the Orthogonal Fast Lyapunov Indicator (OFLI); the Spectral Distance (D) and the Dynamical Spectras of Stretching Numbers (SSNs). We also include in the record the   Relative Lyapunov Indicator (RLI), which is not a variational indicator as the others. Then, we test a numerical technique to integrate   Ordinary Differential Equations (ODEs) based on the Taylor method implemented by Jorba &amp; Zou (2005) (called taylor), and we compare its performance with other two well-known efficient integrators: the Prince &amp; Dormand (1981) implementation of a Runge-Kutta of order 7-8 (DOPRI8) and a Bulirsch-St\&#8221;oer implementation. These tests are run under two very different systems from the complexity of their equations point of view: a triaxial galactic potential model and a perturbed 3D quartic oscillator.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/comparative-study-of-variational-chaos-indicators-and-odes-numerical-integrators-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Free-free Emission and Radio Recombination Lines from Photoevaporating Disks</title>
		<link>http://voxcharta.org/2012/05/07/free-free-emission-and-radio-recombination-lines-from-photoevaporating-disks/</link>
		<comments>http://voxcharta.org/2012/05/07/free-free-emission-and-radio-recombination-lines-from-photoevaporating-disks/#comments</comments>
		<pubDate>Tue, 08 May 2012 01:04:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[centimeter wavelength]]></category>
		<category><![CDATA[central star]]></category>
		<category><![CDATA[continuum emission]]></category>
		<category><![CDATA[dispersal]]></category>
		<category><![CDATA[electron density]]></category>
		<category><![CDATA[energy photons]]></category>
		<category><![CDATA[flow rate]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[inference]]></category>
		<category><![CDATA[infrared observation]]></category>
		<category><![CDATA[instrumentation]]></category>
		<category><![CDATA[intensity]]></category>
		<category><![CDATA[mass flow rate]]></category>
		<category><![CDATA[millimeter]]></category>
		<category><![CDATA[profile]]></category>
		<category><![CDATA[radio recombination lines]]></category>
		<category><![CDATA[Sun]]></category>
		<category><![CDATA[vla observation]]></category>
		<category><![CDATA[wind parameters]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/free-free-emission-and-radio-recombination-lines-from-photoevaporating-disks/</guid>
		<description><![CDATA[Recent infrared observations have demonstrated that photoevaporation driven by high-energy photons from the central star contributes to the dispersal of protoplanetary disks. Here, we show that photoevaporative winds should produce a detectable free-free continuum emission given the range of stellar ionizing photons and X-ray luminosities inferred for young sun-like stars. We point out that VLA [...]]]></description>
			<content:encoded><![CDATA[<p>Recent infrared observations have demonstrated that photoevaporation driven by high-energy photons from the central star contributes to the dispersal of protoplanetary disks. Here, we show that photoevaporative winds should produce a detectable free-free continuum emission given the range of stellar ionizing photons and X-ray luminosities inferred for young sun-like stars. We point out that VLA observations of the nearby disk around TWHya might have already detected this emission at centimeter wavelengths and calculate the wind electron density and mass flow rate. We also estimate the intensities of H radio recombination lines tracing the wind and discuss which ones could be detected with current instrumentation. The detection and profiles of these recombination lines would unambiguously prove our inference of free-free emission from photoevaporating disks like TWHya. In addition, radio/millimeter data can help constraining wind parameters such as temperature and electron density that are fundamental in measuring mass flow rates.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>On the pulse-width statistics in radio pulsars. III. Importance of the conal profile components</title>
		<link>http://voxcharta.org/2012/05/07/on-the-pulse-width-statistics-in-radio-pulsars-iii-importance-of-the-conal-profile-components/</link>
		<comments>http://voxcharta.org/2012/05/07/on-the-pulse-width-statistics-in-radio-pulsars-iii-importance-of-the-conal-profile-components/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:52:02 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[coherence]]></category>
		<category><![CDATA[core component]]></category>
		<category><![CDATA[curvature radius]]></category>
		<category><![CDATA[electron positron]]></category>
		<category><![CDATA[emission region]]></category>
		<category><![CDATA[estimation]]></category>
		<category><![CDATA[gap]]></category>
		<category><![CDATA[inclination angle]]></category>
		<category><![CDATA[magnetic field line]]></category>
		<category><![CDATA[numerical factor]]></category>
		<category><![CDATA[polar cap]]></category>
		<category><![CDATA[profile components]]></category>
		<category><![CDATA[pulse width]]></category>
		<category><![CDATA[radio emission]]></category>
		<category><![CDATA[radio pulsar]]></category>
		<category><![CDATA[rankin]]></category>
		<category><![CDATA[scatter plot]]></category>
		<category><![CDATA[sim 2]]></category>
		<category><![CDATA[stellar radii]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/on-the-pulse-width-statistics-in-radio-pulsars-iii-importance-of-the-conal-profile-components/</guid>
		<description><![CDATA[This work is a continuation of two previous papers of a series, in which we examined the pulse-width statistics of normal radio pulsars. In the first paper we compiled the largest ever database of pulsars with interpulses in their mean profiles. In the second one we confirmed the existence of the lower boundary in the [...]]]></description>
			<content:encoded><![CDATA[<p>This work is a continuation of two previous papers of a series, in which we examined the pulse-width statistics of normal radio pulsars. In the first paper we compiled the largest ever database of pulsars with interpulses in their mean profiles. In the second one we confirmed the existence of the lower boundary in the scatter plot of core component pulse-widths versus pulsar period W50 sim 2.5 P^{-0.5}[deg], first discovered by Rankin using much smaller number of interpulse cases. In this paper we show that the same lower boundary also exists for conal profile components. Rankin proposed a very simple method of estimation of pulsar inclination angle based on comparing the width W50 of its core component with the period dependent value of the lower boundary. We claim that this method can be extended to conal components as well. To explain an existence of the lower boundary Rankin proposed that the core emission originates at or near the polar cap surface. We demonstrated clearly that no coherent pulsar radio emission can originate at altitudes lower than 10 stellar radii, irrespective of the actual mechanism of coherence. We argue that the lower boundary reflects the narrowest angular structures that can be distinguished in the average pulsar beam. These structures represent the core and the conal components in mean pulsar profiles. The P^{-0.5} dependence follows from the dipolar nature of magnetic field lines in the radio emission region, while the numerical factor of about 2.5 deg reflects the curvature radius of a non-dipolar surface magnetic field in the partially screened gap above the polar cap, where dense electron-positron plasma is created. Both core and conal emission should originate at altitudes of about 50 stellar radii in a typical pulsar, with a possibility that the core beam is emitted at a slightly lower heights than the conal ones.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
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		<item>
		<title>Constraints on small-scale cosmological perturbations from gamma-ray searches for dark matter</title>
		<link>http://voxcharta.org/2012/05/07/constraints-on-small-scale-cosmological-perturbations-from-gamma-ray-searches-for-dark-matter/</link>
		<comments>http://voxcharta.org/2012/05/07/constraints-on-small-scale-cosmological-perturbations-from-gamma-ray-searches-for-dark-matter/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:42:50 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abundance]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[density perturbations]]></category>
		<category><![CDATA[early universe]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[indirect detection]]></category>
		<category><![CDATA[inflation]]></category>
		<category><![CDATA[large area space telescope]]></category>
		<category><![CDATA[pbh]]></category>
		<category><![CDATA[phase transition]]></category>
		<category><![CDATA[power spectrum]]></category>
		<category><![CDATA[primordial power]]></category>
		<category><![CDATA[probes]]></category>
		<category><![CDATA[ray fluxes]]></category>
		<category><![CDATA[scales]]></category>
		<category><![CDATA[telescopes]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/constraints-on-small-scale-cosmological-perturbations-from-gamma-ray-searches-for-dark-matter/</guid>
		<description><![CDATA[Events like inflation or phase transitions can produce large density perturbations on very small scales in the early Universe. Probes of small scales are therefore useful for e.g. discriminating between inflationary models. Until recently, the only such constraint came from non-observation of primordial black holes (PBHs), associated with the largest perturbations. Moderate-amplitude perturbations can collapse [...]]]></description>
			<content:encoded><![CDATA[<p>Events like inflation or phase transitions can produce large density perturbations on very small scales in the early Universe. Probes of small scales are therefore useful for e.g. discriminating between inflationary models. Until recently, the only such constraint came from non-observation of primordial black holes (PBHs), associated with the largest perturbations. Moderate-amplitude perturbations can collapse shortly after matter-radiation equality to form ultracompact minihalos (UCMHs) of dark matter, in far greater abundance than PBHs. If dark matter self-annihilates, UCMHs become excellent targets for indirect detection. Here we discuss the gamma-ray fluxes expected from UCMHs, the prospects of observing them with gamma-ray telescopes, and limits upon the primordial power spectrum derived from their non-observation by the Fermi Large Area Space Telescope.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
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		<item>
		<title>The formation of young dense star clusters through mergers</title>
		<link>http://voxcharta.org/2012/05/07/the-formation-of-young-dense-star-clusters-through-mergers/</link>
		<comments>http://voxcharta.org/2012/05/07/the-formation-of-young-dense-star-clusters-through-mergers/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:42:29 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[body simulation]]></category>
		<category><![CDATA[central density]]></category>
		<category><![CDATA[dense cluster]]></category>
		<category><![CDATA[dense star]]></category>
		<category><![CDATA[dynamical evolution]]></category>
		<category><![CDATA[dynamical state]]></category>
		<category><![CDATA[large magellanic cloud]]></category>
		<category><![CDATA[mass distribution]]></category>
		<category><![CDATA[massive cluster]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[massive star cluster]]></category>
		<category><![CDATA[merger]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[NGC]]></category>
		<category><![CDATA[relaxation time]]></category>
		<category><![CDATA[runaway]]></category>
		<category><![CDATA[runaway star]]></category>
		<category><![CDATA[segregation]]></category>
		<category><![CDATA[spatial distribution]]></category>
		<category><![CDATA[westerlund 1]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/the-formation-of-young-dense-star-clusters-through-mergers/</guid>
		<description><![CDATA[Young star clusters like R136 in the Large Magellanic Cloud and NGC 3603, Westerlund 1, and 2 in the Milky Way are dynamically more evolved than expected based on their current relaxation times. In particular, the combination of a high degree of mass segregation, a relatively low central density, and the large number of massive [...]]]></description>
			<content:encoded><![CDATA[<p>Young star clusters like R136 in the Large Magellanic Cloud and NGC 3603, Westerlund 1, and 2 in the Milky Way are dynamically more evolved than expected based on their current relaxation times. In particular, the combination of a high degree of mass segregation, a relatively low central density, and the large number of massive runaway stars in their vicinity are hard to explain with the monolithic formation of these clusters. Young star clusters can achieve such a mature dynamical state if they formed through the mergers of a number of less massive clusters. The shorter relaxation times of less massive clusters cause them to dynamically evolve further by the time they merge, and the merger product preserves the memory of the dynamical evolution of its constituent clusters. With a series of $N$-body simulations, we study the dynamical evolution of single massive clusters and those that are assembled through merging smaller clusters together. We find that the formation of massive star clusters through the mergers of smaller clusters can reproduce the currently observed spatial distribution of massive stars, the density, and the characteristics (number and mass distribution) of the stars ejected as runaways from young dense clusters. We therefore conclude that these clusters and possibly other young massive star clusters formed through the mergers of smaller clusters.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
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		<item>
		<title>A Wide-Field Near-Ir H2 2.122$\mu$m line survey of the Braid Nebula Star Formation Region in Cygnus OB7</title>
		<link>http://voxcharta.org/2012/05/07/a-wide-field-near-ir-h2-2-122mum-line-survey-of-the-braid-nebula-star-formation-region-in-cygnus-ob7/</link>
		<comments>http://voxcharta.org/2012/05/07/a-wide-field-near-ir-h2-2-122mum-line-survey-of-the-braid-nebula-star-formation-region-in-cygnus-ob7/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:41:53 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[analysis suggests that]]></category>
		<category><![CDATA[auriga]]></category>
		<category><![CDATA[colour analysis]]></category>
		<category><![CDATA[dark nebula]]></category>
		<category><![CDATA[evolutionary phase]]></category>
		<category><![CDATA[extinction]]></category>
		<category><![CDATA[field observation]]></category>
		<category><![CDATA[line survey]]></category>
		<category><![CDATA[m line]]></category>
		<category><![CDATA[mm data]]></category>
		<category><![CDATA[molecular cloud]]></category>
		<category><![CDATA[outburst]]></category>
		<category><![CDATA[outflow data]]></category>
		<category><![CDATA[protostar]]></category>
		<category><![CDATA[signpost]]></category>
		<category><![CDATA[square degree field]]></category>
		<category><![CDATA[square degree region]]></category>
		<category><![CDATA[star formation processes]]></category>
		<category><![CDATA[star formation region]]></category>
		<category><![CDATA[ukirt]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/a-wide-field-near-ir-h2-2-122mum-line-survey-of-the-braid-nebula-star-formation-region-in-cygnus-ob7/</guid>
		<description><![CDATA[Context. Outflows and jets are the first signposts of ongoing star formation processes in any molecular cloud, yet their study in optical bands provides limited results due to the large extinction present. Near-infrared unbiased wide-field observations in the H2 1-0 S(1) line at 2.122{\mu}m alleviates the problem, enabling us to detect more outflows and trace [...]]]></description>
			<content:encoded><![CDATA[<p>Context. Outflows and jets are the first signposts of ongoing star formation processes in any molecular cloud, yet their study in optical bands provides limited results due to the large extinction present. Near-infrared unbiased wide-field observations in the H2 1-0 S(1) line at 2.122{\mu}m alleviates the problem, enabling us to detect more outflows and trace them closer to their driving sources. Aims. As part of a large-scale multi-waveband study of ongoing star formation in the Braid Nebula Star Formation region, we focus on a one square degree region that includes Lynds Dark Nebula 1003 and 1004. Our goal is to find all of the near-infrared outflows, uncover their driving sources and estimate their evolutionary phase. Methods. We use near-infrared wide-field observations obtained with WFCAM on UKIRT, in conjunction with previously-published optical and archival MM data, to search for outflows and identify their driving sources; we subsequently use colour-colour analysis to determine the evolutionary phase of each source. Results. Within a one square degree field we have identified 37 complex MHOs, most of which are new. After combining our findings with other wide-field, multi-waveband observations of the same region we were able to discern 28 outflows and at least 18 protostars. Our analysis suggests that these protostars are younger and/or more energetic than those of the Taurus-Auriga region. The outflow data enable us to suggest connection between outflow ejection and repetitive FU Ori outburst events. We also find that star formation progresses from W to E across the investigated region.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/a-wide-field-near-ir-h2-2-122mum-line-survey-of-the-braid-nebula-star-formation-region-in-cygnus-ob7/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The relativistic pulsar-white dwarf binary PSR J1738+0333 II. The most stringent test of scalar-tensor gravity</title>
		<link>http://voxcharta.org/2012/05/07/the-relativistic-pulsar-white-dwarf-binary-psr-j17380333-ii-the-most-stringent-test-of-scalar-tensor-gravity/</link>
		<comments>http://voxcharta.org/2012/05/07/the-relativistic-pulsar-white-dwarf-binary-psr-j17380333-ii-the-most-stringent-test-of-scalar-tensor-gravity/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:41:40 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[binary system]]></category>
		<category><![CDATA[brans]]></category>
		<category><![CDATA[cassini]]></category>
		<category><![CDATA[dwarf companion]]></category>
		<category><![CDATA[eccentricity]]></category>
		<category><![CDATA[general relativity]]></category>
		<category><![CDATA[generalization]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[gravity theory]]></category>
		<category><![CDATA[modified newtonian dynamics]]></category>
		<category><![CDATA[orbital decay]]></category>
		<category><![CDATA[parameter space]]></category>
		<category><![CDATA[proper motion]]></category>
		<category><![CDATA[psr]]></category>
		<category><![CDATA[scalar field]]></category>
		<category><![CDATA[scalar gravity]]></category>
		<category><![CDATA[stringent constraints]]></category>
		<category><![CDATA[stringent test]]></category>
		<category><![CDATA[white dwarf]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/the-relativistic-pulsar-white-dwarf-binary-psr-j17380333-ii-the-most-stringent-test-of-scalar-tensor-gravity/</guid>
		<description><![CDATA[(abridged) We report the results of a 10-year timing campaign on PSR J1738+0333, a 5.85-ms pulsar in a low-eccentricity 8.5-hour orbit with a low-mass white dwarf companion (&#8230;) The measurements of proper motion and parallax allow for a precise subtraction of the kinematic contribution to the observed orbital decay; this results in a significant measurement [...]]]></description>
			<content:encoded><![CDATA[<p>(abridged) We report the results of a 10-year timing campaign on PSR J1738+0333, a 5.85-ms pulsar in a low-eccentricity 8.5-hour orbit with a low-mass white dwarf companion (&#8230;) The measurements of proper motion and parallax allow for a precise subtraction of the kinematic contribution to the observed orbital decay; this results in a significant measurement of the intrinsic orbital decay: (-25.9 +/- 3.2) \times 10^{-15} s/s. This is consistent with the orbital decay from the emission of gravitational waves predicted by general relativity, (-27.7 +1.5/-1.9) \times 10^{-15} s/s (&#8230;). This agreement introduces a tight upper limit on dipolar gravitational wave emission, a prediction of most alternative theories of gravity for asymmetric binary systems such as this. We use this limit to derive the most stringent constraints ever on a wide class of gravity theories, where gravity involves a scalar field contribution. When considering general scalar-tensor theories of gravity, our new bounds are more stringent than the best current solar-system limits over most of the parameter space, and constrain the matter-scalar coupling constant {\alpha}_0^2 to be below the 10^{-5} level. For the special case of the Jordan-Fierz-Brans-Dicke, we obtain the one-sigma bound {\alpha}_0^2 &lt; 2 \times 10^{-5}, which is within a factor two of the Cassini limit. We also use our limit on dipolar gravitational wave emission to constrain a wide class of theories of gravity which are based on a generalization of Bekenstein&#039;s Tensor-Vector-Scalar gravity (TeVeS), a relativistic formulation of Modified Newtonian Dynamics (MOND).</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/the-relativistic-pulsar-white-dwarf-binary-psr-j17380333-ii-the-most-stringent-test-of-scalar-tensor-gravity/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Study of the luminous blue variable star candidate G26.47+0.02 and its environment</title>
		<link>http://voxcharta.org/2012/05/07/study-of-the-luminous-blue-variable-star-candidate-g26-470-02-and-its-environment/</link>
		<comments>http://voxcharta.org/2012/05/07/study-of-the-luminous-blue-variable-star-candidate-g26-470-02-and-its-environment/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:40:36 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[binary nature]]></category>
		<category><![CDATA[binary system]]></category>
		<category><![CDATA[chandra x ray]]></category>
		<category><![CDATA[hi absorption]]></category>
		<category><![CDATA[hypothesis]]></category>
		<category><![CDATA[interstellar medium]]></category>
		<category><![CDATA[ir source]]></category>
		<category><![CDATA[lbv]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[nebula]]></category>
		<category><![CDATA[radio continuum]]></category>
		<category><![CDATA[ray analysis]]></category>
		<category><![CDATA[scale survey]]></category>
		<category><![CDATA[shock]]></category>
		<category><![CDATA[stellar object]]></category>
		<category><![CDATA[stellar wind]]></category>
		<category><![CDATA[surroundings]]></category>
		<category><![CDATA[term observation]]></category>
		<category><![CDATA[thermal emission]]></category>
		<category><![CDATA[variable star]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/study-of-the-luminous-blue-variable-star-candidate-g26-470-02-and-its-environment/</guid>
		<description><![CDATA[The luminous blue variable (LBV) stars are peculiar very massive stars. The study of these stellar objects and their surroundings is important for understanding the evolution of massive stars and its effects on the interstellar medium. We study the LBV star candidate G26.47+0.02. Using several large-scale surveys in different frequencies we performed a multiwavelength study [...]]]></description>
			<content:encoded><![CDATA[<p>The luminous blue variable (LBV) stars are peculiar very massive stars. The study of these stellar objects and their surroundings is important for understanding the evolution of massive stars and its effects on the interstellar medium. We study the LBV star candidate G26.47+0.02. Using several large-scale surveys in different frequencies we performed a multiwavelength study of G26.47+0.02 and its surroundings. We found a molecular shell (seen in the 13CO J=1-0 line) that partially surrounds the mid-infrared nebula of G26.47+0.02, which suggests an interaction between the strong stellar winds and the molecular gas. From the HI absorption and the molecular gas study we conclude that G26.47+0.02 is located at a distance of ~4.8 kpc. The radio continuum analysis shows a both thermal and non-thermal emission toward this LBV candidate, pointing to wind-wind collision shocks from a binary system. This hypothesis is supported by a search of near-IR sources and the Chandra X-ray analysis. Additional multiwavelength and long-term observations are needed to detect some possible variable behavior, and if that is found, to confirm the binary nature of the system.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/study-of-the-luminous-blue-variable-star-candidate-g26-470-02-and-its-environment/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Distance Measurements and Stellar Population Properties via Surface Brightness Fluctuations</title>
		<link>http://voxcharta.org/2012/05/07/distance-measurements-and-stellar-population-properties-via-surface-brightness-fluctuations/</link>
		<comments>http://voxcharta.org/2012/05/07/distance-measurements-and-stellar-population-properties-via-surface-brightness-fluctuations/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:39:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[asymptotic giant branch]]></category>
		<category><![CDATA[biases]]></category>
		<category><![CDATA[different stages]]></category>
		<category><![CDATA[distance scale]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[globular cluster]]></category>
		<category><![CDATA[horizontal branch]]></category>
		<category><![CDATA[important tools]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[multiplicity]]></category>
		<category><![CDATA[new developments]]></category>
		<category><![CDATA[sbf]]></category>
		<category><![CDATA[selection effect]]></category>
		<category><![CDATA[stellar content]]></category>
		<category><![CDATA[stellar evolution]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[stellar system]]></category>
		<category><![CDATA[surface brightness fluctuations]]></category>
		<category><![CDATA[unprecedented accuracy]]></category>
		<category><![CDATA[wavelength band]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/distance-measurements-and-stellar-population-properties-via-surface-brightness-fluctuations/</guid>
		<description><![CDATA[Surface Brightness Fluctuations (SBFs) are one of the most powerful techniques to measure the distance and to constrain the unresolved stellar content of extragalactic systems. For a given bandpass, the absolute SBF magnitude \bar{M} depends on the properties of the underlying stellar population. Multi-band SBFs allow scientists to probe different stages of the stellar evolution: [...]]]></description>
			<content:encoded><![CDATA[<p>Surface Brightness Fluctuations (SBFs) are one of the most powerful techniques to measure the distance and to constrain the unresolved stellar content of extragalactic systems. For a given bandpass, the absolute SBF magnitude \bar{M} depends on the properties of the underlying stellar population. Multi-band SBFs allow scientists to probe different stages of the stellar evolution: UV and blue wavelength band SBFs are sensitive to the evolution of stars within the hot Horizontal Branch (HB) and post-Asymptotic Giant Branch (post-AGB) phase, whereas optical SBF magnitudes explore the stars within the Red Giant Branch (RGB) and HB regime. Near- and Far-infrared SBF luminosities probe the important stellar evolution stage within the AGB and Thermally-Pulsating Asymptotic Giant Branch (TP-AGB) phase. Since the first successful application by Tonry and Schneider, a multiplicity of works have used this method to expand the distance scale up to 150 Mpc and beyond. This article gives a historical background of distance measurements, reviews the basic concepts of the SBF technique, presents a broad sample of these investigations and discusses possible selection effects, biases, and limitations of the method. In particular, exciting new developments and improvements in the field of stellar population synthesis are discussed that are essential to understand the physics and properties of the populations in unresolved stellar systems. Further, promising future directions of the SBF technique are presented. With new upcoming space-based satellites such as Gaia, the SBF method will remain as one of the most important tools to derive distances to galaxies with unprecedented accuracy and to give detailed insights into the stellar content of globular clusters and galaxies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/distance-measurements-and-stellar-population-properties-via-surface-brightness-fluctuations/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A critical analysis of the UV-continuum slopes of high-redshift galaxies; no evidence (yet) for extreme stellar populations at z &gt; 6 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/07/a-critical-analysis-of-the-uv-continuum-slopes-of-high-redshift-galaxies-no-evidence-yet-for-extreme-stellar-populations-at-z-6-replacement-2/</link>
		<comments>http://voxcharta.org/2012/05/07/a-critical-analysis-of-the-uv-continuum-slopes-of-high-redshift-galaxies-no-evidence-yet-for-extreme-stellar-populations-at-z-6-replacement-2/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:38:41 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abundant source]]></category>
		<category><![CDATA[beta 3]]></category>
		<category><![CDATA[clear evidence]]></category>
		<category><![CDATA[critical study]]></category>
		<category><![CDATA[detection threshold]]></category>
		<category><![CDATA[extreme value]]></category>
		<category><![CDATA[fundamental test]]></category>
		<category><![CDATA[galaxy population]]></category>
		<category><![CDATA[hudf]]></category>
		<category><![CDATA[law index]]></category>
		<category><![CDATA[redshift galaxies]]></category>
		<category><![CDATA[redshift range]]></category>
		<category><![CDATA[selection bias]]></category>
		<category><![CDATA[slope analysis]]></category>
		<category><![CDATA[source detection]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[typical value]]></category>
		<category><![CDATA[uv continuum]]></category>
		<category><![CDATA[uv power]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/a-critical-analysis-of-the-uv-continuum-slopes-of-high-redshift-galaxies-no-evidence-yet-for-extreme-stellar-populations-at-z-6-replacement-2/</guid>
		<description><![CDATA[It has recently been reported that the faintest galaxies at z~6-7 display extremely blue UV continuum slopes, with a UV power-law index beta ~ -3. Such slopes are bluer than previously reported for any other galaxy population, and imply extinction-free, young, very low-metallicity stellar populations with a high ionizing photon escape fraction. Here we undertake [...]]]></description>
			<content:encoded><![CDATA[<p>It has recently been reported that the faintest galaxies at z~6-7 display extremely blue UV continuum slopes, with a UV power-law index beta ~ -3. Such slopes are bluer than previously reported for any other galaxy population, and imply extinction-free, young, very low-metallicity stellar populations with a high ionizing photon escape fraction. Here we undertake a critical study of the evidence for such extreme values of beta, combining three new WFC3/IR-selected samples of galaxies spanning ~2 decades in UV luminosity over the redshift range z~4.5-8. We explore the impact of inclusion/exclusion of less robust high-z candidates, and use the varying depths of the samples to explore the effects of noise and selection bias. Simple data-consistency arguments suggest that artificially blue average values of beta can result when the analysis is extended into the deepest ~ 0.5-mag bin of these WFC3/IR-selected samples, regardless of the actual luminosity or z range probed. By confining attention to robust, well-detected high-z galaxy candidates, we find that the average value of beta is consistent with -2.05 +/- 0.10 for z=5-7, and -22 &lt; M_UV &lt; -18. We create and analyse a set of simulations which demonstrate that a bias towards artifically low/blue average values of beta is indeed expected when the UV slope analysis is extended towards the source detection threshold, and conclude that there is as yet no clear evidence for UV slopes significantly bluer than beta ~ -2, the typical value displayed by the bluest star-forming galaxies at more modest z. A robust measurement of beta for the faintest galaxies at z~7-8 remains a key observational goal, as it provides a fundamental test for high escape fractions from a potentially abundant source of reionizing photons. This goal is achievable with HST, but requires still deeper WFC3/IR imaging in the HUDF.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/a-critical-analysis-of-the-uv-continuum-slopes-of-high-redshift-galaxies-no-evidence-yet-for-extreme-stellar-populations-at-z-6-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Improved constraints on the primordial power spectrum at small scales from ultracompact minihalos [Replacement]</title>
		<link>http://voxcharta.org/2012/05/07/improved-constraints-on-the-primordial-power-spectrum-at-small-scales-from-ultracompact-minihalos-replacement/</link>
		<comments>http://voxcharta.org/2012/05/07/improved-constraints-on-the-primordial-power-spectrum-at-small-scales-from-ultracompact-minihalos-replacement/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:37:54 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abundance]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[compilation]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[cosmic microwave background]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[epochs]]></category>
		<category><![CDATA[equality]]></category>
		<category><![CDATA[gamma ray sources]]></category>
		<category><![CDATA[history of the universe]]></category>
		<category><![CDATA[horizon]]></category>
		<category><![CDATA[massive particle]]></category>
		<category><![CDATA[orders of magnitude]]></category>
		<category><![CDATA[power spectrum]]></category>
		<category><![CDATA[present day]]></category>
		<category><![CDATA[primordial density fluctuations]]></category>
		<category><![CDATA[primordial power]]></category>
		<category><![CDATA[radiation]]></category>
		<category><![CDATA[scale structure]]></category>
		<category><![CDATA[scales]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/improved-constraints-on-the-primordial-power-spectrum-at-small-scales-from-ultracompact-minihalos-replacement/</guid>
		<description><![CDATA[For a Gaussian spectrum of primordial density fluctuations, ultracompact minihalos (UCMHs) of dark matter are expected to be produced in much greater abundance than, e.g., primordial black holes. Forming shortly after matter-radiation equality, these objects would develop very dense and spiky dark matter profiles. In the standard scenario where dark matter consists of thermally-produced, weakly-interacting [...]]]></description>
			<content:encoded><![CDATA[<p>For a Gaussian spectrum of primordial density fluctuations, ultracompact minihalos (UCMHs) of dark matter are expected to be produced in much greater abundance than, e.g., primordial black holes. Forming shortly after matter-radiation equality, these objects would develop very dense and spiky dark matter profiles. In the standard scenario where dark matter consists of thermally-produced, weakly-interacting massive particles, UCMHs could thus appear as highly luminous gamma-ray sources, or leave an imprint in the cosmic microwave background by changing the reionisation history of the Universe. We derive corresponding limits on the cosmic abundance of UCMHs at different epochs, and translate them into constraints on the primordial power spectrum. We find the resulting constraints to be quite severe, especially at length scales much smaller than what can be directly probed by the cosmic microwave background or large-scale structure observations. We use our results to provide an updated compilation of the best available constraints on the power of density fluctuations on all scales, ranging from the present-day horizon to scales more than 20 orders of magnitude smaller.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/improved-constraints-on-the-primordial-power-spectrum-at-small-scales-from-ultracompact-minihalos-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The SPLASH Survey: Spectroscopy of 15 M31 Dwarf Spheroidal Satellite Galaxies [Replacement]</title>
		<link>http://voxcharta.org/2012/05/07/the-splash-survey-spectroscopy-of-15-m31-dwarf-spheroidal-satellite-galaxies-replacement/</link>
		<comments>http://voxcharta.org/2012/05/07/the-splash-survey-spectroscopy-of-15-m31-dwarf-spheroidal-satellite-galaxies-replacement/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:36:55 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[andromeda galaxy m31]]></category>
		<category><![CDATA[contamination]]></category>
		<category><![CDATA[dark halo]]></category>
		<category><![CDATA[dark matter halo]]></category>
		<category><![CDATA[dispersion]]></category>
		<category><![CDATA[dwarf]]></category>
		<category><![CDATA[foreground]]></category>
		<category><![CDATA[giant star]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[previous results]]></category>
		<category><![CDATA[remainder]]></category>
		<category><![CDATA[satellite]]></category>
		<category><![CDATA[satellite galaxy]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[substructure]]></category>
		<category><![CDATA[velocities]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/the-splash-survey-spectroscopy-of-15-m31-dwarf-spheroidal-satellite-galaxies-replacement/</guid>
		<description><![CDATA[We present a resolved-star spectroscopic survey of 15 dwarf spheroidal (dSph) satellites of the Andromeda Galaxy (M31) as part of the Spectroscopic and Photometric Landscape of Andromeda&#8217;s Stellar Halo (SPLASH) project. We filter foreground contamination from Milky Way (MW) stars, noting that MW substructure is evident in this contaminant sample. We also filter M31 halo [...]]]></description>
			<content:encoded><![CDATA[<p>We present a resolved-star spectroscopic survey of 15 dwarf spheroidal (dSph) satellites of the Andromeda Galaxy (M31) as part of the Spectroscopic and Photometric Landscape of Andromeda&#8217;s Stellar Halo (SPLASH) project. We filter foreground contamination from Milky Way (MW) stars, noting that MW substructure is evident in this contaminant sample. We also filter M31 halo field giant stars, and identify the remainder as probable dSph members. We then use these members to determine the kinematical properties of the dSphs. For the first time, we confirm that And XVII, XXI, and XXII show kinematics consistent with bound, dark matter-dominated galaxies. From the velocity dispersions for the full sample of dSphs we determine masses, which we combine with the size and luminosity of the galaxies to produce mass-size-luminosity scaling relations. With these scalings we determine that the M31 dSphs are fully consistent with the MW dSphs, suggesting that the well-studied MW satellite population provides a fair sample for broader conclusions. We also estimate dark matter halo masses of the satellites, and find that there is no sign that the luminosity of these galaxies depends on their dark halo mass, a result consistent with what is seen for MW dwarfs. Two of the M31 dSphs (And XV, XVI) have estimated maximum circular velocities smaller than 12 km/s (to 1sigma), which likely places them within the lowest mass dark matter halos known to host stars (along with Bootes I of the MW). Finally, we use the systemic velocities of the M31 satellites to estimate the total mass of the M31 halo: within 139 kpc, M31&#8217;s mass is 8 +4.1 &#8211; 3.7 x 10^11 corresponding to a virial mass for M31&#8217;s dark matter halo of 1.2 +0.9 -0.7 x 10^12, consistent with previous results.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/the-splash-survey-spectroscopy-of-15-m31-dwarf-spheroidal-satellite-galaxies-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Tracing Magnetic Fields with Ground State Alignment [Replacement]</title>
		<link>http://voxcharta.org/2012/05/07/tracing-magnetic-fields-with-ground-state-alignment-replacement-2/</link>
		<comments>http://voxcharta.org/2012/05/07/tracing-magnetic-fields-with-ground-state-alignment-replacement-2/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:32:58 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[3d orientation]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[alignment]]></category>
		<category><![CDATA[astrophysical processes]]></category>
		<category><![CDATA[atoms ions]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[early universe]]></category>
		<category><![CDATA[harbinger]]></category>
		<category><![CDATA[interstellar magnetic fields]]></category>
		<category><![CDATA[life time]]></category>
		<category><![CDATA[magnetic field direction]]></category>
		<category><![CDATA[magnetic field studies]]></category>
		<category><![CDATA[maser research]]></category>
		<category><![CDATA[matter transport]]></category>
		<category><![CDATA[observational study]]></category>
		<category><![CDATA[physical processes]]></category>
		<category><![CDATA[polarization]]></category>
		<category><![CDATA[realignment]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[transport processes]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/tracing-magnetic-fields-with-ground-state-alignment-replacement-2/</guid>
		<description><![CDATA[Observational studies of magnetic fields are vital as magnetic fields play a crucial role in various astrophysical processes, including star formation, accretion of matter, transport processes (e.g., transport of heat), and cosmic rays. We identified a process &#8220;ground state alignment&#8221; as a new way to determine the magnetic field direction in diffuse medium. The alignment [...]]]></description>
			<content:encoded><![CDATA[<p>Observational studies of magnetic fields are vital as magnetic fields play a crucial role in various astrophysical processes, including star formation, accretion of matter, transport processes (e.g., transport of heat), and cosmic rays. We identified a process &#8220;ground state alignment&#8221; as a new way to determine the magnetic field direction in diffuse medium. The alignment is due to anisotropic radiation impinging on the atom/ion, while the magnetic field induces precession and realign the atom/ion and therefore the polarization of the emitted or absorbed radiation reflects the direction of the magnetic field. The atoms get aligned at their low levels and, as the life-time of the atoms/ions we deal with is long, the alignment induced by anisotropic radiation is susceptible to weak magnetic fields ($1{\rm G}\gtrsim B\gtrsim 10^{-15}$G). Compared to the upper level Hanle effect, atomic realignment is most suitable for the studies of magnetic field in the diffuse medium, where magnetic field is relatively weak. In fact, the effects of atomic/ionic alignment, including the realignment in magnetic field, were studied in the laboratory decades ago, mostly in relation to the maser research. Recently, the atomic effect has been already detected in observations from circumstellar medium and this is a harbinger of future extensive magnetic field studies. A unique feature of the atomic realignment is that they can reveal the 3D orientation of magnetic field. In this article, we shall review the basic physical processes involved in atomic realignment and its applications to interplanetary, circumstellar and interstellar magnetic fields. In addition, our research reveals that the polarization of the radiation arising from the transitions between fine and hyperfine states of the ground level can provide a unique diagnostics of magnetic fields, including those in the Early Universe.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/tracing-magnetic-fields-with-ground-state-alignment-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>The observed properties of dwarf galaxies in and around the Local Group [Replacement]</title>
		<link>http://voxcharta.org/2012/05/07/the-observed-properties-of-dwarf-galaxies-in-and-around-the-local-group-replacement/</link>
		<comments>http://voxcharta.org/2012/05/07/the-observed-properties-of-dwarf-galaxies-in-and-around-the-local-group-replacement/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:32:37 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[basic knowledge]]></category>
		<category><![CDATA[central surface brightness]]></category>
		<category><![CDATA[dwarf galaxy]]></category>
		<category><![CDATA[dynamical characteristics]]></category>
		<category><![CDATA[galaxy formation]]></category>
		<category><![CDATA[isolated galaxies]]></category>
		<category><![CDATA[line resource]]></category>
		<category><![CDATA[local group]]></category>
		<category><![CDATA[m31]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[morphological diversity]]></category>
		<category><![CDATA[nearby galaxy]]></category>
		<category><![CDATA[observational capabilities]]></category>
		<category><![CDATA[observational parameters]]></category>
		<category><![CDATA[outer regions]]></category>
		<category><![CDATA[satellite system]]></category>
		<category><![CDATA[spatial extent]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[time scale]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/the-observed-properties-of-dwarf-galaxies-in-and-around-the-local-group-replacement/</guid>
		<description><![CDATA[Positional, structural and dynamical parameters for all dwarf galaxies in and around the Local Group are presented, and various aspects of our observational understanding of this volume-limited sample are discussed. Over 100 nearby galaxies that have distance estimates placing them within 3Mpc of the Sun are identified. This distance threshold samples dwarfs in a large [...]]]></description>
			<content:encoded><![CDATA[<p>Positional, structural and dynamical parameters for all dwarf galaxies in and around the Local Group are presented, and various aspects of our observational understanding of this volume-limited sample are discussed. Over 100 nearby galaxies that have distance estimates placing them within 3Mpc of the Sun are identified. This distance threshold samples dwarfs in a large range of environments, from the satellite systems of the MW and M31, to the dwarfs in the outer regions of the Local Group, to the numerous isolated galaxies found in its surroundings. It extends to, but does not include, the galaxies associated with the next nearest groups. Our basic knowledge of this important galactic subset and their resolved stellar populations will continue to improve dramatically over the coming years with existing and future observational capabilities, and they will continue to provide the most detailed information available on numerous aspects of dwarf galaxy formation and evolution. Basic observational parameters, such as distances, velocities, magnitudes, mean metallicities, as well as structural and dynamical characteristics, are collated, homogenized (as far as possible), and presented in tables that will be continually updated to provide a convenient and current on-line resource. As well as discussing the provenance of the tabulated values and uncertainties affecting their usage, the membership and spatial extent of the MW and M31 subgroups and the Local Group are explored. The morphological diversity of the entire sample and sub-groups is discussed, and time-scales are derived for the Local Group members in the context of their orbital histories. The scaling relations and mean stellar metallicity trends defined by the dwarfs are presented, and the origin of a possible floor in central surface brightness (and, more speculatively, stellar mean metallicity) at faint magnitudes is considered.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/the-observed-properties-of-dwarf-galaxies-in-and-around-the-local-group-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>The Star-formation Mass Sequence out to z=2.5 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/07/the-star-formation-mass-sequence-out-to-z2-5-replacement/</link>
		<comments>http://voxcharta.org/2012/05/07/the-star-formation-mass-sequence-out-to-z2-5-replacement/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:31:27 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[attenuation]]></category>
		<category><![CDATA[blue star]]></category>
		<category><![CDATA[consistent manner]]></category>
		<category><![CDATA[dust obscuration]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[quiescent population]]></category>
		<category><![CDATA[red star]]></category>
		<category><![CDATA[sfr]]></category>
		<category><![CDATA[shape]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[stellar light]]></category>
		<category><![CDATA[stellar mass]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/the-star-formation-mass-sequence-out-to-z2-5-replacement/</guid>
		<description><![CDATA[We study the star formation rate (SFR) &#8211; stellar mass (M*) relation in a self-consistent manner from 0 &#60; z  10 at 1 &#60; z &#60; 1.5), 2) red star-forming galaxies with low levels of dust obscuration and low specific SFRs (11%), and 3) dusty, blue star-forming galaxies with high specific SFRs (7%). The [...]]]></description>
			<content:encoded><![CDATA[<p>We study the star formation rate (SFR) &#8211; stellar mass (M*) relation in a self-consistent manner from 0 &lt; z  10 at 1 &lt; z &lt; 1.5), 2) red star-forming galaxies with low levels of dust obscuration and low specific SFRs (11%), and 3) dusty, blue star-forming galaxies with high specific SFRs (7%). The remaining 28% comprises quiescent galaxies. Galaxies on the &quot;normal&quot; star formation sequence show strong trends of increasing dust attenuation with stellar mass and a decreasing specific SFR, with an observed scatter of 0.25 dex (0.17 dex intrinsic scatter). The dusty, blue galaxies reside in the upper envelope of the star formation sequence with remarkably similar spectral shapes at all masses, suggesting that the same physical process is dominating the stellar light. The red, low-dust star-forming galaxies may be in the process of shutting off and migrating to the quiescent population.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/the-star-formation-mass-sequence-out-to-z2-5-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Comparative study of variational chaos indicators and ODEs&#8217; numerical integrators [Replacement]</title>
		<link>http://voxcharta.org/2012/05/07/comparative-study-of-variational-chaos-indicators-and-odes-numerical-integrators-replacement/</link>
		<comments>http://voxcharta.org/2012/05/07/comparative-study-of-variational-chaos-indicators-and-odes-numerical-integrators-replacement/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:31:19 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[algorithm]]></category>
		<category><![CDATA[alignment]]></category>
		<category><![CDATA[comparative study]]></category>
		<category><![CDATA[complexity]]></category>
		<category><![CDATA[different systems]]></category>
		<category><![CDATA[differential]]></category>
		<category><![CDATA[exponential growth]]></category>
		<category><![CDATA[fli]]></category>
		<category><![CDATA[numerical integrator]]></category>
		<category><![CDATA[numerical technique]]></category>
		<category><![CDATA[oer]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[ordinary differential equation]]></category>
		<category><![CDATA[oscillator]]></category>
		<category><![CDATA[rli]]></category>
		<category><![CDATA[runge kutta]]></category>
		<category><![CDATA[sali]]></category>
		<category><![CDATA[taylor method]]></category>
		<category><![CDATA[work deals]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/comparative-study-of-variational-chaos-indicators-and-odes-numerical-integrators-replacement/</guid>
		<description><![CDATA[The reader can find in the literature a lot of different techniques to study the dynamics of a given system and also, many suitable numerical integrators to compute them. Notwithstanding the recent work of Maffione et al. (2011a) for mappings, a detailed comparison among the widespread indicators of chaos in a general system is still [...]]]></description>
			<content:encoded><![CDATA[<p>The reader can find in the literature a lot of different techniques to study the dynamics of a given system and also, many suitable numerical integrators to compute them. Notwithstanding the recent work of Maffione et al. (2011a) for mappings, a detailed comparison among the widespread indicators of chaos in a general system is still lacking. Such a comparison could lead to select the most efficient algorithms given a certain dynamical problem. Furthermore, in order to choose the appropriate numerical integrators to compute them, more comparative studies among numerical integrators are also needed.   This work deals with both problems. We first extend the work of Maffione et al. (2011) for mappings to the 2D H\&#8217;enon &amp; Heiles (1964) potential, and compare several variational indicators of chaos: the Lyapunov Indicator (LI); the Mean Exponential Growth Factor of Nearby Orbits (MEGNO); the Smaller Alignment Index (SALI) and its generalized version, the Generalized Alignment Index (GALI); the Fast Lyapunov Indicator (FLI) and its variant, the Orthogonal Fast Lyapunov Indicator (OFLI); the Spectral Distance (D) and the Dynamical Spectras of Stretching Numbers (SSNs). We also include in the record the   Relative Lyapunov Indicator (RLI), which is not a variational indicator as the others. Then, we test a numerical technique to integrate   Ordinary Differential Equations (ODEs) based on the Taylor method implemented by Jorba &amp; Zou (2005) (called taylor), and we compare its performance with other two well-known efficient integrators: the Prince &amp; Dormand (1981) implementation of a Runge-Kutta of order 7-8 (DOPRI8) and a Bulirsch-St\&#8221;oer implementation. These tests are run under two very different systems from the complexity of their equations point of view: a triaxial galactic potential model and a perturbed 3D quartic oscillator.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/comparative-study-of-variational-chaos-indicators-and-odes-numerical-integrators-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Metallicity of the Monoceros Stream</title>
		<link>http://voxcharta.org/2012/05/06/the-metallicity-of-the-monoceros-stream/</link>
		<comments>http://voxcharta.org/2012/05/06/the-metallicity-of-the-monoceros-stream/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:53:22 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[asymmetry]]></category>
		<category><![CDATA[caii]]></category>
		<category><![CDATA[calcium deficiencies]]></category>
		<category><![CDATA[deg]]></category>
		<category><![CDATA[dex]]></category>
		<category><![CDATA[disk stars]]></category>
		<category><![CDATA[dispersion]]></category>
		<category><![CDATA[distribution function]]></category>
		<category><![CDATA[dwarf galaxy]]></category>
		<category><![CDATA[footprint]]></category>
		<category><![CDATA[galactic longitude]]></category>
		<category><![CDATA[k line]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[member stars]]></category>
		<category><![CDATA[metallicity]]></category>
		<category><![CDATA[program star]]></category>
		<category><![CDATA[spectroscopic]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[stellar density]]></category>
		<category><![CDATA[tidal stream]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/the-metallicity-of-the-monoceros-stream/</guid>
		<description><![CDATA[We present low-resolution MMT Hectospec spectroscopy of 594 candidate Monoceros stream member stars. Based on strong color-magnitude diagram overdensities, we targeted three fields within the stream&#8217;s footprint, with 178 deg &#60; l &#60; 203 deg and -25 deg &#60; b &#60; 25 deg. By comparing the measured iron abundances with those expected from smooth Galactic [...]]]></description>
			<content:encoded><![CDATA[<p>We present low-resolution MMT Hectospec spectroscopy of 594 candidate Monoceros stream member stars. Based on strong color-magnitude diagram overdensities, we targeted three fields within the stream&#8217;s footprint, with 178 deg &lt; l &lt; 203 deg and -25 deg &lt; b &lt; 25 deg. By comparing the measured iron abundances with those expected from smooth Galactic components alone, we measure, for the first time, the spectroscopic metallicity distribution function for Monoceros. We find the stream to be chemically distinct from both the thick disk and halo, with [Fe/H] = -1, and do not detect a trend in the stream&#039;s metallicity with Galactic longitude. Passing from b = +25 deg to b = -25 deg the median Monoceros metallicity trends upward by 0.1 dex, though uncertainties in modeling sample contamination by the disk and halo make this a marginal detection. In each field, we find Monoceros to have an intrinsic [Fe/H] dispersion of 0.10-0.22 dex. From the CaII K line, we measure [Ca/Fe] for a subsample of metal poor program stars with -1.1 &lt; [Fe/H] &lt; -0.5. In two of three fields, we find calcium deficiencies qualitatively similar to previously reported [Ti/Fe] underabundances in Monoceros and the Sagittarius tidal stream. Further, using 90 spectra of thick disk stars in the Monoceros pointings with b ~ +/-25 deg, we detect a 0.22 dex north/south metallicity asymmetry coincident with known stellar density asymmetry at R_GC ~ 12 kpc and |Z| ~ 1.7 kpc. Our median Monoceros [Fe/H] = -1.0 and its relatively low dispersion naturally fit the expectation for an appropriately luminous M_V ~ -13 dwarf galaxy progenitor.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/the-metallicity-of-the-monoceros-stream/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Discovery of Two Very Wide Binaries with Ultracool Companions and a New Brown Dwarf at the L/T Transition</title>
		<link>http://voxcharta.org/2012/05/06/discovery-of-two-very-wide-binaries-with-ultracool-companions-and-a-new-brown-dwarf-at-the-lt-transition/</link>
		<comments>http://voxcharta.org/2012/05/06/discovery-of-two-very-wide-binaries-with-ultracool-companions-and-a-new-brown-dwarf-at-the-lt-transition/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:50:22 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[2mass]]></category>
		<category><![CDATA[angular separation]]></category>
		<category><![CDATA[binaries]]></category>
		<category><![CDATA[brown dwarf]]></category>
		<category><![CDATA[catalog]]></category>
		<category><![CDATA[companion]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[infrared spectra]]></category>
		<category><![CDATA[infrared spectrum]]></category>
		<category><![CDATA[infrared survey]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[micron]]></category>
		<category><![CDATA[optical spectrum]]></category>
		<category><![CDATA[pair]]></category>
		<category><![CDATA[proper motion]]></category>
		<category><![CDATA[sky survey]]></category>
		<category><![CDATA[spectral type]]></category>
		<category><![CDATA[transition]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/discovery-of-two-very-wide-binaries-with-ultracool-companions-and-a-new-brown-dwarf-at-the-lt-transition/</guid>
		<description><![CDATA[We present the discovery and spectroscopic follow-up of a nearby late-type L dwarf (2M0614+3950), and two extremely wide very-low-mass binary systems (2M0525-7425AB and 2M1348-1344AB), resulting from our search for common proper motion pairs containing ultracool components in the Two Micron All Sky Survey (2MASS) and the Wide-field Infrared Survey Explorer (WISE) catalogs. The near-infrared spectrum [...]]]></description>
			<content:encoded><![CDATA[<p>We present the discovery and spectroscopic follow-up of a nearby late-type L dwarf (2M0614+3950), and two extremely wide very-low-mass binary systems (2M0525-7425AB and 2M1348-1344AB), resulting from our search for common proper motion pairs containing ultracool components in the Two Micron All Sky Survey (2MASS) and the Wide-field Infrared Survey Explorer (WISE) catalogs. The near-infrared spectrum of 2M0614+3950 indicates a spectral type L9 \pm 1 object residing at a distance of 26.1 \pm 1.3 pc. The optical spectrum of the 2M0525-7425 primary reveals an M3.0 \pm 0.5 dwarf, accompanied by a secondary previously classified as L2. The system has an angular separation of ~44&#8243;, equivalent to ~2000 AU at the 45.7 \pm 2.5 pc distance. Using optical and infrared spectra, respectively, we classify the components of 2M1348-1344AB as M4.5 \pm 0.5 and T6 \pm 1. The angular separation of ~68&#8243; is equivalent to ~1300 AU at the distance of 19.2 \pm 0.9 pc. 2M1348-1344AB is one of only five very wide (separation &gt; 1000 AU) systems containing late T dwarfs known to date.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/discovery-of-two-very-wide-binaries-with-ultracool-companions-and-a-new-brown-dwarf-at-the-lt-transition/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Comparative study of variational chaos indicators and ODEs&#8217; numerical integrators [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/06/comparative-study-of-variational-chaos-indicators-and-odes-numerical-integrators-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/06/comparative-study-of-variational-chaos-indicators-and-odes-numerical-integrators-cross-listing/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:47:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[algorithm]]></category>
		<category><![CDATA[alignment]]></category>
		<category><![CDATA[comparative study]]></category>
		<category><![CDATA[complexity]]></category>
		<category><![CDATA[different systems]]></category>
		<category><![CDATA[differential]]></category>
		<category><![CDATA[exponential growth]]></category>
		<category><![CDATA[fli]]></category>
		<category><![CDATA[numerical integrator]]></category>
		<category><![CDATA[numerical technique]]></category>
		<category><![CDATA[oer]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[ordinary differential equation]]></category>
		<category><![CDATA[oscillator]]></category>
		<category><![CDATA[rli]]></category>
		<category><![CDATA[runge kutta]]></category>
		<category><![CDATA[sali]]></category>
		<category><![CDATA[taylor method]]></category>
		<category><![CDATA[work deals]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/comparative-study-of-variational-chaos-indicators-and-odes-numerical-integrators-cross-listing/</guid>
		<description><![CDATA[The reader can find in the literature a lot of different techniques to study the dynamics of a given system and also, many suitable numerical integrators to compute them. Notwithstanding the recent work of Maffione et al. (2011a) for mappings, a detailed comparison among the widespread indicators of chaos in a general system is still [...]]]></description>
			<content:encoded><![CDATA[<p>The reader can find in the literature a lot of different techniques to study the dynamics of a given system and also, many suitable numerical integrators to compute them. Notwithstanding the recent work of Maffione et al. (2011a) for mappings, a detailed comparison among the widespread indicators of chaos in a general system is still lacking. Such a comparison could lead to select the most efficient algorithms given a certain dynamical problem. Furthermore, in order to choose the appropriate numerical integrators to compute them, more comparative studies among numerical integrators are also needed.   This work deals with both problems. We first extend the work of Maffione et al. (2011) for mappings to the 2D H\&#8217;enon &amp; Heiles (1964) potential, and compare several variational indicators of chaos: the Lyapunov Indicator (LI); the Mean Exponential Growth Factor of Nearby Orbits (MEGNO); the Smaller Alignment Index (SALI) and its generalized version, the Generalized Alignment Index (GALI); the Fast Lyapunov Indicator (FLI) and its variant, the Orthogonal Fast Lyapunov Indicator (OFLI); the Spectral Distance (D) and the Dynamical Spectras of Stretching Numbers (SSNs). We also include in the record the   Relative Lyapunov Indicator (RLI), which is not a variational indicator as the others. Then, we test a numerical technique to integrate   Ordinary Differential Equations (ODEs) based on the Taylor method implemented by Jorba &amp; Zou (2005) (called taylor), and we compare its performance with other two well-known efficient integrators: the Prince &amp; Dormand (1981) implementation of a Runge-Kutta of order 7-8 (DOPRI8) and a Bulirsch-St\&#8221;oer implementation. These tests are run under two very different systems from the complexity of their equations point of view: a triaxial galactic potential model and a perturbed 3D quartic oscillator.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/comparative-study-of-variational-chaos-indicators-and-odes-numerical-integrators-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Constraints on the Magellanic Clouds&#8217; Interaction from the Distribution of OB Stars and the Kinematics of Giants</title>
		<link>http://voxcharta.org/2012/05/06/constraints-on-the-magellanic-clouds-interaction-from-the-distribution-of-ob-stars-and-the-kinematics-of-giants/</link>
		<comments>http://voxcharta.org/2012/05/06/constraints-on-the-magellanic-clouds-interaction-from-the-distribution-of-ob-stars-and-the-kinematics-of-giants/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:41:28 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[clump]]></category>
		<category><![CDATA[galactic plane]]></category>
		<category><![CDATA[high density]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[lmc bar]]></category>
		<category><![CDATA[magellanic stream]]></category>
		<category><![CDATA[motion analysis]]></category>
		<category><![CDATA[narrow path]]></category>
		<category><![CDATA[observational result]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[periphery]]></category>
		<category><![CDATA[photometry]]></category>
		<category><![CDATA[proper motion]]></category>
		<category><![CDATA[radial velocity]]></category>
		<category><![CDATA[red giant]]></category>
		<category><![CDATA[small magellanic cloud]]></category>
		<category><![CDATA[spatial distribution]]></category>
		<category><![CDATA[star candidates]]></category>
		<category><![CDATA[supergiant]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/constraints-on-the-magellanic-clouds-interaction-from-the-distribution-of-ob-stars-and-the-kinematics-of-giants/</guid>
		<description><![CDATA[Young, OB-type candidates are identified in a ~7900 sq-deg. region encompassing the Large and Small Magellanic Clouds (LMC/SMC) periphery, the Bridge, part of the Magellanic Stream (MS) and Leading Arm (LA). Selection is based on UV, optical and IR photometry from existing large-area surveys and proper motions from the Southern Proper Motion 4 catalog (SPM4). [...]]]></description>
			<content:encoded><![CDATA[<p>Young, OB-type candidates are identified in a ~7900 sq-deg. region encompassing the Large and Small Magellanic Clouds (LMC/SMC) periphery, the Bridge, part of the Magellanic Stream (MS) and Leading Arm (LA). Selection is based on UV, optical and IR photometry from existing large-area surveys and proper motions from the Southern Proper Motion 4 catalog (SPM4). The spatial distribution of these young star candidates shows: 1) a well-populated SMC wing which continues westward with two branches partially surrounding the SMC, 2) a rather narrow path from the SMC wing eastward toward the LMC which is offset by 1 to 2 deg. from the high-density H I ridge in the Bridge, 3) a well-populated periphery of the LMC dominated by clumps of stars at the ends of the LMC bar and 4) a few scattered candidates in the MS and two overdensities in the LA regions above and below the Galactic plane. Additionally, a proper-motion analysis is made of a radial-velocity selected sample of red giants and supergiants in the LMC, previously shown to be a kinematically and chemically distinct subgroup, most likely captured from the SMC. SPM4 proper motions of these stars also indicate they are distinct from the LMC population. The observational results presented here, combined with the known orbits of the Clouds, and other aspects of the LMC morphology, suggest an off-center, moderate to highly-inclined collision between the SMC and the LMC&#8217;s disk that took place between 100 and 200 Myr ago.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/constraints-on-the-magellanic-clouds-interaction-from-the-distribution-of-ob-stars-and-the-kinematics-of-giants/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Fokker-Planck Models for M15 without a Central Black Hole: The Role of the Mass Function</title>
		<link>http://voxcharta.org/2012/05/06/fokker-planck-models-for-m15-without-a-central-black-hole-the-role-of-the-mass-function/</link>
		<comments>http://voxcharta.org/2012/05/06/fokker-planck-models-for-m15-without-a-central-black-hole-the-role-of-the-mass-function/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:38:08 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[cluster m15]]></category>
		<category><![CDATA[collapsed core]]></category>
		<category><![CDATA[gravitational potential]]></category>
		<category><![CDATA[hst measurements]]></category>
		<category><![CDATA[hubble space telescope]]></category>
		<category><![CDATA[initial mass function]]></category>
		<category><![CDATA[initial population]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[mass function]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[solar mass]]></category>
		<category><![CDATA[spatial distribution]]></category>
		<category><![CDATA[star cluster]]></category>
		<category><![CDATA[star count]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[velocity dispersion]]></category>
		<category><![CDATA[white dwarf]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/fokker-planck-models-for-m15-without-a-central-black-hole-the-role-of-the-mass-function/</guid>
		<description><![CDATA[We have developed a set of dynamically evolving Fokker-Planck models for the collapsed-core globular star cluster M15, which directly address the issue of whether a central black hole is required to fit Hubble Space Telescope (HST) observations of the stellar spatial distribution and kinematics. As in our previous work reported by Dull et al., we [...]]]></description>
			<content:encoded><![CDATA[<p>We have developed a set of dynamically evolving Fokker-Planck models for the collapsed-core globular star cluster M15, which directly address the issue of whether a central black hole is required to fit Hubble Space Telescope (HST) observations of the stellar spatial distribution and kinematics. As in our previous work reported by Dull et al., we find that a central black hole is not needed. Using local mass-function data from HST studies, we have also inferred the global initial stellar mass function. As a consequence of extreme mass segregation, the local mass functions differs from the global mass function at every location. In addition to reproducing the observed mass functions, the models also provide good fits to the star-count and velocity-dispersion profiles, and to the millisecond pulsar accelerations. We address concerns about the large neutron star populations adopted in our previous Fokker-Planck models for M15. We find that good model fits can be obtained with as few as 1600 neutron stars; this corresponds to a retention fraction of 5% of the initial population for our best fit initial mass function. The models contain a substantial population of massive white dwarfs, that range in mass up to 1.2 solar masses. The combined contribution by the massive white dwarfs and neutron stars provides the gravitational potential needed to reproduce HST measurements of the central velocity dispersion profile.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/fokker-planck-models-for-m15-without-a-central-black-hole-the-role-of-the-mass-function/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Metallicity-Dependent quenching of Star Formation at High Redshift in Small Galaxies [Replacement]</title>
		<link>http://voxcharta.org/2012/05/06/metallicity-dependent-quenching-of-star-formation-at-high-redshift-in-small-galaxies-replacement/</link>
		<comments>http://voxcharta.org/2012/05/06/metallicity-dependent-quenching-of-star-formation-at-high-redshift-in-small-galaxies-replacement/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:37:33 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[atomic gas]]></category>
		<category><![CDATA[dark halo]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[history of galaxies]]></category>
		<category><![CDATA[metal enrichment]]></category>
		<category><![CDATA[metals]]></category>
		<category><![CDATA[precursor]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[star formation history]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[suppression]]></category>
		<category><![CDATA[transition]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/metallicity-dependent-quenching-of-star-formation-at-high-redshift-in-small-galaxies-replacement/</guid>
		<description><![CDATA[[abridged] The star formation rates (SFR) of low-metallicity galaxies depend sensitively on the gas metallicity, because metals are crucial to mediating the transition from intermediate-temperature atomic gas to cold molecular gas, a necessary precursor to star formation. We study the impact of this effect on the star formation history of galaxies. We incorporate metallicity-dependent star [...]]]></description>
			<content:encoded><![CDATA[<p>[abridged] The star formation rates (SFR) of low-metallicity galaxies depend sensitively on the gas metallicity, because metals are crucial to mediating the transition from intermediate-temperature atomic gas to cold molecular gas, a necessary precursor to star formation. We study the impact of this effect on the star formation history of galaxies. We incorporate metallicity-dependent star formation and metal enrichment in a simple model that follows the evolution of a halo main progenitor. Our model shows that including the effect of metallicity leads to suppression of star formation at redshift z&gt;2 in dark halos with masses &lt;~ 10^11 Msun, with the suppression becoming near total for halos below ~10^9.5-10 Msun. We find that at high redshift the SFR cannot catch up with the gas inflow rate (IR), because the SFR is limited by the free-fall time, and because it is suppressed further by a lack of metals. As a result, in each galaxy the SFR is growing in time faster than the IR, and the integrated cosmic SFR density is rising with time. The suppressed in situ SFR at high z makes the growth of stellar mass dominated by ex situ SFR which implies that the specific SFR (sSFR) remains constant with time. The intensely accreted gas at high z is accumulating as an atomic gas reservoir. This provides additional fuel for star formation in 10^10 &#8211; 10^12 Msun halos at z ~ 1-3, which allows the SFR to exceed the instantaneous IR, and may enable an even higher outflow rate. At z&lt;1, following the natural decline in IR with time due to the universal expansion, the SFR and sSFR are expected to drop. We specify the expected dependence of sSFR and metallicity on stellar mass and redshift. At a given z, and below a critical mass, these relations are predicted to be flat and rising respectively. Our model predictions qualitatively match some of the puzzling features in the observed star formation history.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/metallicity-dependent-quenching-of-star-formation-at-high-redshift-in-small-galaxies-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Signatures of minor mergers in the Milky Way disc I: The SEGUE stellar sample [Replacement]</title>
		<link>http://voxcharta.org/2012/05/06/signatures-of-minor-mergers-in-the-milky-way-disc-i-the-segue-stellar-sample-replacement/</link>
		<comments>http://voxcharta.org/2012/05/06/signatures-of-minor-mergers-in-the-milky-way-disc-i-the-segue-stellar-sample-replacement/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:34:32 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[body simulation]]></category>
		<category><![CDATA[dark matter halo]]></category>
		<category><![CDATA[energy distribution]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[host galaxy]]></category>
		<category><![CDATA[imprints]]></category>
		<category><![CDATA[merger]]></category>
		<category><![CDATA[merger event]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[orbital parameters]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[phase space]]></category>
		<category><![CDATA[progenitor]]></category>
		<category><![CDATA[sagittarius dwarf galaxy]]></category>
		<category><![CDATA[schuster]]></category>
		<category><![CDATA[segue]]></category>
		<category><![CDATA[similar features]]></category>
		<category><![CDATA[space distribution]]></category>
		<category><![CDATA[spatial region]]></category>
		<category><![CDATA[tight constraints]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/signatures-of-minor-mergers-in-the-milky-way-disc-i-the-segue-stellar-sample-replacement/</guid>
		<description><![CDATA[It is now known that minor mergers are capable of creating structure in the phase-space distribution of their host galaxy&#8217;s disc. In order to search for such imprints in the Milky Way, we analyse the SEGUE F/G-dwarf and the Schuster et al. (2006) stellar samples. We find similar features in these two completely independent stellar [...]]]></description>
			<content:encoded><![CDATA[<p>It is now known that minor mergers are capable of creating structure in the phase-space distribution of their host galaxy&#8217;s disc. In order to search for such imprints in the Milky Way, we analyse the SEGUE F/G-dwarf and the Schuster et al. (2006) stellar samples. We find similar features in these two completely independent stellar samples, consistent with the predictions of a Milky Way minor-merger event. We next apply the same analyses to high-resolution, idealised N-body simulations of the interaction between the Sagittarius dwarf galaxy and the Milky Way. The energy distributions of stellar particle samples in small spatial regions in the host disc reveal strong variations of structure with position. We find good matches to the observations for models with a mass of Sagittarius&#8217; dark matter halo progenitor $\lessapprox 10^{11}$ M$_{\odot}$. Thus, we show that this kind of analysis could be used to provide unprecedentedly tight constraints on Sagittarius&#8217; orbital parameters, as well as place a lower limit on its mass.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/signatures-of-minor-mergers-in-the-milky-way-disc-i-the-segue-stellar-sample-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Kinematic groups beyond the Solar neighbourhood with RAVE</title>
		<link>http://voxcharta.org/2012/05/03/kinematic-groups-beyond-the-solar-neighbourhood-with-rave/</link>
		<comments>http://voxcharta.org/2012/05/03/kinematic-groups-beyond-the-solar-neighbourhood-with-rave/#comments</comments>
		<pubDate>Fri, 04 May 2012 00:57:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[dynamical model]]></category>
		<category><![CDATA[galactic plane]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[hercules group]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[radii]]></category>
		<category><![CDATA[scale features]]></category>
		<category><![CDATA[solar circle]]></category>
		<category><![CDATA[solar neighbourhood]]></category>
		<category><![CDATA[spiral arm]]></category>
		<category><![CDATA[Sun]]></category>
		<category><![CDATA[v 92]]></category>
		<category><![CDATA[velocity distribution]]></category>
		<category><![CDATA[wavelet]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/03/kinematic-groups-beyond-the-solar-neighbourhood-with-rave/</guid>
		<description><![CDATA[We analyse the kinematics of disc stars observed by the RAVE survey in and beyond the Solar neighbourhood.We detect significant overdensities in the velocity distributions using a technique based on the wavelet transform.We find that the main local kinematic groups are large scale features, surviving at least up to ~1 kpc from the Sun in [...]]]></description>
			<content:encoded><![CDATA[<p>We analyse the kinematics of disc stars observed by the RAVE survey in and beyond the Solar neighbourhood.We detect significant overdensities in the velocity distributions using a technique based on the wavelet transform.We find that the main local kinematic groups are large scale features, surviving at least up to ~1 kpc from the Sun in the direction of anti-rotation, and also at ~700 pc below the Galactic plane.We also find that for regions located at different radii than the Sun, the known groups appear shifted in the velocity plane. For example, the Hercules group has a larger azimuthal velocity for regions inside the Solar circle and a lower value outside. We have also discovered a new group at (U, V) = (92,-22) km/s in the Solar neighbourhood and confirmed the significance of other previously found groups. Some of these trends detected for the first time are consistent with dynamical models of the effects of the bar and the spiral arms. More modelling is required to definitively characterise the non-axisymmetric components of our Galaxy using these groups.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/03/kinematic-groups-beyond-the-solar-neighbourhood-with-rave/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Star-formation Mass Sequence out to z=2.5</title>
		<link>http://voxcharta.org/2012/05/03/the-star-formation-mass-sequence-out-to-z2-5/</link>
		<comments>http://voxcharta.org/2012/05/03/the-star-formation-mass-sequence-out-to-z2-5/#comments</comments>
		<pubDate>Fri, 04 May 2012 00:57:24 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[attenuation]]></category>
		<category><![CDATA[blue star]]></category>
		<category><![CDATA[consistent manner]]></category>
		<category><![CDATA[dust obscuration]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[quiescent population]]></category>
		<category><![CDATA[red star]]></category>
		<category><![CDATA[shape]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[stellar light]]></category>
		<category><![CDATA[stellar mass]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/03/the-star-formation-mass-sequence-out-to-z2-5/</guid>
		<description><![CDATA[We study the star formation rate (SFR) &#8211; stellar mass (M*) relation in a self-consistent manner from 0 &#60; z  10 at 1 &#60; z &#60; 1.5), 2) red star-forming galaxies with low levels of dust obscuration and low specific SFRs (12%), and 3) dusty, blue star-forming galaxies with high specific SFRs (6%). The [...]]]></description>
			<content:encoded><![CDATA[<p>We study the star formation rate (SFR) &#8211; stellar mass (M*) relation in a self-consistent manner from 0 &lt; z  10 at 1 &lt; z &lt; 1.5), 2) red star-forming galaxies with low levels of dust obscuration and low specific SFRs (12%), and 3) dusty, blue star-forming galaxies with high specific SFRs (6%). The remaining 29% comprises quiescent galaxies. Galaxies on the &quot;normal&quot; star formation sequence show strong trends of increasing dust attenuation and decreasing sSFR with stellar mass, with an observed scatter of 0.26 dex (0.19 dex intrinsic scatter). The dusty, blue galaxies reside in the upper envelope of the star formation sequence with remarkably similar spectral shapes at all masses, suggesting that the same physical process is dominating the stellar light. The red, low-dust star-forming galaxies may be in the process of shutting off and migrating to the quiescent population.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/03/the-star-formation-mass-sequence-out-to-z2-5/feed/</wfw:commentRss>
		<slash:comments>1</slash:comments>
		</item>
		<item>
		<title>[CII] 158 micron line detection of the warm ionized medium in the Scutum&#8211;Crux spiral arm tangency</title>
		<link>http://voxcharta.org/2012/05/03/cii-158-micron-line-detection-of-the-warm-ionized-medium-in-the-scutum-crux-spiral-arm-tangency/</link>
		<comments>http://voxcharta.org/2012/05/03/cii-158-micron-line-detection-of-the-warm-ionized-medium-in-the-scutum-crux-spiral-arm-tangency/#comments</comments>
		<pubDate>Fri, 04 May 2012 00:56:13 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cii]]></category>
		<category><![CDATA[clouds]]></category>
		<category><![CDATA[cm 3]]></category>
		<category><![CDATA[crux]]></category>
		<category><![CDATA[dispersion]]></category>
		<category><![CDATA[electron density]]></category>
		<category><![CDATA[galactic plane]]></category>
		<category><![CDATA[geometry]]></category>
		<category><![CDATA[hifi]]></category>
		<category><![CDATA[ionized gas]]></category>
		<category><![CDATA[ism]]></category>
		<category><![CDATA[longitude]]></category>
		<category><![CDATA[micron]]></category>
		<category><![CDATA[shock compression]]></category>
		<category><![CDATA[spectral survey]]></category>
		<category><![CDATA[spiral arm]]></category>
		<category><![CDATA[spiral density wave]]></category>
		<category><![CDATA[tangency]]></category>
		<category><![CDATA[velocities]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/03/cii-158-micron-line-detection-of-the-warm-ionized-medium-in-the-scutum-crux-spiral-arm-tangency/</guid>
		<description><![CDATA[HIFI GOT C+ Galactic plane [CII] spectral survey has detected strong emission at the spiral arm tangencies. We use the unique viewing geometry of the Scutum-Crux (S-C) tangency near i = 30degs to detect the warm ionized medium (WIM) component traced by [CII] and to study the effects of spiral density waves on Interstellar Medium [...]]]></description>
			<content:encoded><![CDATA[<p>HIFI GOT C+ Galactic plane [CII] spectral survey has detected strong emission at the spiral arm tangencies. We use the unique viewing geometry of the Scutum-Crux (S-C) tangency near i = 30degs to detect the warm ionized medium (WIM) component traced by [CII] and to study the effects of spiral density waves on Interstellar Medium (ISM) gas. We compare [CII] velocity features with ancillary HI, 12CO and 13CO data near tangent velocities at each longitude to separate the cold neutral medium and the warm neutral + ionized components in the S-C tangency, then we identify [CII] emission at the highest velocities without any contribution from 12CO clouds, as WIM. We present the GOT C+ results for the S-C tangency. We interpret the diffuse and extended excess [CII] emission at and above the tangent velocities as arising in the electron-dominated warm ionized gas in the WIM. We derive an electron density in the range of 0.2 &#8211; 0.9 cm^-3 at each longitude, a factor of several higher than the average value from Halpha and pulsar dispersion. We interpret the excess [CII] in S-C tangency as shock compression of the WIM induced by the spiral density waves.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/03/cii-158-micron-line-detection-of-the-warm-ionized-medium-in-the-scutum-crux-spiral-arm-tangency/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>An observational test for correlations between cosmic rays and magnetic fields</title>
		<link>http://voxcharta.org/2012/05/03/an-observational-test-for-correlations-between-cosmic-rays-and-magnetic-fields/</link>
		<comments>http://voxcharta.org/2012/05/03/an-observational-test-for-correlations-between-cosmic-rays-and-magnetic-fields/#comments</comments>
		<pubDate>Fri, 04 May 2012 00:52:05 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[energy density]]></category>
		<category><![CDATA[equipartition]]></category>
		<category><![CDATA[faraday rotation]]></category>
		<category><![CDATA[fluctuation]]></category>
		<category><![CDATA[galactic magnetic field]]></category>
		<category><![CDATA[intensity]]></category>
		<category><![CDATA[interstellar magnetic fields]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[local energy]]></category>
		<category><![CDATA[magnetic energy]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[number density]]></category>
		<category><![CDATA[polarization data]]></category>
		<category><![CDATA[ray number]]></category>
		<category><![CDATA[relative magnitude]]></category>
		<category><![CDATA[scales]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/03/an-observational-test-for-correlations-between-cosmic-rays-and-magnetic-fields/</guid>
		<description><![CDATA[We derive the magnitude of fluctuations in total synchrotron intensity in the Milky Way, both from observations and from theory under various assumption about the relation between cosmic rays and interstellar magnetic fields. Given the relative magnitude of the fluctuations in the Galactic magnetic field suggested by the Faraday rotation and polarization data, the observations [...]]]></description>
			<content:encoded><![CDATA[<p>We derive the magnitude of fluctuations in total synchrotron intensity in the Milky Way, both from observations and from theory under various assumption about the relation between cosmic rays and interstellar magnetic fields. Given the relative magnitude of the fluctuations in the Galactic magnetic field suggested by the Faraday rotation and polarization data, the observations are inconsistent with local energy equipartition between cosmic rays and magnetic fields. Our analysis of synchrotron fluctuations suggests that the distribution of cosmic rays is nearly uniform at scales of order $100\p$, in contrast to that of the interstellar magnetic field. A conservative upper limit on the relative variations in the cosmic ray number density is 0.2&#8211;0.4 at the scales of order 100\,pc. Our results are consistent with a mild anticorrelation between cosmic-ray and magnetic energy densities at these scales. Energy equipartition between cosmic rays and magnetic fields still may hold, but at scales exceeding 1\,kpc.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/03/an-observational-test-for-correlations-between-cosmic-rays-and-magnetic-fields/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A near-infrared study of the star forming region RCW 34</title>
		<link>http://voxcharta.org/2012/05/03/a-near-infrared-study-of-the-star-forming-region-rcw-34/</link>
		<comments>http://voxcharta.org/2012/05/03/a-near-infrared-study-of-the-star-forming-region-rcw-34/#comments</comments>
		<pubDate>Fri, 04 May 2012 00:49:27 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[colour magnitude diagram]]></category>
		<category><![CDATA[concentration]]></category>
		<category><![CDATA[early b]]></category>
		<category><![CDATA[exposure time]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[infrared imaging]]></category>
		<category><![CDATA[luminosity function]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[main sequence star]]></category>
		<category><![CDATA[maser]]></category>
		<category><![CDATA[methanol]]></category>
		<category><![CDATA[remainder]]></category>
		<category><![CDATA[spatial distribution]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[subset]]></category>
		<category><![CDATA[sutherland]]></category>
		<category><![CDATA[Telescope]]></category>
		<category><![CDATA[type star]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/03/a-near-infrared-study-of-the-star-forming-region-rcw-34/</guid>
		<description><![CDATA[We report the results of a near-infrared imaging study of a $7.8 \times 7.8$ arcmin$^2$ region centered on the 6.7 GHz methanol maser associated with the RCW 34 star forming region using the 1.4m IRSF telescope at Sutherland. A total of 1283 objects were detected simultaneously in J, H, and K for an exposure time [...]]]></description>
			<content:encoded><![CDATA[<p>We report the results of a near-infrared imaging study of a $7.8 \times 7.8$ arcmin$^2$ region centered on the 6.7 GHz methanol maser associated with the RCW 34 star forming region using the 1.4m IRSF telescope at Sutherland. A total of 1283 objects were detected simultaneously in J, H, and K for an exposure time of 10800 seconds. The J-H, H-K two-colour diagram revealed a strong concentration of more than 700 objects with colours similar to what is expected of reddened classical T Tauri stars. The distribution of the objects on the K {\it vs} J-K colour-magnitude diagram is also suggestive that a significant fraction of the 1283 objects is lower mass pre-main sequence stars. We also present the luminosity function for the subset of about 700 pre-main sequence stars and show that it suggests ongoing star formation activity for about $10^7$ years. An examination of the spatial distribution of the pre-main sequence stars shows that the fainter (older) part of the population is more dispersed over the observed region and the brighter (younger) subset is more concentrated around the position of the O8.5V star. This suggests that the physical effects of the O8.5V star and the two early B-type stars on the remainder of the cloud out of which they formed, could have played a role in the onset of the more recent episode of star formation in RCW 34.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/03/a-near-infrared-study-of-the-star-forming-region-rcw-34/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Properties of Two Low Redshift O VI Absorbers and Their Associated Galaxies Toward 3C 263</title>
		<link>http://voxcharta.org/2012/05/03/the-properties-of-two-low-redshift-o-vi-absorbers-and-their-associated-galaxies-toward-3c-263/</link>
		<comments>http://voxcharta.org/2012/05/03/the-properties-of-two-low-redshift-o-vi-absorbers-and-their-associated-galaxies-toward-3c-263/#comments</comments>
		<pubDate>Fri, 04 May 2012 00:42:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorber]]></category>
		<category><![CDATA[absorption line]]></category>
		<category><![CDATA[absorption system]]></category>
		<category><![CDATA[doppler]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[filament]]></category>
		<category><![CDATA[fuse]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[impact parameter]]></category>
		<category><![CDATA[Lambda]]></category>
		<category><![CDATA[object spectrograph]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[phase system]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[spiral]]></category>
		<category><![CDATA[temperature gas]]></category>
		<category><![CDATA[traces]]></category>
		<category><![CDATA[transition temperature]]></category>
		<category><![CDATA[ultraviolet observations]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/03/the-properties-of-two-low-redshift-o-vi-absorbers-and-their-associated-galaxies-toward-3c-263/</guid>
		<description><![CDATA[Ultraviolet observations of the QSO 3C 263 (zem = 0.652) with COS and FUSE reveal O VI absorption systems at z = 0.06342 and 0.14072 . WIYN multi-object spectrograph observations provide information about the galaxies associated with the absorbers. The multi-phase system at z = 0.06342 traces cool photoionized gas and warm collisionally ionized gas [...]]]></description>
			<content:encoded><![CDATA[<p>Ultraviolet observations of the QSO 3C 263 (zem = 0.652) with COS and FUSE reveal O VI absorption systems at z = 0.06342 and 0.14072 . WIYN multi-object spectrograph observations provide information about the galaxies associated with the absorbers. The multi-phase system at z = 0.06342 traces cool photoionized gas and warm collisionally ionized gas associated with a L ~ 0.31L* compact spiral emission line galaxy with an impact parameter of 63 kpc. The cool photoionized gas in the absorber is well modeled with log U ~ -2.6, log N(H) ~17.8, log n(H) ~ -3.3 and [Si/H] = -0.14\pm0.23. The collisionally ionized gas containing C IV and O VI probably arises in cooling shock heated transition temperature gas with log T ~ 5.5. The absorber is likely tracing circumgalactic gas enriched by gas ejected from the spiral emission line galaxy. The simple system at z = 0.14072 only contains O VI and broad and narrow H I. The O VI with b = 33.4\pm11.9 km s-1 is likely associated with the broad H I {\lambda}1215 absorption with b = 86.7\pm15.4 km s-1. The difference in Doppler parameters implies the detection of a very large column of warm gas with log T = 5.61(+0.16, -0.25), log N(H) = 19.54(+0.26, -0.44) and [O/H] = -1.48 (+0.46, -0.26). This absorber is possibly associated with a 1.6L* absorption line galaxy with an impact parameter of 617 kpc although an origin in warm filament gas or in the halo of a fainter galaxy is more likely.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/03/the-properties-of-two-low-redshift-o-vi-absorbers-and-their-associated-galaxies-toward-3c-263/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Dynamical Friction in a magnetized gas</title>
		<link>http://voxcharta.org/2012/05/03/dynamical-friction-in-a-magnetized-gas/</link>
		<comments>http://voxcharta.org/2012/05/03/dynamical-friction-in-a-magnetized-gas/#comments</comments>
		<pubDate>Fri, 04 May 2012 00:40:52 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[ambient medium]]></category>
		<category><![CDATA[analytical solution]]></category>
		<category><![CDATA[density field]]></category>
		<category><![CDATA[dynamical structure]]></category>
		<category><![CDATA[friction force]]></category>
		<category><![CDATA[magnetic effect]]></category>
		<category><![CDATA[magnetic field increases]]></category>
		<category><![CDATA[perturbation]]></category>
		<category><![CDATA[perturbation analysis]]></category>
		<category><![CDATA[point mass]]></category>
		<category><![CDATA[validity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/03/dynamical-friction-in-a-magnetized-gas/</guid>
		<description><![CDATA[When a gravitating point mass moves subsonically through a magnetized and isothermal medium, the dynamical structure of the flow is studied far from the mass using a perturbation analysis. Analytical solutions for the first-order density and the velocity perturbations are presented. Validity of our solutions is restricted to the cases where the Alfven velocity in [...]]]></description>
			<content:encoded><![CDATA[<p>When a gravitating point mass moves subsonically through a magnetized and isothermal medium, the dynamical structure of the flow is studied far from the mass using a perturbation analysis. Analytical solutions for the first-order density and the velocity perturbations are presented. Validity of our solutions is restricted to the cases where the Alfven velocity in the ambient medium is less than the accretor&#8217;s velocity. The density field is less dense because of the magnetic effects according to the solutions and the dynamical friction force becomes lower as the strength of the magnetic field increases.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/03/dynamical-friction-in-a-magnetized-gas/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Tracing Outflows and Accretion: A Bimodal Azimuthal Dependence of MgII Absorption</title>
		<link>http://voxcharta.org/2012/05/02/tracing-outflows-and-accretion-a-bimodal-azimuthal-dependence-of-mgii-absorption/</link>
		<comments>http://voxcharta.org/2012/05/02/tracing-outflows-and-accretion-a-bimodal-azimuthal-dependence-of-mgii-absorption/#comments</comments>
		<pubDate>Thu, 03 May 2012 00:50:33 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorption]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[azimuthal angle]]></category>
		<category><![CDATA[bimodal]]></category>
		<category><![CDATA[dependence]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[minor axis]]></category>
		<category><![CDATA[probability distribution function]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/02/tracing-outflows-and-accretion-a-bimodal-azimuthal-dependence-of-mgii-absorption/</guid>
		<description><![CDATA[We report a bimodality in the azimuthal angle distribution of gas around galaxies as traced by MgII absorption: Halo gas prefers to exist near the projected galaxy major and minor axes. The bimodality is demonstrated by computing the mean azimuthal angle probability distribution function using 88 spectroscopically confirmed MgII absorption-selected galaxies [W_r(2796)&#62; 0.1A] and 35 [...]]]></description>
			<content:encoded><![CDATA[<p>We report a bimodality in the azimuthal angle distribution of gas around galaxies as traced by MgII absorption: Halo gas prefers to exist near the projected galaxy major and minor axes. The bimodality is demonstrated by computing the mean azimuthal angle probability distribution function using 88 spectroscopically confirmed MgII absorption-selected galaxies [W_r(2796)&gt; 0.1A] and 35 spectroscopically confirmed non-absorbing galaxies [W_r(2796)&lt;0.1A] imaged with HST and SDSS. The azimuthal angle distribution for non-absorbers is flat, indicating no azimuthal preference for gas characterized by W_r(2796)&lt;0.1A. We find that blue star-forming galaxies clearly drive the bimodality. We compute an azimuthal angle dependent MgII absorption covering fraction and find that it is enhanced by as much as 20-30% along the major and minor axes. The equivalent width distribution for gas along the major axis is likely skewed toward weaker MgII absorption than for gas along the projected minor axis. These combined results are highly suggestive that the bimodality is driven by gas accreted along the galaxy major axis and outflowing along the galaxy minor axis. The opening angle of outflows is 2.5 times larger than for accreting gas. We find the probably of detecting outflows is 60%, implying that winds are more commonly observed. This scenario is consistent with ideas of galaxy evolution were star-forming galaxies accrete new gas reservoirs, forming new stars and producing winds, while red early-type galaxies exist passively due to a lack of new gas reservoirs to form new stars.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/02/tracing-outflows-and-accretion-a-bimodal-azimuthal-dependence-of-mgii-absorption/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Circum-Galactic Gas and the Isotropic Gamma Ray Background</title>
		<link>http://voxcharta.org/2012/05/02/circum-galactic-gas-and-the-isotropic-gamma-ray-background/</link>
		<comments>http://voxcharta.org/2012/05/02/circum-galactic-gas-and-the-isotropic-gamma-ray-background/#comments</comments>
		<pubDate>Thu, 03 May 2012 00:49:34 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[collisions]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[galactic disk]]></category>
		<category><![CDATA[galactic gas]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[hydrogen]]></category>
		<category><![CDATA[interstellar gas]]></category>
		<category><![CDATA[line of sight]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[observational evidence]]></category>
		<category><![CDATA[radiation field]]></category>
		<category><![CDATA[ray space]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[space telescope]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/02/circum-galactic-gas-and-the-isotropic-gamma-ray-background/</guid>
		<description><![CDATA[Interactions of cosmic rays with the interstellar gas and radiation fields of the Milky Way provide the majority of the gamma rays observed by the Fermi Gamma Ray Space Telescope. In addition to the gas which is densely concentrated along the Galactic Disk, hydrodynamical simulations and observational evidence favor the presence of a halo of [...]]]></description>
			<content:encoded><![CDATA[<p>Interactions of cosmic rays with the interstellar gas and radiation fields of the Milky Way provide the majority of the gamma rays observed by the Fermi Gamma Ray Space Telescope. In addition to the gas which is densely concentrated along the Galactic Disk, hydrodynamical simulations and observational evidence favor the presence of a halo of hot (T~10^6 K) ionized hydrogen (H_II), extending with non-negligible densities out to the virial radius of the Milky Way. We show that cosmic ray collisions with this circum-galactic gas should be expected to provide a significant flux of gamma rays, on the order of 10% of the observed isotopic gamma ray background at energies above 1 GeV. In addition, gamma rays originating from the extended H_II halos of other galaxies along a given line-of-sight should contribute to this background at a similar level.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/02/circum-galactic-gas-and-the-isotropic-gamma-ray-background/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Impact of Contaminated RR Lyrae/Globular Cluster Photometry on the Distance Scale</title>
		<link>http://voxcharta.org/2012/05/02/the-impact-of-contaminated-rr-lyraeglobular-cluster-photometry-on-the-distance-scale/</link>
		<comments>http://voxcharta.org/2012/05/02/the-impact-of-contaminated-rr-lyraeglobular-cluster-photometry-on-the-distance-scale/#comments</comments>
		<pubDate>Thu, 03 May 2012 00:48:06 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absolute magnitude]]></category>
		<category><![CDATA[age of the universe]]></category>
		<category><![CDATA[constituent]]></category>
		<category><![CDATA[contamination]]></category>
		<category><![CDATA[core]]></category>
		<category><![CDATA[dependence]]></category>
		<category><![CDATA[distance scale]]></category>
		<category><![CDATA[globular cluster]]></category>
		<category><![CDATA[impetus]]></category>
		<category><![CDATA[m54]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[photometry]]></category>
		<category><![CDATA[propagation]]></category>
		<category><![CDATA[rr lyrae]]></category>
		<category><![CDATA[scale rr]]></category>
		<category><![CDATA[surface brightness]]></category>
		<category><![CDATA[systematic uncertainty]]></category>
		<category><![CDATA[variables]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/02/the-impact-of-contaminated-rr-lyraeglobular-cluster-photometry-on-the-distance-scale/</guid>
		<description><![CDATA[RR Lyrae variables and the stellar constituents of globular clusters are employed to establish the cosmic distance scale and age of the universe. However, photometry for RR Lyrae variables in the globular clusters M3, M15, M54, M92, NGC2419, and NGC6441 exhibit a dependence on the clustercentric distance. For example, variables and stars positioned near the [...]]]></description>
			<content:encoded><![CDATA[<p>RR Lyrae variables and the stellar constituents of globular clusters are employed to establish the cosmic distance scale and age of the universe. However, photometry for RR Lyrae variables in the globular clusters M3, M15, M54, M92, NGC2419, and NGC6441 exhibit a dependence on the clustercentric distance. For example, variables and stars positioned near the crowded high-surface brightness cores of the clusters may suffer from photometric contamination, which invariably affects a suite of inferred parameters (e.g., distance, color excess, absolute magnitude, etc.). The impetus for this study is to mitigate the propagation of systematic uncertainties by increasing awareness of the pernicious impact of contaminated and radial-dependent photometry.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/02/the-impact-of-contaminated-rr-lyraeglobular-cluster-photometry-on-the-distance-scale/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Dark Matter in the Milky Way&#8217;s Dwarf Spheroidal Satellites</title>
		<link>http://voxcharta.org/2012/05/02/dark-matter-in-the-milky-ways-dwarf-spheroidal-satellites/</link>
		<comments>http://voxcharta.org/2012/05/02/dark-matter-in-the-milky-ways-dwarf-spheroidal-satellites/#comments</comments>
		<pubDate>Thu, 03 May 2012 00:43:52 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[discrepancy]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[luminous galaxies]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[particle nature]]></category>
		<category><![CDATA[phenomenology]]></category>
		<category><![CDATA[satellite]]></category>
		<category><![CDATA[stellar population]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/02/dark-matter-in-the-milky-ways-dwarf-spheroidal-satellites/</guid>
		<description><![CDATA[The Milky Way&#8217;s dwarf spheroidal satellites include the nearest, smallest and least luminous galaxies known. They also exhibit the largest discrepancies between dynamical and luminous masses. This article reviews the development of empirical constraints on the structure and kinematics of dSph stellar populations and discusses how this phenomenology translates into constraints on the amount and [...]]]></description>
			<content:encoded><![CDATA[<p>The Milky Way&#8217;s dwarf spheroidal satellites include the nearest, smallest and least luminous galaxies known. They also exhibit the largest discrepancies between dynamical and luminous masses. This article reviews the development of empirical constraints on the structure and kinematics of dSph stellar populations and discusses how this phenomenology translates into constraints on the amount and distribution of dark matter within dSphs. Some implications for cosmology and the particle nature of dark matter are discussed, and some topics/questions for future study are identified.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/02/dark-matter-in-the-milky-ways-dwarf-spheroidal-satellites/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Massive stars in massive clusters II: Disruption of bound clusters by photoionization</title>
		<link>http://voxcharta.org/2012/05/02/massive-stars-in-massive-clusters-ii-disruption-of-bound-clusters-by-photoionization/</link>
		<comments>http://voxcharta.org/2012/05/02/massive-stars-in-massive-clusters-ii-disruption-of-bound-clusters-by-photoionization/#comments</comments>
		<pubDate>Thu, 03 May 2012 00:43:07 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion flows]]></category>
		<category><![CDATA[disruption]]></category>
		<category><![CDATA[dynamical effects]]></category>
		<category><![CDATA[ejecta]]></category>
		<category><![CDATA[filamentary structure]]></category>
		<category><![CDATA[gravitational potential energy]]></category>
		<category><![CDATA[hii region]]></category>
		<category><![CDATA[ionizing radiation]]></category>
		<category><![CDATA[massive cloud]]></category>
		<category><![CDATA[massive cluster]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[neutral gas]]></category>
		<category><![CDATA[photoionization]]></category>
		<category><![CDATA[photon]]></category>
		<category><![CDATA[profound effect]]></category>
		<category><![CDATA[time window]]></category>
		<category><![CDATA[timescale]]></category>
		<category><![CDATA[turbulent kinetic energy]]></category>
		<category><![CDATA[type star]]></category>
		<category><![CDATA[velocities]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/02/massive-stars-in-massive-clusters-ii-disruption-of-bound-clusters-by-photoionization/</guid>
		<description><![CDATA[We present an SPH parameter study of the dynamical effect of photoionization from O&#8211;type stars on star&#8211;forming clouds of a range of masses and sizes during the time window before supernovae explode. Our model clouds all have the same degree of turbulent support initially, the ratio of turbulent kinetic energy to gravitational potential energy being [...]]]></description>
			<content:encoded><![CDATA[<p>We present an SPH parameter study of the dynamical effect of photoionization from O&#8211;type stars on star&#8211;forming clouds of a range of masses and sizes during the time window before supernovae explode. Our model clouds all have the same degree of turbulent support initially, the ratio of turbulent kinetic energy to gravitational potential energy being set to $E_{\rm kin}/|E_{\rm pot}|$=0.7. We allow the clouds to form stars and study the dynamical effects of the ionizing radiation from the massive stars or clusters born within them. We find that dense filamentary structures and accretion flows limit the quantities of gas that can be ionized, particularly in the higher density clusters. More importantly, the higher escape velocities in our more massive (10$^{6}$M$_{\odot}$) clouds prevent the HII regions from sweeping up and expelling significant quantities of gas, so that the most massive clouds are largely dynamically unaffected by ionizing feedback. However, feedback has a profound effect on the lower&#8211;density 10$^{4}$ and 10$^{5}$M$_{\odot}$ clouds in our study, creating vast evacuated bubbles and expelling tens of percent of the neutral gas in the 3Myr timescale before the first supernovae are expected to detonate, resulting in clouds highly porous to both photons and supernova ejecta.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/02/massive-stars-in-massive-clusters-ii-disruption-of-bound-clusters-by-photoionization/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Detection of the hydroperoxyl radical HO2 toward \rho Oph A: Additional constraints on the water chemical network</title>
		<link>http://voxcharta.org/2012/05/02/detection-of-the-hydroperoxyl-radical-ho2-toward-rho-oph-a-additional-constraints-on-the-water-chemical-network/</link>
		<comments>http://voxcharta.org/2012/05/02/detection-of-the-hydroperoxyl-radical-ho2-toward-rho-oph-a-additional-constraints-on-the-water-chemical-network/#comments</comments>
		<pubDate>Thu, 03 May 2012 00:42:55 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[30m]]></category>
		<category><![CDATA[apex]]></category>
		<category><![CDATA[chemical model]]></category>
		<category><![CDATA[dust grains]]></category>
		<category><![CDATA[fractional abundance]]></category>
		<category><![CDATA[gas phase]]></category>
		<category><![CDATA[grain surface]]></category>
		<category><![CDATA[ho2]]></category>
		<category><![CDATA[hooh]]></category>
		<category><![CDATA[hydrogen peroxide]]></category>
		<category><![CDATA[intermediate product]]></category>
		<category><![CDATA[molecular transitions]]></category>
		<category><![CDATA[network context]]></category>
		<category><![CDATA[observational result]]></category>
		<category><![CDATA[precursor]]></category>
		<category><![CDATA[rho oph]]></category>
		<category><![CDATA[surface reaction]]></category>
		<category><![CDATA[water chemical]]></category>
		<category><![CDATA[water formation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/02/detection-of-the-hydroperoxyl-radical-ho2-toward-rho-oph-a-additional-constraints-on-the-water-chemical-network/</guid>
		<description><![CDATA[Context: Hydrogen peroxide (HOOH) was recently detected toward \rho Oph A. Subsequent astrochemical modeling that included reactions in the gas phase and on the surface of dust grains was able to explain the observed abundance, and highlighted the importance of grain chemistry in the formation of HOOH as an intermediate product in water formation. This [...]]]></description>
			<content:encoded><![CDATA[<p>Context: Hydrogen peroxide (HOOH) was recently detected toward \rho Oph A. Subsequent astrochemical modeling that included reactions in the gas phase and on the surface of dust grains was able to explain the observed abundance, and highlighted the importance of grain chemistry in the formation of HOOH as an intermediate product in water formation. This study also predicted that the hydroperoxyl radical HO2, the precursor of HOOH, should be detectable. Aims: We aim at detecting the hydroperoxyl radical HO2 in \rho Oph A. Methods: We used the IRAM 30m and the APEX telescopes to target the brightest HO2 lines at about 130 and 260 GHz. Results: We detect five lines of HO2 (comprising seven individual molecular transitions). The fractional abundance of HO2 is found to be about 1e-10, a value similar to the abundance of HOOH. This observational result is consistent with the prediction of the above mentioned astrochemical model, and thereby validates our current understanding of the water formation on dust grains. Conclusions: This detection, anticipated by a sophisticated gas-grain chemical model, demonstrates that models of grain chemistry have improved tremendously and that grain surface reactions now form a crucial part of the overall astrochemical network.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/02/detection-of-the-hydroperoxyl-radical-ho2-toward-rho-oph-a-additional-constraints-on-the-water-chemical-network/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The transition mass-loss rate: Calibrating the role of line-driven winds in massive star evolution</title>
		<link>http://voxcharta.org/2012/05/02/the-transition-mass-loss-rate-calibrating-the-role-of-line-driven-winds-in-massive-star-evolution/</link>
		<comments>http://voxcharta.org/2012/05/02/the-transition-mass-loss-rate-calibrating-the-role-of-line-driven-winds-in-massive-star-evolution/#comments</comments>
		<pubDate>Thu, 03 May 2012 00:41:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[arches]]></category>
		<category><![CDATA[driven wind]]></category>
		<category><![CDATA[empirical mass]]></category>
		<category><![CDATA[mass loss rates]]></category>
		<category><![CDATA[mass range]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[order of magnitude]]></category>
		<category><![CDATA[quantification]]></category>
		<category><![CDATA[star evolution]]></category>
		<category><![CDATA[stellar evolution models]]></category>
		<category><![CDATA[stellar wind]]></category>
		<category><![CDATA[theoretical model]]></category>
		<category><![CDATA[theoretical result]]></category>
		<category><![CDATA[transition point]]></category>
		<category><![CDATA[wind strength]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/02/the-transition-mass-loss-rate-calibrating-the-role-of-line-driven-winds-in-massive-star-evolution/</guid>
		<description><![CDATA[A debate has arisen regarding the importance of stationary versus eruptive mass loss for massive star evolution. The reason is that stellar winds have been found to be clumped, which results in the reduction of unclumped empirical mass-loss rates. Most stellar evolution models employ theoretical mass-loss rates which are already reduced by a moderate factor [...]]]></description>
			<content:encoded><![CDATA[<p>A debate has arisen regarding the importance of stationary versus eruptive mass loss for massive star evolution. The reason is that stellar winds have been found to be clumped, which results in the reduction of unclumped empirical mass-loss rates. Most stellar evolution models employ theoretical mass-loss rates which are already reduced by a moderate factor of ~2-3 compared to non-corrected empirical rates. A key question is whether these reduced rates are of the correct order of magnitude, or if they should be reduced even further, which would mean that the alternative of eruptive mass loss becomes necessary. Here we introduce the transition mass-loss rate (dM/dt)_trans between O and Wolf-Rayet (WR) stars. Its novelty is that it is model independent. All that is required is postulating the spectroscopic transition point in a given data-set, and determining the stellar luminosity, which is far less model dependent than the mass-loss rate. The transition mass-loss rate is subsequently used to calibrate stellar wind strength by its application to the Of/WNh stars in the Arches cluster. Good agreement is found with two alternative modelling/theoretical results, suggesting that the rates provided by current theoretical models are of the right order of magnitude in the ~50Msun mass range. Our results do not confirm the specific need for eruptive mass loss as Luminous Blue Variables, and current stellar evolution modelling for Galactic massive stars seems sound. Mass loss through alternative mechanisms might still become necessary at lower masses, and/or metallicities, and the quantification of alternative mass loss is desirable.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/02/the-transition-mass-loss-rate-calibrating-the-role-of-line-driven-winds-in-massive-star-evolution/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>10 pc Scale Circumnuclear Molecular Gas Imaging of Nearby AGNs</title>
		<link>http://voxcharta.org/2012/05/02/10-pc-scale-circumnuclear-molecular-gas-imaging-of-nearby-agns/</link>
		<comments>http://voxcharta.org/2012/05/02/10-pc-scale-circumnuclear-molecular-gas-imaging-of-nearby-agns/#comments</comments>
		<pubDate>Thu, 03 May 2012 00:41:10 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[agns]]></category>
		<category><![CDATA[chemical composition]]></category>
		<category><![CDATA[clear evidence]]></category>
		<category><![CDATA[co line]]></category>
		<category><![CDATA[galaxy m51]]></category>
		<category><![CDATA[galaxy ngc]]></category>
		<category><![CDATA[gas distribution]]></category>
		<category><![CDATA[gas imaging]]></category>
		<category><![CDATA[interferometer]]></category>
		<category><![CDATA[line ratio]]></category>
		<category><![CDATA[molecular gas kinematics]]></category>
		<category><![CDATA[nearby galaxy]]></category>
		<category><![CDATA[plateau]]></category>
		<category><![CDATA[radio galaxy]]></category>
		<category><![CDATA[rotation feature]]></category>
		<category><![CDATA[sma]]></category>
		<category><![CDATA[submillimeter array]]></category>
		<category><![CDATA[unified model]]></category>
		<category><![CDATA[velocity gradient]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/02/10-pc-scale-circumnuclear-molecular-gas-imaging-of-nearby-agns/</guid>
		<description><![CDATA[We present the images and kinematics of circumnuclear molecular gas from 100 pc scale down to 10 pc scale in nearby active galactic nuclei (AGNs) using the Submillimeter Array (SMA) and the Plateau de Bure Interferometer (PdBI). We have observed several nearby galaxies that host AGNs, such as the nearest radio galaxy Centaurus A (NGC [...]]]></description>
			<content:encoded><![CDATA[<p>We present the images and kinematics of circumnuclear molecular gas from 100 pc scale down to 10 pc scale in nearby active galactic nuclei (AGNs) using the Submillimeter Array (SMA) and the Plateau de Bure Interferometer (PdBI). We have observed several nearby galaxies that host AGNs, such as the nearest radio galaxy Centaurus A (NGC 5128), the Seyfert 2 galaxy M51 (NGC 5194), the Seyfert 2 galaxy NGC 1068, the Seyfert 1 galaxy NGC 1097, and the Seyfert 2 / starburst composite galaxy NGC 4945, in CO lines to see whether the molecular gas distribution, kinematics, and physical conditions at 10 &#8211; 100 pc scale follows the AGN unified model or not. In 100 pc scale, most of the circumnuclear molecular gas shows smooth velocity gradient, suggesting a regular rotating feature, and also shows abnormal line ratios, suggesting the existence of active sources to make the circumnuclear molecular gas dense and/or warm conditions or abnormal chemical compositions. In 10 pc scale, on the other hand, the molecular gas kinematics shows various characteristics, some shows very disturbed kinematics such as a jet-entrained feature in the galaxies that have jets, but some still shows regular rotation feature in a galaxy that does not have obvious jets. These results indicate that the kinematics and physical/chemical conditions of the circumnuclear molecular gas at the scale less than 100 pc is highly affected by the AGN activities, and at this scale, there is no clear evidence of any unified feature seen in the circumnuclear molecular gas.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/02/10-pc-scale-circumnuclear-molecular-gas-imaging-of-nearby-agns/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Progress in Understanding the Diffuse UV Cosmic Background</title>
		<link>http://voxcharta.org/2012/05/02/progress-in-understanding-the-diffuse-uv-cosmic-background/</link>
		<comments>http://voxcharta.org/2012/05/02/progress-in-understanding-the-diffuse-uv-cosmic-background/#comments</comments>
		<pubDate>Thu, 03 May 2012 00:39:09 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[background radiation]]></category>
		<category><![CDATA[cosmic background]]></category>
		<category><![CDATA[diffuse background]]></category>
		<category><![CDATA[grating]]></category>
		<category><![CDATA[jayant]]></category>
		<category><![CDATA[lyman alpha]]></category>
		<category><![CDATA[preliminary investigation]]></category>
		<category><![CDATA[sky]]></category>
		<category><![CDATA[solar system]]></category>
		<category><![CDATA[starlight]]></category>
		<category><![CDATA[time measurement]]></category>
		<category><![CDATA[trove]]></category>
		<category><![CDATA[ultraviolet spectrometer]]></category>
		<category><![CDATA[voyager]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/02/progress-in-understanding-the-diffuse-uv-cosmic-background/</guid>
		<description><![CDATA[I report on progress in my ongoing work with Professor Jayant Murthy concerning the origin and nature of the diffuse ultraviolet background radiation over the sky. We have obtained and are reducing a vast trove of Voyager ultraviolet spectrometer observations of the diffuse background shortward of Lyman alpha, including for the first time measurements made [...]]]></description>
			<content:encoded><![CDATA[<p>I report on progress in my ongoing work with Professor Jayant Murthy concerning the origin and nature of the diffuse ultraviolet background radiation over the sky. We have obtained and are reducing a vast trove of Voyager ultraviolet spectrometer observations of the diffuse background shortward of Lyman alpha, including for the first time measurements made from the outermost regions of the solar system, where noise from solar-system scattered (and then grating-scattered) solar Lyman alpha is lowest. Also, we have obtained and are investigating the complete set of GALEX observations of the diffuse ultraviolet background longward of Lyman alpha. Preliminary investigation appears to confirm that longward of Lyman alpha there exists a component of the diffuse ultraviolet background that is not dust-scattered starlight.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/02/progress-in-understanding-the-diffuse-uv-cosmic-background/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Ionized gas diagnostics from protoplanetary discs in the Orion Nebula and the abundance discrepancy problem</title>
		<link>http://voxcharta.org/2012/05/02/ionized-gas-diagnostics-from-protoplanetary-discs-in-the-orion-nebula-and-the-abundance-discrepancy-problem/</link>
		<comments>http://voxcharta.org/2012/05/02/ionized-gas-diagnostics-from-protoplanetary-discs-in-the-orion-nebula-and-the-abundance-discrepancy-problem/#comments</comments>
		<pubDate>Thu, 03 May 2012 00:37:31 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[adf]]></category>
		<category><![CDATA[background contamination]]></category>
		<category><![CDATA[background gas]]></category>
		<category><![CDATA[background subtraction]]></category>
		<category><![CDATA[beta coefficient]]></category>
		<category><![CDATA[density gas]]></category>
		<category><![CDATA[distribution maps]]></category>
		<category><![CDATA[electron density]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[field spectroscopy]]></category>
		<category><![CDATA[high density]]></category>
		<category><![CDATA[high velocity]]></category>
		<category><![CDATA[integral field]]></category>
		<category><![CDATA[ionic abundances]]></category>
		<category><![CDATA[line ratio]]></category>
		<category><![CDATA[orion nebula]]></category>
		<category><![CDATA[physical model]]></category>
		<category><![CDATA[recombination lines]]></category>
		<category><![CDATA[spatial distribution]]></category>
		<category><![CDATA[typical value]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/02/ionized-gas-diagnostics-from-protoplanetary-discs-in-the-orion-nebula-and-the-abundance-discrepancy-problem/</guid>
		<description><![CDATA[We present results from integral field spectroscopy with PMAS. The observed field contains: five protoplanetary discs (also known as proplyds), the high-velocity jet HH 514 and a bowshock. Spatial distribution maps are obtained for different emission line fluxes, the c(H{\beta}) coefficient, electron densities and temperatures, ionic abundances of different ions from collisionally excited lines (CELs), [...]]]></description>
			<content:encoded><![CDATA[<p>We present results from integral field spectroscopy with PMAS. The observed field contains: five protoplanetary discs (also known as proplyds), the high-velocity jet HH 514 and a bowshock. Spatial distribution maps are obtained for different emission line fluxes, the c(H{\beta}) coefficient, electron densities and temperatures, ionic abundances of different ions from collisionally excited lines (CELs), C2+ and O2+ abundances from recombination lines (RLs) and the abundance discrepancy factor of O2+, ADF(O2+). We find that collisional de-excitation has a major influence on the line fluxes in the proplyds. If this is not properly accounted for then physical conditions deduced from commonly used line ratios will be in error, leading to unreliable chemical abundances for these objects. We obtain the intrinsic emission of the proplyds 177-341, 170-337 and 170-334 by a direct subtraction of the background emission, though the last two present some background contamination due to their small sizes. A detailed analysis of 177-341 spectra reveals the presence of high-density gas (3.8\times10^5 cm^-3) in contrast to the typical values observed in the background gas of the nebula (3800 cm^-3). We also explore how the background subtraction could be affected by the possible opacity of the proplyd. We construct a physical model for the proplyd 177-341 finding a good agreement between the predicted and observed line ratios. Finally, we find that the use of reliable physical conditions returns an ADF(O2+) about zero for the intrinsic spectra of 177-341, while the background emission presents the typical ADF(O2+) observed in the Orion Nebula. We conclude that the presence of high-density ionized gas is severely affecting the abundances determined from CELs and, therefore, those from RLs should be considered as a better approximation to the true abundances.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/02/ionized-gas-diagnostics-from-protoplanetary-discs-in-the-orion-nebula-and-the-abundance-discrepancy-problem/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A First Look at Galaxy Flyby Interactions: I. Characterizing the Frequency of Flybys in a Cosmological Context [Replacement]</title>
		<link>http://voxcharta.org/2012/05/02/a-first-look-at-galaxy-flyby-interactions-i-characterizing-the-frequency-of-flybys-in-a-cosmological-context-replacement/</link>
		<comments>http://voxcharta.org/2012/05/02/a-first-look-at-galaxy-flyby-interactions-i-characterizing-the-frequency-of-flybys-in-a-cosmological-context-replacement/#comments</comments>
		<pubDate>Thu, 03 May 2012 00:35:07 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[analytic model]]></category>
		<category><![CDATA[anomaly]]></category>
		<category><![CDATA[body simulation]]></category>
		<category><![CDATA[cosmological context]]></category>
		<category><![CDATA[dark matter halo]]></category>
		<category><![CDATA[dynamical evolution]]></category>
		<category><![CDATA[dynamical interaction]]></category>
		<category><![CDATA[flyby]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[galaxy evolution]]></category>
		<category><![CDATA[galaxy merger]]></category>
		<category><![CDATA[hierarchical level]]></category>
		<category><![CDATA[hierarchical structure formation]]></category>
		<category><![CDATA[interaction history]]></category>
		<category><![CDATA[mass ratio]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[tentative evidence]]></category>
		<category><![CDATA[typical classes]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/02/a-first-look-at-galaxy-flyby-interactions-i-characterizing-the-frequency-of-flybys-in-a-cosmological-context-replacement/</guid>
		<description><![CDATA[Hierarchical structure formation theory is based on the notion that mergers drive galaxy evolution, so a considerable framework of semi-analytic models and N-body simulations has been constructed to calculate how mergers transform a growing galaxy. However, galaxy mergers are only one type of major dynamical interaction between halos &#8212; another class of encounter, a close [...]]]></description>
			<content:encoded><![CDATA[<p>Hierarchical structure formation theory is based on the notion that mergers drive galaxy evolution, so a considerable framework of semi-analytic models and N-body simulations has been constructed to calculate how mergers transform a growing galaxy. However, galaxy mergers are only one type of major dynamical interaction between halos &#8212; another class of encounter, a close flyby, has been largely ignored. We use cosmological N-body simulations to reconstruct the entire dynamical interaction history of dark matter halos. We present a careful method of identifying and tracking a dark matter halo which resolves the typical classes of anomalies that occur in N-body data. This technique allows us to robustly follow halos and several hierarchical levels of subhalos as they grow, dissolve, merge, and flyby one another &#8212; thereby constructing both a census of the dynamical interactions in a volume and an archive of the dynamical evolution of an individual halo. In addition to a census of mergers, our tool characterizes the frequency of close flyby interactions in the Universe. We find that the number of close flyby interactions is comparable to, or even surpasses, the number of mergers for halo masses $\gtrsim 10^{11}\,\Msun$ at $z \lesssim 2$. Halo flybys occur so frequently to high mass halos that they are continually perturbed, unable to reach a dynamical equilibrium. In particular, we find that Milky Way type halos undergo a similar number of flybys as mergers irrespective of mass-ratio for $z\lesssim 2$. We also find tentative evidence that at high redshift, $z \gtrsim 14$, flybys are as frequent as mergers. Our results suggest that close halo flybys can play an important role in the evolution of the earliest dark matter halos and their galaxies, and can still influence galaxy evolution at the present epoch. [Abridged]</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/02/a-first-look-at-galaxy-flyby-interactions-i-characterizing-the-frequency-of-flybys-in-a-cosmological-context-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Formation of Massive Black Holes in Dense Star Clusters. II. IMF and Primordial Mass Segregation [Replacement]</title>
		<link>http://voxcharta.org/2012/05/02/formation-of-massive-black-holes-in-dense-star-clusters-ii-imf-and-primordial-mass-segregation-replacement/</link>
		<comments>http://voxcharta.org/2012/05/02/formation-of-massive-black-holes-in-dense-star-clusters-ii-imf-and-primordial-mass-segregation-replacement/#comments</comments>
		<pubDate>Thu, 03 May 2012 00:34:29 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[cluster mass]]></category>
		<category><![CDATA[core collapse]]></category>
		<category><![CDATA[dense star]]></category>
		<category><![CDATA[explicit treatment]]></category>
		<category><![CDATA[hole mass]]></category>
		<category><![CDATA[imf]]></category>
		<category><![CDATA[initial mass function]]></category>
		<category><![CDATA[main sequence star]]></category>
		<category><![CDATA[massive cluster]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[relaxation time]]></category>
		<category><![CDATA[runaway growth]]></category>
		<category><![CDATA[segregation]]></category>
		<category><![CDATA[star cluster]]></category>
		<category><![CDATA[stellar collisions]]></category>
		<category><![CDATA[tcc]]></category>
		<category><![CDATA[vms]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/02/formation-of-massive-black-holes-in-dense-star-clusters-ii-imf-and-primordial-mass-segregation-replacement/</guid>
		<description><![CDATA[A promising mechanism to form intermediate-mass black holes (IMBHs) is the runaway merger in dense star clusters, where main-sequence stars collide and form a very massive star (VMS), which then collapses to a black hole. In this paper we study the effects of primordial mass segregation and the importance of the stellar initial mass function [...]]]></description>
			<content:encoded><![CDATA[<p>A promising mechanism to form intermediate-mass black holes (IMBHs) is the runaway merger in dense star clusters, where main-sequence stars collide and form a very massive star (VMS), which then collapses to a black hole. In this paper we study the effects of primordial mass segregation and the importance of the stellar initial mass function (IMF) on the runaway growth of VMSs using a dynamical Monte Carlo code for N-body systems with N as high as 10^6 stars. Our code now includes an explicit treatment of all stellar collisions. We place special emphasis on the possibility of top-heavy IMFs, as observed in some very young massive clusters. We find that both primordial mass segregation and the shape of the IMF affect the rate of core collapse of star clusters and thus the time of the runaway. When we include primordial mass segregation we generally see a decrease in core collapse time (tcc). Moreover, primordial mass segregation increases the average mass in the core, thus reducing the central relaxation time, which also decreases tcc. The final mass of the VMS formed is always close to \sim 10^-3 of the total cluster mass, in agreement with the previous studies and is reminiscent of the observed correlation between the central black hole mass and the bulge mass of the galaxies. As the degree of primordial mass segregation is increased, the mass of the VMS increases at most by a factor of 3. Flatter IMFs generally increase the average mass in the whole cluster, which increases tcc. For the range of IMFs investigated in this paper, this increase in tcc is to some degree balanced by stellar collisions, which accelerate core collapse. Thus there is no significant change in tcc for the somewhat flatter global IMFs observed in very young massive clusters.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/02/formation-of-massive-black-holes-in-dense-star-clusters-ii-imf-and-primordial-mass-segregation-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Herschel-SPIRE Imaging Spectroscopy of Molecular Gas in M82</title>
		<link>http://voxcharta.org/2012/05/01/herschel-spire-imaging-spectroscopy-of-molecular-gas-in-m82/</link>
		<comments>http://voxcharta.org/2012/05/01/herschel-spire-imaging-spectroscopy-of-molecular-gas-in-m82/#comments</comments>
		<pubDate>Wed, 02 May 2012 00:48:43 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[central position]]></category>
		<category><![CDATA[co line]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[density column]]></category>
		<category><![CDATA[density gradient]]></category>
		<category><![CDATA[galaxy m82]]></category>
		<category><![CDATA[hcn]]></category>
		<category><![CDATA[hco]]></category>
		<category><![CDATA[herschel]]></category>
		<category><![CDATA[high temperature]]></category>
		<category><![CDATA[likelihood analysis]]></category>
		<category><![CDATA[line ratio]]></category>
		<category><![CDATA[micron]]></category>
		<category><![CDATA[molecular hydrogen]]></category>
		<category><![CDATA[radiative transfer code]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[spire]]></category>
		<category><![CDATA[starburst galaxy]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/01/herschel-spire-imaging-spectroscopy-of-molecular-gas-in-m82/</guid>
		<description><![CDATA[We present new Herschel-SPIRE imaging spectroscopy (194-671 microns) of the bright starburst galaxy M82. Covering the CO ladder from J=4-3 to J=13-12, spectra were obtained at multiple positions for a fully sampled ~ 3 x 3 arcminute map, including a longer exposure at the central position. We present measurements of 12CO, 13CO, [CI], [NII], HCN, [...]]]></description>
			<content:encoded><![CDATA[<p>We present new Herschel-SPIRE imaging spectroscopy (194-671 microns) of the bright starburst galaxy M82. Covering the CO ladder from J=4-3 to J=13-12, spectra were obtained at multiple positions for a fully sampled ~ 3 x 3 arcminute map, including a longer exposure at the central position. We present measurements of 12CO, 13CO, [CI], [NII], HCN, and HCO+ in emission, along with OH+, H2O+ and HF in absorption and H2O in both emission and absorption, with discussion. We use a radiative transfer code and Bayesian likelihood analysis to model the temperature, density, column density, and filling factor of multiple components of molecular gas traced by 12CO and 13CO, adding further evidence to the high-J lines tracing a much warmer (~ 500 K), less massive component than the low-J lines. The addition of 13CO (and [CI]) is new and indicates that [CI] may be tracing different gas than 12CO. No temperature/density gradients can be inferred from the map, indicating that the single-pointing spectrum is descriptive of the bulk properties of the galaxy. At such a high temperature, cooling is dominated by molecular hydrogen. Photon-dominated region (PDR) models require higher densities than those indicated by our Bayesian likelihood analysis in order to explain the high-J CO line ratios, though cosmic-ray enhanced PDR models can do a better job reproducing the emission at lower densities. Shocks and turbulent heating are likely required to explain the bright high-J emission.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/01/herschel-spire-imaging-spectroscopy-of-molecular-gas-in-m82/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Simulations of High-Velocity Clouds. II. Ablation from High-Velocity Clouds as a Source of Low-Velocity High Ions</title>
		<link>http://voxcharta.org/2012/05/01/simulations-of-high-velocity-clouds-ii-ablation-from-high-velocity-clouds-as-a-source-of-low-velocity-high-ions/</link>
		<comments>http://voxcharta.org/2012/05/01/simulations-of-high-velocity-clouds-ii-ablation-from-high-velocity-clouds-as-a-source-of-low-velocity-high-ions/#comments</comments>
		<pubDate>Wed, 02 May 2012 00:46:36 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[ablation]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[composite model]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[environmental gas]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[external radiation]]></category>
		<category><![CDATA[galactic halo]]></category>
		<category><![CDATA[high velocity]]></category>
		<category><![CDATA[hydrodynamic]]></category>
		<category><![CDATA[mixture]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[nitrogen]]></category>
		<category><![CDATA[oxygen ions]]></category>
		<category><![CDATA[photoionization]]></category>
		<category><![CDATA[radiation field]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[supernova remnant]]></category>
		<category><![CDATA[velocities]]></category>
		<category><![CDATA[velocity clouds]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/01/simulations-of-high-velocity-clouds-ii-ablation-from-high-velocity-clouds-as-a-source-of-low-velocity-high-ions/</guid>
		<description><![CDATA[In order to determine if the material ablated from high-velocity clouds (HVCs) is a significant source of low-velocity high ions (C IV, N V, and O VI) such as those found in the Galactic halo, we simulate the hydrodynamics of the gas and the time-dependent ionization evolution of its carbon, nitrogen, and oxygen ions. Our [...]]]></description>
			<content:encoded><![CDATA[<p>In order to determine if the material ablated from high-velocity clouds (HVCs) is a significant source of low-velocity high ions (C IV, N V, and O VI) such as those found in the Galactic halo, we simulate the hydrodynamics of the gas and the time-dependent ionization evolution of its carbon, nitrogen, and oxygen ions. Our suite of simulations examines the ablation of warm material from clouds of various sizes, densities, and velocities as they pass through the hot Galactic halo. The ablated material mixes with the environmental gas, producing an intermediate-temperature mixture that is rich in high ions and that slows to the speed of the surrounding gas. We find that the slow mixed material is a significant source of the low-velocity O VI that is observed in the halo, as it can account for at least ~1/3 of the observed O VI column density. Hence, any complete model of the high ions in the halo should include the contribution to the O VI from ablated HVC material. However, such material is unlikely to be a major source of the observed C IV, presumably because the observed C IV is affected by photoionization, which our models do not include. We discuss a composite model that includes contributions from HVCs, supernova remnants, a cooling Galactic fountain, and photoionization by an external radiation field. By design, this model matches the observed O VI column density. This model can also account for most or all of the observed C IV, but only half of the observed N V.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/01/simulations-of-high-velocity-clouds-ii-ablation-from-high-velocity-clouds-as-a-source-of-low-velocity-high-ions/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Anchoring the Distance Scale via X-ray/IR Data for Cepheid Clusters: SU Cas</title>
		<link>http://voxcharta.org/2012/05/01/anchoring-the-distance-scale-via-x-rayir-data-for-cepheid-clusters-su-cas/</link>
		<comments>http://voxcharta.org/2012/05/01/anchoring-the-distance-scale-via-x-rayir-data-for-cepheid-clusters-su-cas/#comments</comments>
		<pubDate>Wed, 02 May 2012 00:45:24 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[2mass]]></category>
		<category><![CDATA[calibration]]></category>
		<category><![CDATA[cepheid]]></category>
		<category><![CDATA[cluster]]></category>
		<category><![CDATA[delta cep]]></category>
		<category><![CDATA[distance]]></category>
		<category><![CDATA[distance scale]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[iue]]></category>
		<category><![CDATA[omm]]></category>
		<category><![CDATA[proper motion]]></category>
		<category><![CDATA[pulsation]]></category>
		<category><![CDATA[ray observations]]></category>
		<category><![CDATA[select group]]></category>
		<category><![CDATA[star cluster]]></category>
		<category><![CDATA[tandem]]></category>
		<category><![CDATA[trigonometric]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xmm newton]]></category>
		<category><![CDATA[zeta gem]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/01/anchoring-the-distance-scale-via-x-rayir-data-for-cepheid-clusters-su-cas/</guid>
		<description><![CDATA[New X-ray (XMM-Newton) and JHKs (OMM) observations for members of the star cluster Alessi 95, which Turner et al.(2012) discovered hosts the classical Cepheid SU Cas, were used in tandem with UCAC3 (proper motion) and 2MASS observations to determine precise cluster parameters: E(J-H)=0.08+-0.02 and d=405+-15 pc. The ensuing consensus among cluster, pulsation, IUE, and trigonometric [...]]]></description>
			<content:encoded><![CDATA[<p>New X-ray (XMM-Newton) and JHKs (OMM) observations for members of the star cluster Alessi 95, which Turner et al.(2012) discovered hosts the classical Cepheid SU Cas, were used in tandem with UCAC3 (proper motion) and 2MASS observations to determine precise cluster parameters: E(J-H)=0.08+-0.02 and d=405+-15 pc. The ensuing consensus among cluster, pulsation, IUE, and trigonometric distances (d=414+-5(se)+-10(sd) pc) places SU Cas in a select group of nearby fundamental Cepheid calibrators (Delta Cep, Zeta Gem). High-resolution X-ray observations may be employed to expand that sample as the data proved pertinent for identifying numerous stars associated with SU Cas. Acquiring X-ray observations of additional fields may foster efforts to refine Cepheid calibrations used to constrain H_0.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/01/anchoring-the-distance-scale-via-x-rayir-data-for-cepheid-clusters-su-cas/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>20 cm VLA Radio-Continuum Study of M31 &#8211; Images and Point Source Catalogues</title>
		<link>http://voxcharta.org/2012/05/01/20-cm-vla-radio-continuum-study-of-m31-images-and-point-source-catalogues/</link>
		<comments>http://voxcharta.org/2012/05/01/20-cm-vla-radio-continuum-study-of-m31-images-and-point-source-catalogues/#comments</comments>
		<pubDate>Wed, 02 May 2012 00:41:40 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[continuum images]]></category>
		<category><![CDATA[continuum observations]]></category>
		<category><![CDATA[high angular resolution]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[high sensitivity]]></category>
		<category><![CDATA[Lambda]]></category>
		<category><![CDATA[new image]]></category>
		<category><![CDATA[point source]]></category>
		<category><![CDATA[radio continuum]]></category>
		<category><![CDATA[rms]]></category>
		<category><![CDATA[source catalogue]]></category>
		<category><![CDATA[telescope image]]></category>
		<category><![CDATA[very large array]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/01/20-cm-vla-radio-continuum-study-of-m31-images-and-point-source-catalogues/</guid>
		<description><![CDATA[We present a series of new high-sensitivity and high-resolution radio-continuum images of M31 at \lambda=20 cm (\nu=1.4 GHz). These new images were produced by merging archived 20 cm radio-continuum observations from the Very Large Array (VLA) telescope. Images presented here are sensitive to rms=60 \mu Jy and feature high angular resolution (&#60;10&#34;). A complete sample [...]]]></description>
			<content:encoded><![CDATA[<p>We present a series of new high-sensitivity and high-resolution radio-continuum images of M31 at \lambda=20 cm (\nu=1.4 GHz). These new images were produced by merging archived 20 cm radio-continuum observations from the Very Large Array (VLA) telescope. Images presented here are sensitive to rms=60 \mu Jy and feature high angular resolution (&lt;10&quot;). A complete sample of discrete radio sources have been catalogued and analysed across 17 individual VLA projects. We identified a total of 864 unique discrete radio sources across the field of M31. One of the most prominent regions in M31 is the ring feature for which we estimated total integrated flux of 706 mJy at \lambda=20 cm. We compare here, detected sources to those listed in Gelfand et al. (2004) at \lambda=92 cm and find 118 sources in common to both surveys. The majority (61%) of these sources exhibit a spectral index of \alpha &lt;-0.6 indicating that their emission is predominantly non-thermal in nature. That is more typical for background objects.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/01/20-cm-vla-radio-continuum-study-of-m31-images-and-point-source-catalogues/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A 10 kpc Scale Seyfert Galaxy Outflow: HST/COS Observations of IRAS F22456-5125</title>
		<link>http://voxcharta.org/2012/05/01/a-10-kpc-scale-seyfert-galaxy-outflow-hstcos-observations-of-iras-f22456-5125/</link>
		<comments>http://voxcharta.org/2012/05/01/a-10-kpc-scale-seyfert-galaxy-outflow-hstcos-observations-of-iras-f22456-5125/#comments</comments>
		<pubDate>Wed, 02 May 2012 00:38:14 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[central source]]></category>
		<category><![CDATA[civ]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[cosmic origin]]></category>
		<category><![CDATA[distance]]></category>
		<category><![CDATA[fuse]]></category>
		<category><![CDATA[galactic wind]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[hubble space telescope]]></category>
		<category><![CDATA[ira]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[number density]]></category>
		<category><![CDATA[outflow]]></category>
		<category><![CDATA[siii]]></category>
		<category><![CDATA[transition]]></category>
		<category><![CDATA[trough]]></category>
		<category><![CDATA[uv spectrum]]></category>
		<category><![CDATA[velocities]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/01/a-10-kpc-scale-seyfert-galaxy-outflow-hstcos-observations-of-iras-f22456-5125/</guid>
		<description><![CDATA[We present analysis of the UV-spectrum of the low-z AGN IRAS-F22456-5125 obtained with the Cosmic Origins Spectrograph on board the Hubble Space Telescope. The spectrum reveals six main kinematic components, spanning a range of velocities of up to 800 km s-1, which for the first time are observed in troughs associated with CII, CIV, NV, [...]]]></description>
			<content:encoded><![CDATA[<p>We present analysis of the UV-spectrum of the low-z AGN IRAS-F22456-5125 obtained with the Cosmic Origins Spectrograph on board the Hubble Space Telescope. The spectrum reveals six main kinematic components, spanning a range of velocities of up to 800 km s-1, which for the first time are observed in troughs associated with CII, CIV, NV, SiII, SiIII, SiIV and SIV. We also obtain data on the OVI troughs, which we compare to those available from an earlier FUSE epoch. Column densities measured from these ions allow us to derive a well-constrained photoionization solution for each outflow component. Two of these kinematic components show troughs associated with transitions from excited states of SiII\ and CII. The number density inferred from these troughs, in combination with the deduced ioinization parameter, allows us to determine the distance to these outflow components from the central source. We find these components to be at a distance of ~ 10 kpc. The distances and the number densities derived are consistent with the outflow being part of a galactic wind.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/01/a-10-kpc-scale-seyfert-galaxy-outflow-hstcos-observations-of-iras-f22456-5125/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>The Chandra View of NGC 4178: The Lowest Mass Black Hole in a Bulgeless Disk Galaxy?</title>
		<link>http://voxcharta.org/2012/05/01/the-chandra-view-of-ngc-4178-the-lowest-mass-black-hole-in-a-bulgeless-disk-galaxy/</link>
		<comments>http://voxcharta.org/2012/05/01/the-chandra-view-of-ngc-4178-the-lowest-mass-black-hole-in-a-bulgeless-disk-galaxy/#comments</comments>
		<pubDate>Wed, 02 May 2012 00:37:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[chandra data]]></category>
		<category><![CDATA[disk galaxy]]></category>
		<category><![CDATA[ergs]]></category>
		<category><![CDATA[faintness]]></category>
		<category><![CDATA[fundamental plane]]></category>
		<category><![CDATA[hardness ratio]]></category>
		<category><![CDATA[hole mass]]></category>
		<category><![CDATA[imbh]]></category>
		<category><![CDATA[law model]]></category>
		<category><![CDATA[nuclear sources]]></category>
		<category><![CDATA[ray binaries]]></category>
		<category><![CDATA[ray point]]></category>
		<category><![CDATA[ray sources]]></category>
		<category><![CDATA[spectral analysis]]></category>
		<category><![CDATA[spectral property]]></category>
		<category><![CDATA[ULX]]></category>
		<category><![CDATA[vla data]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/01/the-chandra-view-of-ngc-4178-the-lowest-mass-black-hole-in-a-bulgeless-disk-galaxy/</guid>
		<description><![CDATA[Using high resolution Chandra data, we report the presence of a weak X-ray point source coincident with the nucleus of NGC 4178, a late-type bulgeless disk galaxy known to have high ionization mid-infrared (mid-IR) lines typically associated with active galactic nuclei (AGNs). Although the faintness of this source precludes a direct spectral analysis, we are [...]]]></description>
			<content:encoded><![CDATA[<p>Using high resolution Chandra data, we report the presence of a weak X-ray point source coincident with the nucleus of NGC 4178, a late-type bulgeless disk galaxy known to have high ionization mid-infrared (mid-IR) lines typically associated with active galactic nuclei (AGNs). Although the faintness of this source precludes a direct spectral analysis, we are able to infer its basic spectral properties using hardness ratios. X-ray modeling, combined with the nuclear mid-IR characteristics, suggests that NGC 4178 may host a highly absorbed AGN accreting at a high rate with a bolometric luminosity on order of 10^43 ergs/s. The black hole mass estimate, based on our Chandra data and archival VLA data using the most recent fundamental plane relations is \sim 10^4 &#8211; 10^5 M\odot, possibly the lowest mass nuclear black hole currently known. There are also three off-nuclear sources, two with a similar brightness to the nuclear source at 36&#8243; and 32&#8243; from the center. As with the nuclear source, hardness ratios are used to estimate spectra for these two sources, and both are consistent with a simple power- law model with absorption. These two sources have X-ray luminosities of the order of \sim 10^38 ergs/s, which place them at the threshold between X-ray binaries and ultra-luminous X-ray sources (ULXs). The third off-nuclear source, located 49&#8243; from the center, is the brightest source detected, with an X-ray luminosity of \sim 10^40 ergs/s. Its spectrum is well-fit with an absorbed power law model, suggesting that it is a ULX. We also fit its spectrum with the Bulk Motion Comptonization (BMC) model and suggest that this source is consistent with an intermediate-mass black hole (IMBH) of mass (6\times2)\times10^3 M\odot.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/01/the-chandra-view-of-ngc-4178-the-lowest-mass-black-hole-in-a-bulgeless-disk-galaxy/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>The Assembly History of Disk Galaxies: II. Probing the Emerging Tully-Fisher Relation During 1&lt;z&lt;1.7 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/01/the-assembly-history-of-disk-galaxies-ii-probing-the-emerging-tully-fisher-relation-during-1z1-7-replacement/</link>
		<comments>http://voxcharta.org/2012/05/01/the-assembly-history-of-disk-galaxies-ii-probing-the-emerging-tully-fisher-relation-during-1z1-7-replacement/#comments</comments>
		<pubDate>Wed, 02 May 2012 00:34:06 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[disk galaxy]]></category>
		<category><![CDATA[fisher]]></category>
		<category><![CDATA[tully]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/01/the-assembly-history-of-disk-galaxies-ii-probing-the-emerging-tully-fisher-relation-during-1z1-7-replacement/</guid>
		<description><![CDATA[Through extended integrations using the recently-installed deep depletion CCD on the red arm of the Keck I Low Resolution Imaging Spectrograph, we present new measurements of the resolved spectra of 70 morphologically-selected star-forming galaxies with i_AB&#60;24.1 in the redshift range 1&#60;z2. Remarkably, we find a well-defined Tully-Fisher relation with up to 60% increase in scatter [...]]]></description>
			<content:encoded><![CDATA[<p>Through extended integrations using the recently-installed deep depletion CCD on the red arm of the Keck I Low Resolution Imaging Spectrograph, we present new measurements of the resolved spectra of 70 morphologically-selected star-forming galaxies with i_AB&lt;24.1 in the redshift range 1&lt;z2. Remarkably, we find a well-defined Tully-Fisher relation with up to 60% increase in scatter and stellar mass zero-point shift constraint of 0.02+/-0.02 dex since z~1.7, compared to the local relation. Although our sample is incomplete in terms of either a fixed stellar mass or star formation rate limit, we discuss the implications that typical star-forming disk galaxies evolve to arrive on a well-defined Tully-Fisher relation within a surprisingly short period of cosmic history.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/01/the-assembly-history-of-disk-galaxies-ii-probing-the-emerging-tully-fisher-relation-during-1z1-7-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Lives of High Redshift Mergers [Replacement]</title>
		<link>http://voxcharta.org/2012/05/01/the-lives-of-high-redshift-mergers-replacement/</link>
		<comments>http://voxcharta.org/2012/05/01/the-lives-of-high-redshift-mergers-replacement/#comments</comments>
		<pubDate>Wed, 02 May 2012 00:32:13 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[body simulation]]></category>
		<category><![CDATA[coalescence]]></category>
		<category><![CDATA[comparative study]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[definitions]]></category>
		<category><![CDATA[duration]]></category>
		<category><![CDATA[formulae]]></category>
		<category><![CDATA[friction]]></category>
		<category><![CDATA[hybrid model]]></category>
		<category><![CDATA[mass range]]></category>
		<category><![CDATA[merger]]></category>
		<category><![CDATA[merger time]]></category>
		<category><![CDATA[practical application]]></category>
		<category><![CDATA[robust approximation]]></category>
		<category><![CDATA[tidal disruption]]></category>
		<category><![CDATA[timescale]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/01/the-lives-of-high-redshift-mergers-replacement/</guid>
		<description><![CDATA[We present a comparative study of recent works on merger-timescales with dynamical friction and find a strong contrast between idealized/isolated mergers (Boylan-Kolchin et al. 2008) and mergers from a cosmological volume (Jiang et al. 2008). Our study measures the duration of mergers in a cosmological N-body simulation of dark matter, with emphasis on higher redshifts [...]]]></description>
			<content:encoded><![CDATA[<p>We present a comparative study of recent works on merger-timescales with dynamical friction and find a strong contrast between idealized/isolated mergers (Boylan-Kolchin et al. 2008) and mergers from a cosmological volume (Jiang et al. 2008). Our study measures the duration of mergers in a cosmological N-body simulation of dark matter, with emphasis on higher redshifts (z &lt; 10) and a lower mass range. In our analysis we consider and compare two merger definitions; tidal disruption and coalescence. We find that the merger-time formula proposed by Jiang et al. (2008) describes our results well and conclude that cosmologically motivated merger-time formulae provide a more versatile and statistically robust approximation for practical applications such as semi-analytic/hybrid models.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/01/the-lives-of-high-redshift-mergers-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The M16 molecular complex under the influence of NGC6611. Herschel&#8217;s perspective of the heating effect on the Eagle Nebula</title>
		<link>http://voxcharta.org/2012/04/30/the-m16-molecular-complex-under-the-influence-of-ngc6611-herschels-perspective-of-the-heating-effect-on-the-eagle-nebula/</link>
		<comments>http://voxcharta.org/2012/04/30/the-m16-molecular-complex-under-the-influence-of-ngc6611-herschels-perspective-of-the-heating-effect-on-the-eagle-nebula/#comments</comments>
		<pubDate>Tue, 01 May 2012 01:03:12 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[density maps]]></category>
		<category><![CDATA[diffuse cloud]]></category>
		<category><![CDATA[eagle nebula m16]]></category>
		<category><![CDATA[filament]]></category>
		<category><![CDATA[filamentary structure]]></category>
		<category><![CDATA[herschel]]></category>
		<category><![CDATA[high mass]]></category>
		<category><![CDATA[initial condition]]></category>
		<category><![CDATA[m 500]]></category>
		<category><![CDATA[mass star]]></category>
		<category><![CDATA[millimetre]]></category>
		<category><![CDATA[penetration depth]]></category>
		<category><![CDATA[pillars of creation]]></category>
		<category><![CDATA[protostar]]></category>
		<category><![CDATA[spectral energy distribution]]></category>
		<category><![CDATA[star cluster]]></category>
		<category><![CDATA[temperature gradient]]></category>
		<category><![CDATA[three dimensional geometry]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/30/the-m16-molecular-complex-under-the-influence-of-ngc6611-herschels-perspective-of-the-heating-effect-on-the-eagle-nebula/</guid>
		<description><![CDATA[We present Herschel images from the HOBYS key program of the Eagle Nebula (M16) in the far-infrared and sub-millimetre, using the PACS and SPIRE cameras at 70{\mu}m, 160{\mu}m, 250{\mu}m, 350{\mu}m, 500{\mu}m. M16, home to the Pillars of Creation, is largely under the influence of the nearby NGC6611 high-mass star cluster. The Herschel images reveal a [...]]]></description>
			<content:encoded><![CDATA[<p>We present Herschel images from the HOBYS key program of the Eagle Nebula (M16) in the far-infrared and sub-millimetre, using the PACS and SPIRE cameras at 70{\mu}m, 160{\mu}m, 250{\mu}m, 350{\mu}m, 500{\mu}m. M16, home to the Pillars of Creation, is largely under the influence of the nearby NGC6611 high-mass star cluster. The Herschel images reveal a clear dust temperature gradient running away from the centre of the cavity carved by the OB cluster. We investigate the heating effect of NGC6611 on the entire M16 star-forming complex seen by Herschel including the diffuse cloud environment and the dense filamentary structures identified in this region. In addition, we interpret the three-dimensional geometry of M16 with respect to the nebula, its surrounding environment, and the NGC6611 cavity. The dust temperature and column density maps reveal a prominent eastern filament running north-south and away from the high-mass star-forming central region and the NGC6611 cluster, as well as a northern filament which extends around and away from the cluster. The dust temperature in each of these filaments decreases with increasing distance from the NGC6611 cluster, indicating a heating penetration depth of \sim 10 pc in each direction in 3 &#8211; 6 \times 10^{22} cm-2 column density filaments. We show that in high-mass star-forming regions OB clusters impact the temperature of future star-forming sites, modifying the initial conditions for collapse and effecting the evolutionary criteria of protostars developed from spectral energy distributions. Possible scenarios for the origin of the morphology seen in this region are discussed, including a western equivalent to the eastern filament, which was destroyed by the creation of the OB cluster and its subsequent winds and radiation.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/30/the-m16-molecular-complex-under-the-influence-of-ngc6611-herschels-perspective-of-the-heating-effect-on-the-eagle-nebula/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Lives of High Redshift</title>
		<link>http://voxcharta.org/2012/04/30/the-lives-of-high-redshift/</link>
		<comments>http://voxcharta.org/2012/04/30/the-lives-of-high-redshift/#comments</comments>
		<pubDate>Tue, 01 May 2012 01:02:40 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[body simulation]]></category>
		<category><![CDATA[coalescence]]></category>
		<category><![CDATA[comparative study]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[definitions]]></category>
		<category><![CDATA[duration]]></category>
		<category><![CDATA[formulae]]></category>
		<category><![CDATA[friction]]></category>
		<category><![CDATA[hybrid model]]></category>
		<category><![CDATA[mass range]]></category>
		<category><![CDATA[merger]]></category>
		<category><![CDATA[merger time]]></category>
		<category><![CDATA[practical application]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[robust approximation]]></category>
		<category><![CDATA[tidal disruption]]></category>
		<category><![CDATA[timescale]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/30/the-lives-of-high-redshift/</guid>
		<description><![CDATA[We present a comparative study of recent works on merger-timescales with dynamical friction and find a strong contrast between idealized/isolated mergers (Boylan-Kolchin et al. 2008) and mergers from a cosmological volume (Jiang et al. 2008). Our study measures the duration of mergers in a cosmological N-body simulation of dark matter, with emphasis on higher redshifts [...]]]></description>
			<content:encoded><![CDATA[<p>We present a comparative study of recent works on merger-timescales with dynamical friction and find a strong contrast between idealized/isolated mergers (Boylan-Kolchin et al. 2008) and mergers from a cosmological volume (Jiang et al. 2008). Our study measures the duration of mergers in a cosmological N-body simulation of dark matter, with emphasis on higher redshifts (z &lt; 10) and a lower mass range. In our analysis we consider and compare two merger definitions; tidal disruption and coalescence. We find that the merger-time formula proposed by Jiang et al. (2008) describes our results well and conclude that cosmologically motivated merger-time formulae provide a more versatile and statistically robust approximation for practical applications such as semi-analytic/hybrid models.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/30/the-lives-of-high-redshift/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Chemical segregation toward massive hot cores: The AFGL2591 star forming region</title>
		<link>http://voxcharta.org/2012/04/30/chemical-segregation-toward-massive-hot-cores-the-afgl2591-star-forming-region/</link>
		<comments>http://voxcharta.org/2012/04/30/chemical-segregation-toward-massive-hot-cores-the-afgl2591-star-forming-region/#comments</comments>
		<pubDate>Tue, 01 May 2012 00:57:56 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[chemical segregation]]></category>
		<category><![CDATA[concentric shells]]></category>
		<category><![CDATA[core]]></category>
		<category><![CDATA[high angular resolution]]></category>
		<category><![CDATA[high mass]]></category>
		<category><![CDATA[images]]></category>
		<category><![CDATA[linear scale]]></category>
		<category><![CDATA[mass star]]></category>
		<category><![CDATA[molecular species]]></category>
		<category><![CDATA[resolution observations]]></category>
		<category><![CDATA[sma]]></category>
		<category><![CDATA[species type]]></category>
		<category><![CDATA[submillimeter array]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/30/chemical-segregation-toward-massive-hot-cores-the-afgl2591-star-forming-region/</guid>
		<description><![CDATA[We present high angular resolution observations (0.5&#8243;x0.3&#8243;) carried out with the Submillimeter Array (SMA) toward the AFGL2591 high-mass star forming region. Our SMA images reveal a clear chemical segregation within the AFGL2591 VLA 3 hot core, where different molecular species (Type I, II and III) appear distributed in three concentric shells. This is the first [...]]]></description>
			<content:encoded><![CDATA[<p>We present high angular resolution observations (0.5&#8243;x0.3&#8243;) carried out with the Submillimeter Array (SMA) toward the AFGL2591 high-mass star forming region. Our SMA images reveal a clear chemical segregation within the AFGL2591 VLA 3 hot core, where different molecular species (Type I, II and III) appear distributed in three concentric shells. This is the first time that such a chemical segregation is ever reported at linear scales &lt;3000 AU within a hot core. While Type I species (H2S and 13CS) peak at the AFGL2591 VLA 3 protostar, Type II molecules (HC3N, OCS, SO and SO2) show a double-peaked structure circumventing the continuum peak. Type III species, represented by CH3OH, form a ring-like structure surrounding the continuum emission. The excitation temperatures of SO2, HC3N and CH3OH (185+-11 K, 150+-20 K and 124+-12 K, respectively) show a temperature gradient within the AFGL2591 VLA 3 envelope, consistent with previous observations and modeling of the source. By combining the H2S, SO2 and CH3OH images, representative of the three concentric shells, we find that the global kinematics of the molecular gas follow Keplerian-like rotation around a 40 Mo-star. The chemical segregation observed toward AFGL2591 VLA 3 is explained by the combination of molecular UV photo-dissociation and a high-temperature (~1000 K) gas-phase chemistry within the low extinction innermost region in the AFGL2591 VLA 3 hot core.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/30/chemical-segregation-toward-massive-hot-cores-the-afgl2591-star-forming-region/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>N-body simulation of clumpy torus: application to AGN</title>
		<link>http://voxcharta.org/2012/04/30/n-body-simulation-of-clumpy-torus-application-to-agn/</link>
		<comments>http://voxcharta.org/2012/04/30/n-body-simulation-of-clumpy-torus-application-to-agn/#comments</comments>
		<pubDate>Tue, 01 May 2012 00:51:59 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[body simulation]]></category>
		<category><![CDATA[central mass]]></category>
		<category><![CDATA[cross section]]></category>
		<category><![CDATA[density distribution]]></category>
		<category><![CDATA[dependence]]></category>
		<category><![CDATA[eccentricity]]></category>
		<category><![CDATA[efficiency]]></category>
		<category><![CDATA[equilibrium]]></category>
		<category><![CDATA[gaussian density]]></category>
		<category><![CDATA[gravitational field]]></category>
		<category><![CDATA[gravity]]></category>
		<category><![CDATA[inclination]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[oval shape]]></category>
		<category><![CDATA[test particle]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/30/n-body-simulation-of-clumpy-torus-application-to-agn/</guid>
		<description><![CDATA[The gravitational properties of torus have been investigated. It is shown that the torus can be formed from the test particles orbiting in the gravitational field of the central mass. In this case the toroidal distribution is achieved due to significant spread of inclinations and eccentricities of their orbits. To investigate a self-gravity of the [...]]]></description>
			<content:encoded><![CDATA[<p>The gravitational properties of torus have been investigated. It is shown that the torus can be formed from the test particles orbiting in the gravitational field of the central mass. In this case the toroidal distribution is achieved due to significant spread of inclinations and eccentricities of their orbits. To investigate a self-gravity of the torus we considered the N-body problem for the torus located in the gravitational field of the central mass. It is shown that in the equilibrium state the cross-section of the torus has an oval shape with Gaussian density distribution. The dependence of obscuring efficiency as a function of torus inclination is found.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/30/n-body-simulation-of-clumpy-torus-application-to-agn/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Luminous Infrared Galaxies With the Submillimeter Array. III. The Dense Kiloparsec Molecular Concentrations of Arp 299</title>
		<link>http://voxcharta.org/2012/04/30/luminous-infrared-galaxies-with-the-submillimeter-array-iii-the-dense-kiloparsec-molecular-concentrations-of-arp-299/</link>
		<comments>http://voxcharta.org/2012/04/30/luminous-infrared-galaxies-with-the-submillimeter-array-iii-the-dense-kiloparsec-molecular-concentrations-of-arp-299/#comments</comments>
		<pubDate>Tue, 01 May 2012 00:46:51 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[alpha co]]></category>
		<category><![CDATA[arp]]></category>
		<category><![CDATA[cm 3]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[dense gas]]></category>
		<category><![CDATA[density column]]></category>
		<category><![CDATA[different regions]]></category>
		<category><![CDATA[galaxy nuclei]]></category>
		<category><![CDATA[gas components]]></category>
		<category><![CDATA[james clerk maxwell]]></category>
		<category><![CDATA[kiloparsec]]></category>
		<category><![CDATA[luminous infrared galaxies]]></category>
		<category><![CDATA[mpc]]></category>
		<category><![CDATA[myr]]></category>
		<category><![CDATA[orders of magnitude]]></category>
		<category><![CDATA[radiative transfer code]]></category>
		<category><![CDATA[rapid depletion]]></category>
		<category><![CDATA[spiral galaxy]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[submillimeter array]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/30/luminous-infrared-galaxies-with-the-submillimeter-array-iii-the-dense-kiloparsec-molecular-concentrations-of-arp-299/</guid>
		<description><![CDATA[We have used high resolution (~2.3&#8243;) observations of the local (D = 46 Mpc) luminous infrared galaxy Arp 299 to map out the physical properties of the molecular gas which provides the fuel for its extreme star formation activity. The 12CO J=3-2, 12CO J=2-1 and 13CO J=2-1 lines were observed with the Submillimeter Array and [...]]]></description>
			<content:encoded><![CDATA[<p>We have used high resolution (~2.3&#8243;) observations of the local (D = 46 Mpc) luminous infrared galaxy Arp 299 to map out the physical properties of the molecular gas which provides the fuel for its extreme star formation activity. The 12CO J=3-2, 12CO J=2-1 and 13CO J=2-1 lines were observed with the Submillimeter Array and the short spacings of the 12CO J=2-1 and J=3-2 observations have been recovered using James Clerk Maxwell Telescope single dish observations. We use the radiative transfer code RADEX to estimate the physical properties (density, column density and temperature) of the different regions in this system. The RADEX solutions of the two galaxy nuclei, IC 694 and NGC 3690, are consistent with a wide range of gas components, from warm moderately dense gas with T_{kin} &gt; 30 K and n(H_{2}) ~ 0.3 &#8211; 3 x 10^{3} cm^{-3} to cold dense gas with T_{kin} ~ 10-30 K and n(H_{2}) &gt; 3 x 10^{3} cm^{-3}. The overlap region is shown to have a better constrained solution with T_{\rm{kin}}$ ~ 10-50 K and n(H_{2}) ~ 1-30 x 10^{3} cm^{-3}. We estimate the gas masses and star formation rates of each region in order to derive molecular gas depletion times. The depletion times of all regions (20-60 Myr) are found to be about 2 orders of magnitude lower than those of normal spiral galaxies. This rapid depletion time can probably be explained by a high fraction of dense gas on kiloparsec scales in Arp 299. We estimate the CO-to-H_{2} factor, \alpha_{co} to be 0.4 \pm 0.3 (3 x 10^{-4}/ x_{CO}) M_{sol} (K km s^{-1} pc^{2})^{-1} for the overlap region. This value agrees well with values determined previously for more advanced merger systems.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/30/luminous-infrared-galaxies-with-the-submillimeter-array-iii-the-dense-kiloparsec-molecular-concentrations-of-arp-299/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Adaptable Radiative Transfer Innovations for Submillimetre Telescopes (ARTIST) &#8211; Dust polarisation module (DustPol)</title>
		<link>http://voxcharta.org/2012/04/30/adaptable-radiative-transfer-innovations-for-submillimetre-telescopes-artist-dust-polarisation-module-dustpol/</link>
		<comments>http://voxcharta.org/2012/04/30/adaptable-radiative-transfer-innovations-for-submillimetre-telescopes-artist-dust-polarisation-module-dustpol/#comments</comments>
		<pubDate>Tue, 01 May 2012 00:45:42 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[ALMA]]></category>
		<category><![CDATA[atacama large millimeter]]></category>
		<category><![CDATA[atacama large millimeter array]]></category>
		<category><![CDATA[based user interface]]></category>
		<category><![CDATA[cm 3]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[dust emission]]></category>
		<category><![CDATA[innovation]]></category>
		<category><![CDATA[ira]]></category>
		<category><![CDATA[line emission]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[map]]></category>
		<category><![CDATA[maximum degree]]></category>
		<category><![CDATA[model library]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[planck]]></category>
		<category><![CDATA[python]]></category>
		<category><![CDATA[radiative transfer]]></category>
		<category><![CDATA[reduction software]]></category>
		<category><![CDATA[telescopes]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/30/adaptable-radiative-transfer-innovations-for-submillimetre-telescopes-artist-dust-polarisation-module-dustpol/</guid>
		<description><![CDATA[We present a new publicly available tool (DustPol) aimed to model the polarised thermal dust emission. The module DustPol, which is publicly available, is part of the ARTIST (Adaptable Radiative Transfer Innovations for Submillimetre Telescopes) package, which also offers tools for modelling the polarisation of line emission together with a model library and a Python-based [...]]]></description>
			<content:encoded><![CDATA[<p>We present a new publicly available tool (DustPol) aimed to model the polarised thermal dust emission. The module DustPol, which is publicly available, is part of the ARTIST (Adaptable Radiative Transfer Innovations for Submillimetre Telescopes) package, which also offers tools for modelling the polarisation of line emission together with a model library and a Python-based user interface. DustPol can easily manage analytical as well as pre-gridded models to generate synthetic maps of the Stokes I, Q, and U parameters. These maps are stored in FITS format which is straightforwardly read by the data reduction software used, e.g., by the Atacama Large Millimeter Array (ALMA). This turns DustPol into a powerful engine for the prediction of the expected polarisation features of a source observed with ALMA or the Planck satellite as well as for the interpretation of existing submillimetre observations obtained with other telescopes. DustPol allows the parameterisation of the maximum degree of polarisation and we find that, in a prestellar core, if there is depolarisation, this effect should happen at densities of 10^6 cm-3 or larger. We compare a model generated by DustPol with the observational polarisation data of the low-mass Class 0 object NGC 1333 IRAS 4A, finding that the total and the polarised emission are consistent.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/30/adaptable-radiative-transfer-innovations-for-submillimetre-telescopes-artist-dust-polarisation-module-dustpol/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Order and chaos in a galactic model with a strong nuclear bar</title>
		<link>http://voxcharta.org/2012/04/30/order-and-chaos-in-a-galactic-model-with-a-strong-nuclear-bar/</link>
		<comments>http://voxcharta.org/2012/04/30/order-and-chaos-in-a-galactic-model-with-a-strong-nuclear-bar/#comments</comments>
		<pubDate>Tue, 01 May 2012 00:43:45 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[chao]]></category>
		<category><![CDATA[chaotic motion]]></category>
		<category><![CDATA[contrary]]></category>
		<category><![CDATA[dynamical system]]></category>
		<category><![CDATA[equilibrium]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[global energy]]></category>
		<category><![CDATA[global model]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[harmonic oscillator]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[local energy]]></category>
		<category><![CDATA[local motion]]></category>
		<category><![CDATA[low energy]]></category>
		<category><![CDATA[massive nuclei]]></category>
		<category><![CDATA[nucleus]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[previous research]]></category>
		<category><![CDATA[resonance phenomena]]></category>
		<category><![CDATA[vicinity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/30/order-and-chaos-in-a-galactic-model-with-a-strong-nuclear-bar/</guid>
		<description><![CDATA[We use a composite gravitational galactic model consisting of a disk, a halo, a massive nucleus and a strong nuclear bar, in order to study the connections between global and local parameters in a realistic dynamical system. The local model is constructed from a two-dimensional perturbed harmonic oscillator and can be derived by expanding the [...]]]></description>
			<content:encoded><![CDATA[<p>We use a composite gravitational galactic model consisting of a disk, a halo, a massive nucleus and a strong nuclear bar, in order to study the connections between global and local parameters in a realistic dynamical system. The local model is constructed from a two-dimensional perturbed harmonic oscillator and can be derived by expanding the global model in the vicinity of the central stable Lagrange equilibrium point. The frequencies of oscillations are not arbitrary, but they are connected with all the parameters involved with the global model. Moreover, the value of the local energy is also connected with the value of the global energy. Low and high energy stars in the global model display chaotic motion. Comparison with previous research reveals that the presence of the massive nucleus is responsible for the chaotic motion of the low energy stars. In the local motion, the low energy stars show interesting resonance phenomena, but the chaotic motion, if any, is negligible. On the contrary, the high energy stars do not show bounded motion in the local model. This is an indication of particular activity near the center of galaxies possessing massive nuclei.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/30/order-and-chaos-in-a-galactic-model-with-a-strong-nuclear-bar/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Precise Relic WIMP Abundance and its Impact on Searches for Dark Matter Annihilation [Replacement]</title>
		<link>http://voxcharta.org/2012/04/30/precise-relic-wimp-abundance-and-its-impact-on-searches-for-dark-matter-annihilation-replacement/</link>
		<comments>http://voxcharta.org/2012/04/30/precise-relic-wimp-abundance-and-its-impact-on-searches-for-dark-matter-annihilation-replacement/#comments</comments>
		<pubDate>Tue, 01 May 2012 00:32:43 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abundance]]></category>
		<category><![CDATA[annihilation]]></category>
		<category><![CDATA[canonical]]></category>
		<category><![CDATA[cross section]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[early universe]]></category>
		<category><![CDATA[Fermi]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[mass density]]></category>
		<category><![CDATA[mass dependence]]></category>
		<category><![CDATA[mass region]]></category>
		<category><![CDATA[massive particle]]></category>
		<category><![CDATA[noticeable impact]]></category>
		<category><![CDATA[present day]]></category>
		<category><![CDATA[relic]]></category>
		<category><![CDATA[uncertainty]]></category>
		<category><![CDATA[wimp]]></category>
		<category><![CDATA[wmap]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/30/precise-relic-wimp-abundance-and-its-impact-on-searches-for-dark-matter-annihilation-replacement/</guid>
		<description><![CDATA[If dark matter (DM) is a weakly interacting massive particle (WIMP) that is a thermal relic of the early Universe, then its total self-annihilation cross section is revealed by its present-day mass density. The canonical thermally averaged cross section for a generic WIMP is usually stated as 3*10^-26 cm^3s^-1, with unspecified uncertainty, and taken to [...]]]></description>
			<content:encoded><![CDATA[<p>If dark matter (DM) is a weakly interacting massive particle (WIMP) that is a thermal relic of the early Universe, then its total self-annihilation cross section is revealed by its present-day mass density. The canonical thermally averaged cross section for a generic WIMP is usually stated as 3*10^-26 cm^3s^-1, with unspecified uncertainty, and taken to be independent of WIMP mass. Recent searches for annihilation products of DM annihilation have just reached the sensitivity to exclude this canonical cross section for 100% branching ratio to certain final states and small WIMP masses. The ultimate goal is to probe all kinematically allowed final states as a function of mass and, if all states are adequately excluded, set a lower limit to the WIMP mass. Probing the low-mass region is further motivated due to recent hints for a light WIMP in direct and indirect searches. We revisit the thermal relic abundance calculation for a generic WIMP and show that the required cross section can be calculated precisely. It varies significantly with mass at masses below 10 GeV, reaching a maximum of 5.2*10^-26 cm^3s^-1 at masses around 0.3 GeV, and is 2.2*10^-26 cm^3s^-1 with feeble mass-dependence for masses above 10 GeV. These results, which differ significantly from the canonical value and have not been taken into account in searches for annihilation products from generic WIMPs, have a noticeable impact on the interpretation of present limits from Fermi-LAT and WMAP+ACT.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/30/precise-relic-wimp-abundance-and-its-impact-on-searches-for-dark-matter-annihilation-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Carbon-rich dust production in metal-poor galaxies in the Local Group [Replacement]</title>
		<link>http://voxcharta.org/2012/04/30/carbon-rich-dust-production-in-metal-poor-galaxies-in-the-local-group-replacement/</link>
		<comments>http://voxcharta.org/2012/04/30/carbon-rich-dust-production-in-metal-poor-galaxies-in-the-local-group-replacement/#comments</comments>
		<pubDate>Tue, 01 May 2012 00:32:23 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorption]]></category>
		<category><![CDATA[acetylene]]></category>
		<category><![CDATA[asymptotic giant branch]]></category>
		<category><![CDATA[carbon budget]]></category>
		<category><![CDATA[carbon star]]></category>
		<category><![CDATA[dredge]]></category>
		<category><![CDATA[dust emission]]></category>
		<category><![CDATA[dwarf spheroidals]]></category>
		<category><![CDATA[fornax]]></category>
		<category><![CDATA[infrared spectrograph]]></category>
		<category><![CDATA[local group]]></category>
		<category><![CDATA[magellanic cloud]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[pulsation]]></category>
		<category><![CDATA[sculptor]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectral property]]></category>
		<category><![CDATA[spheroidal galaxy]]></category>
		<category><![CDATA[spitzer space telescope]]></category>
		<category><![CDATA[stellar core]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/30/carbon-rich-dust-production-in-metal-poor-galaxies-in-the-local-group-replacement/</guid>
		<description><![CDATA[We have observed a sample of 19 carbon stars in the Sculptor, Carina, Fornax, and Leo I dwarf spheroidal galaxies with the Infrared Spectrograph on the Spitzer Space Telescope. The spectra show significant quantities of dust around the carbon stars in Sculptor, Fornax, and Leo I, but little in Carina. Previous comparisons of carbon stars [...]]]></description>
			<content:encoded><![CDATA[<p>We have observed a sample of 19 carbon stars in the Sculptor, Carina, Fornax, and Leo I dwarf spheroidal galaxies with the Infrared Spectrograph on the Spitzer Space Telescope. The spectra show significant quantities of dust around the carbon stars in Sculptor, Fornax, and Leo I, but little in Carina. Previous comparisons of carbon stars with similar pulsation properties in the Galaxy and the Magellanic Clouds revealed no evidence that metallicity affected the production of dust by carbon stars. However, the more metal-poor stars in the current sample appear to be generating less dust. These data extend two known trends to lower metallicities. In more metal-poor samples, the SiC dust emission weakens, while the acetylene absorption strengthens. The bolometric magnitudes and infrared spectral properties of the carbon stars in Fornax are consistent with metallicities more similar to carbon stars in the Magellanic Clouds than in the other dwarf spheroidals in our sample. A study of the carbon budget in these stars reinforces previous considerations that the dredge-up of sufficient quantities of carbon from the stellar cores may trigger the final superwind phase, ending a star&#8217;s lifetime on the asymptotic giant branch.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/30/carbon-rich-dust-production-in-metal-poor-galaxies-in-the-local-group-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The same, but different: Stochasticity in binary destruction</title>
		<link>http://voxcharta.org/2012/04/29/the-same-but-different-stochasticity-in-binary-destruction/</link>
		<comments>http://voxcharta.org/2012/04/29/the-same-but-different-stochasticity-in-binary-destruction/#comments</comments>
		<pubDate>Mon, 30 Apr 2012 01:04:06 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[10s]]></category>
		<category><![CDATA[body simulation]]></category>
		<category><![CDATA[cluster]]></category>
		<category><![CDATA[conclusive evidence]]></category>
		<category><![CDATA[distribution ranges]]></category>
		<category><![CDATA[distributions]]></category>
		<category><![CDATA[exact details]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[initial population]]></category>
		<category><![CDATA[intermediates]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[mass ratio]]></category>
		<category><![CDATA[myr]]></category>
		<category><![CDATA[nebula]]></category>
		<category><![CDATA[population]]></category>
		<category><![CDATA[separations]]></category>
		<category><![CDATA[stochasticity]]></category>
		<category><![CDATA[survival]]></category>
		<category><![CDATA[visual binary]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/29/the-same-but-different-stochasticity-in-binary-destruction/</guid>
		<description><![CDATA[Observations of binaries in clusters tend to be of visual binaries with separations of 10s &#8211; 100s au. Such binaries are &#8216;intermediates&#8217; and their destruction or survival depends on the exact details of their individual dynamical history. We investigate the stochasticity of the destruction of such binaries and the differences between the initial and processed [...]]]></description>
			<content:encoded><![CDATA[<p>Observations of binaries in clusters tend to be of visual binaries with separations of 10s &#8211; 100s au. Such binaries are &#8216;intermediates&#8217; and their destruction or survival depends on the exact details of their individual dynamical history. We investigate the stochasticity of the destruction of such binaries and the differences between the initial and processed populations using N-body simulations. We concentrate on Orion Nebula Cluster-like clusters, where the observed binary separation distribution ranges from 62 &#8211; 620 au.   We find that, starting from the same initial binary population in statistically identical clusters, the number of intermediate binaries that are destroyed after 1 Myr can vary by a factor of &gt;2, and that the resulting separation distributions can be statistically completely different in initially substructured clusters. We also find that the mass ratio distributions are altered (destroying more low mass ratio systems), but not as significantly as the binary fractions or separation distributions. We conclude that finding very different intermediate (visual) binary populations in different clusters does not provide conclusive evidence that the initial populations were different.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/29/the-same-but-different-stochasticity-in-binary-destruction/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Can filamentary accretion explain the orbital poles of the Milky Way satellites?</title>
		<link>http://voxcharta.org/2012/04/29/can-filamentary-accretion-explain-the-orbital-poles-of-the-milky-way-satellites/</link>
		<comments>http://voxcharta.org/2012/04/29/can-filamentary-accretion-explain-the-orbital-poles-of-the-milky-way-satellites/#comments</comments>
		<pubDate>Mon, 30 Apr 2012 01:03:49 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[alignment]]></category>
		<category><![CDATA[angular momentum]]></category>
		<category><![CDATA[aquarius project]]></category>
		<category><![CDATA[cosmological simulations]]></category>
		<category><![CDATA[galaxy interaction]]></category>
		<category><![CDATA[likelihood]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[numerical model]]></category>
		<category><![CDATA[phase space]]></category>
		<category><![CDATA[probability]]></category>
		<category><![CDATA[satellite]]></category>
		<category><![CDATA[satellite galaxy]]></category>
		<category><![CDATA[satellite orbit]]></category>
		<category><![CDATA[scenarios]]></category>
		<category><![CDATA[space distribution]]></category>
		<category><![CDATA[state of the art]]></category>
		<category><![CDATA[tidal debris]]></category>
		<category><![CDATA[tidal dwarf galaxies]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/29/can-filamentary-accretion-explain-the-orbital-poles-of-the-milky-way-satellites/</guid>
		<description><![CDATA[Several scenarios have been suggested to explain the phase-space distribution of the Milky Way (MW) satellite galaxies in a disc of satellites (DoS). To quantitatively compare these different possibilities, a new method analysing angular momentum directions in modelled data is presented. It determines how likely it is to find sets of angular momenta as concentrated [...]]]></description>
			<content:encoded><![CDATA[<p>Several scenarios have been suggested to explain the phase-space distribution of the Milky Way (MW) satellite galaxies in a disc of satellites (DoS). To quantitatively compare these different possibilities, a new method analysing angular momentum directions in modelled data is presented. It determines how likely it is to find sets of angular momenta as concentrated and as close to a polar orientation as is observed for the MW satellite orbital poles. The method can be easily applied to orbital pole data from different models. The observed distribution of satellite orbital poles is compared to published angular momentum directions of subhalos derived from six cosmological state-of-the-art simulations in the Aquarius project. This tests the possibility that filamentary accretion might be able to naturally explain the satellite orbits within the DoS. For the most likely alignment of main halo and MW disc spin, the probability to reproduce the MW satellite orbital pole properties turns out to be less than 0.5 per cent in Aquarius models. Even an isotropic distribution of angular momenta has a higher likelihood to produce the observed distribution. The two Via Lactea cosmological simulations give results similar to the Aquarius simulations. Comparing instead with numerical models of galaxy-interactions gives a probability of up to 90 per cent for some models to draw the observed distribution of orbital poles from the angular momenta of tidal debris. This indicates that the formation as tidal dwarf galaxies in a single encounter is a viable, if not the only, process to explain the phase-space distribution of the MW satellite galaxies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/29/can-filamentary-accretion-explain-the-orbital-poles-of-the-milky-way-satellites/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Estimating column density from ammonia (1,1) emission in star-forming regions</title>
		<link>http://voxcharta.org/2012/04/29/estimating-column-density-from-ammonia-11-emission-in-star-forming-regions/</link>
		<comments>http://voxcharta.org/2012/04/29/estimating-column-density-from-ammonia-11-emission-in-star-forming-regions/#comments</comments>
		<pubDate>Mon, 30 Apr 2012 01:03:35 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[approximate method]]></category>
		<category><![CDATA[approximation]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[core]]></category>
		<category><![CDATA[density maps]]></category>
		<category><![CDATA[density of ammonia]]></category>
		<category><![CDATA[estimates]]></category>
		<category><![CDATA[inversion]]></category>
		<category><![CDATA[mapping observations]]></category>
		<category><![CDATA[outskirt]]></category>
		<category><![CDATA[partition function]]></category>
		<category><![CDATA[regime]]></category>
		<category><![CDATA[signal to noise]]></category>
		<category><![CDATA[signal to noise ratio]]></category>
		<category><![CDATA[timescale]]></category>
		<category><![CDATA[transition]]></category>
		<category><![CDATA[uncertainty]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/29/estimating-column-density-from-ammonia-11-emission-in-star-forming-regions/</guid>
		<description><![CDATA[We present a new, approximate method of calculating the column density of ammonia in mapping observations of the 23 GHz inversion lines. The temperature regime typically found in star forming regions allows for the assumption of a slowly varying partition function for ammonia. It is therefore possible to determine the column density using only the [...]]]></description>
			<content:encoded><![CDATA[<p>We present a new, approximate method of calculating the column density of ammonia in mapping observations of the 23 GHz inversion lines. The temperature regime typically found in star forming regions allows for the assumption of a slowly varying partition function for ammonia. It is therefore possible to determine the column density using only the (J=1,K=1) inversion transition rather than the typical combination of the (1,1) and (2,2) transitions, with additional uncertainties comparable to or less than typical observational error.   The proposed method allows column density and mass estimates to be extended into areas of lower signal to noise ratio. We show examples of column density maps around a number of cores in the W3 and Perseus star-forming regions made using this approximation, along with a comparison to the corresponding results obtained using the full two-transition approach. We suggest that this method is a useful tool in studying the distribution of mass around YSOs, particularly in the outskirts of the protostellar envelope where the (2,2) ammonia line is often undetectable on the short timescales necessary for large area mapping.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/29/estimating-column-density-from-ammonia-11-emission-in-star-forming-regions/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Resolved Stellar Population in 50 Regions of M83 from HST/WFC3 Early Release Science Observations</title>
		<link>http://voxcharta.org/2012/04/29/the-resolved-stellar-population-in-50-regions-of-m83-from-hstwfc3-early-release-science-observations/</link>
		<comments>http://voxcharta.org/2012/04/29/the-resolved-stellar-population-in-50-regions-of-m83-from-hstwfc3-early-release-science-observations/#comments</comments>
		<pubDate>Mon, 30 Apr 2012 00:58:02 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[age distribution]]></category>
		<category><![CDATA[age estimate]]></category>
		<category><![CDATA[hubble space telescope]]></category>
		<category><![CDATA[independent method]]></category>
		<category><![CDATA[isochrone]]></category>
		<category><![CDATA[luminous star]]></category>
		<category><![CDATA[measurable difference]]></category>
		<category><![CDATA[morphological appearance]]></category>
		<category><![CDATA[nearby spiral galaxy]]></category>
		<category><![CDATA[older stars]]></category>
		<category><![CDATA[science observations]]></category>
		<category><![CDATA[spiral arm]]></category>
		<category><![CDATA[spiral galaxy m83]]></category>
		<category><![CDATA[star cluster]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[surface brightness fluctuations]]></category>
		<category><![CDATA[wide field camera]]></category>
		<category><![CDATA[young stars]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/29/the-resolved-stellar-population-in-50-regions-of-m83-from-hstwfc3-early-release-science-observations/</guid>
		<description><![CDATA[We present a multi-wavelength photometric study of ~15,000 resolved stars in the nearby spiral galaxy M83 (NGC5236, D=4.61Mpc) based on Hubble Space Telescope Wide Field Camera 3 observations using four filters: F336W, F438W, F555W, and F814W. We select 50 regions (an average size of 260 pc by 280 pc) in the spiral arm and inter-arm [...]]]></description>
			<content:encoded><![CDATA[<p>We present a multi-wavelength photometric study of ~15,000 resolved stars in the nearby spiral galaxy M83 (NGC5236, D=4.61Mpc) based on Hubble Space Telescope Wide Field Camera 3 observations using four filters: F336W, F438W, F555W, and F814W. We select 50 regions (an average size of 260 pc by 280 pc) in the spiral arm and inter-arm areas of M83, and determine the age distribution of the luminous stellar populations in each region. This is accomplished by correcting for extinction towards each individual star by comparing its colors with predictions from stellar isochrones. We compare the resulting luminosity weighted mean ages of the luminous stars in the 50 regions with those determined from several independent methods, including the number ratio of red-to-blue supergiants, morphological appearance of the regions, surface brightness fluctuations, and the ages of clusters in the regions. We find reasonably good agreement between these methods. We also find that young stars are much more likely to be found in concentrated aggregates along spiral arms, while older stars are more dispersed. These results are consistent with the scenario that star formation is associated with the spiral arms, and stars form primarily in star clusters and then disperse on short timescales to form the field population. The locations of Wolf-Rayet stars are found to correlate with the positions of many of the youngest regions, providing additional support for our ability to accurately estimate ages. We address the effects of spatial resolution on the measured colors, magnitudes, and age estimates. While individual stars can occasionally show measurable differences in the colors and magnitudes, the age estimates for entire regions are only slightly affected.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/29/the-resolved-stellar-population-in-50-regions-of-m83-from-hstwfc3-early-release-science-observations/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Search for ionized jets towards high-mass young stellar objects</title>
		<link>http://voxcharta.org/2012/04/29/search-for-ionized-jets-towards-high-mass-young-stellar-objects/</link>
		<comments>http://voxcharta.org/2012/04/29/search-for-ionized-jets-towards-high-mass-young-stellar-objects/#comments</comments>
		<pubDate>Mon, 30 Apr 2012 00:53:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[arcsec]]></category>
		<category><![CDATA[australia telescope]]></category>
		<category><![CDATA[catalog]]></category>
		<category><![CDATA[continuum observations]]></category>
		<category><![CDATA[frequency radio]]></category>
		<category><![CDATA[jets]]></category>
		<category><![CDATA[mass star]]></category>
		<category><![CDATA[phenomena]]></category>
		<category><![CDATA[positive radio]]></category>
		<category><![CDATA[protostar]]></category>
		<category><![CDATA[radio continuum]]></category>
		<category><![CDATA[radio emission]]></category>
		<category><![CDATA[radio source]]></category>
		<category><![CDATA[resolutions]]></category>
		<category><![CDATA[stellar object]]></category>
		<category><![CDATA[systematic search]]></category>
		<category><![CDATA[telescope compact array]]></category>
		<category><![CDATA[ultracompact hii regions]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/29/search-for-ionized-jets-towards-high-mass-young-stellar-objects/</guid>
		<description><![CDATA[We are carrying out multi-frequency radio continuum observations, using the Australia Telescope Compact Array, to systematically search for collimated ionized jets towards high-mass young stellar objects (HMYSOs). Here we report observations at 1.4, 2.4, 4.8 and 8.6 GHz, made with angular resolutions of about 7, 4, 2, and 1 arcsec, respectively, towards six objects of [...]]]></description>
			<content:encoded><![CDATA[<p>We are carrying out multi-frequency radio continuum observations, using the Australia Telescope Compact Array, to systematically search for collimated ionized jets towards high-mass young stellar objects (HMYSOs). Here we report observations at 1.4, 2.4, 4.8 and 8.6 GHz, made with angular resolutions of about 7, 4, 2, and 1 arcsec, respectively, towards six objects of a sample of 33 southern HMYSOs thought to be in very early stages of evolution. The objects in the sample were selected from radio and infrared catalogs by having positive radio spectral indices and being luminous (L_bol &gt; 20,000 L_sun), but underluminous in radio emission compared to that expected from its bolometric luminosity. This criteria makes the radio sources good candidates for being ionized jets. As part of this systematic search, two ionized jets have been discovered: one previously published and the other reported here. The rest of the observed candidates correspond to three hypercompact hii regions and two ultracompact hii regions. The two jets discovered are associated with two of the most luminous (70,000 and 100,000 Lsun) HMYSOs known to harbor this type of objects, showing that the phenomena of collimated ionized winds appears in the formation process of stars at least up to masses of ~ 20 M_sun and provides strong evidence for a disk-mediated accretion scenario for the formation of high-mass stars. From the incidence of jets in our sample, we estimate that the jet phase in high-mass protostars lasts for 40,000 yr.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/29/search-for-ionized-jets-towards-high-mass-young-stellar-objects/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>VLTI/AMBER observations of the Seyfert nucleus of NGC 3783</title>
		<link>http://voxcharta.org/2012/04/29/vltiamber-observations-of-the-seyfert-nucleus-of-ngc-3783/</link>
		<comments>http://voxcharta.org/2012/04/29/vltiamber-observations-of-the-seyfert-nucleus-of-ngc-3783/#comments</comments>
		<pubDate>Mon, 30 Apr 2012 00:51:07 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion disk]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[agns]]></category>
		<category><![CDATA[baseline interferometry]]></category>
		<category><![CDATA[density gradient]]></category>
		<category><![CDATA[fundamental role]]></category>
		<category><![CDATA[infrared interferometry]]></category>
		<category><![CDATA[infrared wavelength range]]></category>
		<category><![CDATA[interferometric observations]]></category>
		<category><![CDATA[k band]]></category>
		<category><![CDATA[milli]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[putative]]></category>
		<category><![CDATA[radius]]></category>
		<category><![CDATA[reverberation measurements]]></category>
		<category><![CDATA[seyfert nucleus]]></category>
		<category><![CDATA[unification]]></category>
		<category><![CDATA[unprecedented spatial resolution]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/29/vltiamber-observations-of-the-seyfert-nucleus-of-ngc-3783/</guid>
		<description><![CDATA[Context. The putative tori surrounding the accretion disks of active galactic nuclei (AGNs) play a fundamental role in the unification scheme of AGNs. Infrared long-baseline interferometry allows us to study the inner dust distribution in AGNs with unprecedented spatial resolution over a wide infrared wavelength range.   Aims. Near- and mid-infrared interferometry is used [...]]]></description>
			<content:encoded><![CDATA[<p>Context. The putative tori surrounding the accretion disks of active galactic nuclei (AGNs) play a fundamental role in the unification scheme of AGNs. Infrared long-baseline interferometry allows us to study the inner dust distribution in AGNs with unprecedented spatial resolution over a wide infrared wavelength range.   Aims. Near- and mid-infrared interferometry is used to investigate the milli-arcsecond-scale dust distribution in the type 1.5 Seyfert nucleus of NGC 3783.   Methods. We observed NGC 3783 with the VLTI/AMBER instrument in the K-band and compared our observations with models.   Results. From the K-band observations, we derive a ring-fit torus radius of 0.74 +/- 0.23 mas or 0.16 +/- 0.05 pc. We compare this size with infrared interferometric observations of other AGNs and UV/optical-infrared reverberation measurements. For the interpretation of our observations, we simultaneously model our near- and mid-infrared visibilities and the SED with a temperature/density-gradient model including an additional inner hot 1400 K ring component.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/29/vltiamber-observations-of-the-seyfert-nucleus-of-ngc-3783/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Molecular line contamination in the SCUBA-2 450 {\mu}m and 850 {\mu}m continuum data</title>
		<link>http://voxcharta.org/2012/04/29/molecular-line-contamination-in-the-scuba-2-450-mum-and-850-mum-continuum-data/</link>
		<comments>http://voxcharta.org/2012/04/29/molecular-line-contamination-in-the-scuba-2-450-mum-and-850-mum-continuum-data/#comments</comments>
		<pubDate>Mon, 30 Apr 2012 00:50:00 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[array]]></category>
		<category><![CDATA[contamination]]></category>
		<category><![CDATA[conversion factor]]></category>
		<category><![CDATA[dust continuum emission]]></category>
		<category><![CDATA[dust emission]]></category>
		<category><![CDATA[emission source]]></category>
		<category><![CDATA[intensity]]></category>
		<category><![CDATA[map]]></category>
		<category><![CDATA[molecular cloud]]></category>
		<category><![CDATA[nearby star]]></category>
		<category><![CDATA[orion]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/29/molecular-line-contamination-in-the-scuba-2-450-mum-and-850-mum-continuum-data/</guid>
		<description><![CDATA[Observations of the dust emission using millimetre/submillimetre bolometer arrays can be contaminated by molecular line flux, such as flux from 12CO. As the brightest molecular line in the submillimetre, it is important to quantify the contribution of CO flux to the dust continuum bands. Conversion factors were used to convert molecular line integrated intensities to [...]]]></description>
			<content:encoded><![CDATA[<p>Observations of the dust emission using millimetre/submillimetre bolometer arrays can be contaminated by molecular line flux, such as flux from 12CO. As the brightest molecular line in the submillimetre, it is important to quantify the contribution of CO flux to the dust continuum bands. Conversion factors were used to convert molecular line integrated intensities to flux detected by bolometer arrays in mJy per beam. These factors were calculated for 12CO line integrated intensities to the SCUBA-2 850 {\mu}m and 450 {\mu}m bands. The conversion factors were then applied to HARP 12CO 3-2 maps of NGC 1333 in the Perseus complex and NGC 2071 and NGC 2024 in the Orion B molecular cloud complex to quantify the respective 12CO flux contribution to the 850 {\mu}m dust continuum emission. Sources with high molecular line contamination were analysed in further detail for molecular outflows and heating by nearby stars to determine the cause of the 12CO contribution. The majority of sources had a 12CO 3-2 flux contribution under 20 per cent. However, in regions of molecular outflows, the 12CO can dominate the source dust continuum (up to 79 per cent contamination) with 12CO fluxes reaching \sim 68 mJy per beam.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/29/molecular-line-contamination-in-the-scuba-2-450-mum-and-850-mum-continuum-data/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Electron-ion Recombination of Fe XII forming Fe XI: Laboratory Measurements and Theoretical Calculations</title>
		<link>http://voxcharta.org/2012/04/29/electron-ion-recombination-of-fe-xii-forming-fe-xi-laboratory-measurements-and-theoretical-calculations/</link>
		<comments>http://voxcharta.org/2012/04/29/electron-ion-recombination-of-fe-xii-forming-fe-xi-laboratory-measurements-and-theoretical-calculations/#comments</comments>
		<pubDate>Mon, 30 Apr 2012 00:46:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[3d core]]></category>
		<category><![CDATA[collision energy]]></category>
		<category><![CDATA[decay rate]]></category>
		<category><![CDATA[dr data]]></category>
		<category><![CDATA[electron beam]]></category>
		<category><![CDATA[excitation]]></category>
		<category><![CDATA[fe xii]]></category>
		<category><![CDATA[heavy ion]]></category>
		<category><![CDATA[heidelberg germany]]></category>
		<category><![CDATA[ion beam]]></category>
		<category><![CDATA[ion storage]]></category>
		<category><![CDATA[laboratory measurement]]></category>
		<category><![CDATA[max planck]]></category>
		<category><![CDATA[max planck institute]]></category>
		<category><![CDATA[nuclear physics]]></category>
		<category><![CDATA[rate coefficient]]></category>
		<category><![CDATA[recombination rate]]></category>
		<category><![CDATA[resonance energy]]></category>
		<category><![CDATA[storage ring]]></category>
		<category><![CDATA[theoretical calculation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/29/electron-ion-recombination-of-fe-xii-forming-fe-xi-laboratory-measurements-and-theoretical-calculations/</guid>
		<description><![CDATA[We have measured electron-ion recombination for Fe XII forming Fe XI using a merged beams configuration at the heavy-ion storage ring TSR located at the Max Planck Institute for Nuclear Physics in Heidelberg, Germany. The measured merged beams recombination rate coefficient (MBRRC) for collision energies from 0 to 1500 eV is presented. This work uses [...]]]></description>
			<content:encoded><![CDATA[<p>We have measured electron-ion recombination for Fe XII forming Fe XI using a merged beams configuration at the heavy-ion storage ring TSR located at the Max Planck Institute for Nuclear Physics in Heidelberg, Germany. The measured merged beams recombination rate coefficient (MBRRC) for collision energies from 0 to 1500 eV is presented. This work uses a new method for determining the absolute MBRRC based on a comparison of the ion beam decay rate with and without the electron beam on. For energies below 75 eV, the spectrum is dominated by dielectronic recombination (DR) resonances associated with 3s-3p and 3p-3d core excitations. At higher energies we observe contributions from 3-N&#8217; and 2-N&#8217; core excitations DR. We compare our experimental results to state-of-the-art multi-configuration Breit-Pauli (MCBP) calculations and find significant differences, both in resonance energies and strengths. We have extracted the DR contributions from the measured MBRRC data and transformed them into a plasma recombination rate coefficient (PRRC) for temperatures in the range of 10^3 to 10^7 K. We show that the previously recommended DR data for Fe XII significantly underestimate the PRRC at temperatures relevant for both photoionized plasmas (PPs) and collisionaly ionized plasmas (CPs). This is to be contrasted with our MCBP PRRC results which agree with the experiment to within 30% at PP temperatures and even better at CP temperatures. We find this agreement despite the disagreement shown by the detailed comparison between our MCBP and experimental MBRRC results. Lastly, we present a simple parameterized form of the experimentally derived PRRC for easy use in astrophysical modelling codes.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/29/electron-ion-recombination-of-fe-xii-forming-fe-xi-laboratory-measurements-and-theoretical-calculations/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>A Multiwavelength Study of Evolved Massive Stars in the Galactic Center</title>
		<link>http://voxcharta.org/2012/04/29/a-multiwavelength-study-of-evolved-massive-stars-in-the-galactic-center/</link>
		<comments>http://voxcharta.org/2012/04/29/a-multiwavelength-study-of-evolved-massive-stars-in-the-galactic-center/#comments</comments>
		<pubDate>Mon, 30 Apr 2012 00:39:42 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[2mass]]></category>
		<category><![CDATA[cataclysmic variables]]></category>
		<category><![CDATA[chandra x ray]]></category>
		<category><![CDATA[continuum emission]]></category>
		<category><![CDATA[distinct region]]></category>
		<category><![CDATA[dust emission]]></category>
		<category><![CDATA[early universe]]></category>
		<category><![CDATA[equivalent width]]></category>
		<category><![CDATA[extinction]]></category>
		<category><![CDATA[galactic center]]></category>
		<category><![CDATA[hii region]]></category>
		<category><![CDATA[irac]]></category>
		<category><![CDATA[magnitude plot]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[massive stellar clusters]]></category>
		<category><![CDATA[order of magnitude]]></category>
		<category><![CDATA[population study]]></category>
		<category><![CDATA[quintuplet cluster]]></category>
		<category><![CDATA[ray observations]]></category>
		<category><![CDATA[width measurements]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/29/a-multiwavelength-study-of-evolved-massive-stars-in-the-galactic-center/</guid>
		<description><![CDATA[The central region of the Milky Way provides a unique laboratory for a systematic, spatially-resolved population study of evolved massive stars of various types in a relatively high metallicity environment. We have conducted a multi-wavelength data analysis of 180 such stars or candidates, most of which were drawn from a recent large-scale HST/NICMOS narrow-band Pa-a [...]]]></description>
			<content:encoded><![CDATA[<p>The central region of the Milky Way provides a unique laboratory for a systematic, spatially-resolved population study of evolved massive stars of various types in a relatively high metallicity environment. We have conducted a multi-wavelength data analysis of 180 such stars or candidates, most of which were drawn from a recent large-scale HST/NICMOS narrow-band Pa-a survey, plus additional 14 Wolf-Rayet stars identified in earlier ground-based spectroscopic observations of the same field. The multi-wavelength data include broad-band IR photometry measurements from HST/NICMOS, SIRIUS, 2MASS, Spitzer/IRAC, and Chandra X-ray observations. We correct for extinctions toward individual stars, improve the Pa-a line equivalent width measurements, quantify the substantial mid-IR dust emission associated with WC stars, and find X-ray counterparts. In the process, we identify 10 foreground sources, some of which may be nearby cataclysmic variables. The WN stars in the Arches and Central clusters show correlations between the Pa-a equivalent width and the adjacent continuum emission. However, the WN stars in the latter cluster are systematically dimmer than those in the Arches cluster, presumably due to the different ages of the two clusters. In the EW-magnitude plot, WNL stars, WC stars and OB supergiants roughly fall into three distinct regions. We estimate that the dust mass associated with individual WC stars in the Quintuplet cluster can reach 1e-5 M, or more than one order of magnitude larger than previous estimates. Thus WC stars could be a significant source of dust in the galaxies of the early universe. Nearly half of the evolved massive stars in the GC are located outside the three known massive stellar clusters. The ionization of several compact HII regions can be accounted for by their enclosed individual evolved massive stars, which thus likely formed in isolation or in small groups.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/29/a-multiwavelength-study-of-evolved-massive-stars-in-the-galactic-center/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Dynamo action in thermally unstable interstellar flows [Replacement]</title>
		<link>http://voxcharta.org/2012/04/29/dynamo-action-in-thermally-unstable-interstellar-flows-replacement/</link>
		<comments>http://voxcharta.org/2012/04/29/dynamo-action-in-thermally-unstable-interstellar-flows-replacement/#comments</comments>
		<pubDate>Mon, 30 Apr 2012 00:36:14 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[conclusion]]></category>
		<category><![CDATA[critical reynolds number]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[dynamo action]]></category>
		<category><![CDATA[flow field]]></category>
		<category><![CDATA[large scale]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[molecular cloud]]></category>
		<category><![CDATA[phase transition]]></category>
		<category><![CDATA[positive correlation]]></category>
		<category><![CDATA[rho]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[thermal instability]]></category>
		<category><![CDATA[Turbulence]]></category>
		<category><![CDATA[unstable regime]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/29/dynamo-action-in-thermally-unstable-interstellar-flows-replacement/</guid>
		<description><![CDATA[Numerous studies have investigated the role of thermal instability in regulating the phase transition between the cold cloudy and warm diffuse medium of the interstellar medium. Considerable interest has also been devoted in investigating the properties of turbulence in thermally unstable flows, special emphasis on molecular clouds and the possibility of star formation. In this [...]]]></description>
			<content:encoded><![CDATA[<p>Numerous studies have investigated the role of thermal instability in regulating the phase transition between the cold cloudy and warm diffuse medium of the interstellar medium. Considerable interest has also been devoted in investigating the properties of turbulence in thermally unstable flows, special emphasis on molecular clouds and the possibility of star formation. In this study, we investigate another setting in which this instability may be important, namely its effect on dynamo action in interstellar flows. The setup we consider is a three dimensional periodic cube of gas with an initially weak magnetic field, subject to heating and cooling, the properties of which are such that thermal instability is provoked at certain temperature regime. Dynamo action is established through external forcing on the flow field. By comparing the results with a cooling function with exactly the same net effect but no thermally unstable regime, we find the following. The critical Reynolds number for the onset of the large-scale dynamo was observed to roughly double between the thermally stable versus unstable runs, the conclusion being that the thermal instability makes large-scale dynamo action more difficult. Whereas density and magnetic fields were observed to be almost completely uncorrelated in the thermally stable cases investigated, the action of thermal instability was observed to produce a positive correlation of the form B propto rho^0.2. This correlation is rather weak, and in addition it was observed to break down at the limit of the highest densities.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/29/dynamo-action-in-thermally-unstable-interstellar-flows-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Gravitational microlensing as a test of a finite-width disk model of the Galaxy [Replacement]</title>
		<link>http://voxcharta.org/2012/04/29/gravitational-microlensing-as-a-test-of-a-finite-width-disk-model-of-the-galaxy-replacement/</link>
		<comments>http://voxcharta.org/2012/04/29/gravitational-microlensing-as-a-test-of-a-finite-width-disk-model-of-the-galaxy-replacement/#comments</comments>
		<pubDate>Mon, 30 Apr 2012 00:36:04 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[aim]]></category>
		<category><![CDATA[baryonic]]></category>
		<category><![CDATA[compact object]]></category>
		<category><![CDATA[disk model]]></category>
		<category><![CDATA[finite width]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gravitational microlensing]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[subtraction]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/29/gravitational-microlensing-as-a-test-of-a-finite-width-disk-model-of-the-galaxy-replacement/</guid>
		<description><![CDATA[The aim of this work is to show in the framework of a simple finite-width disk model that the amount of mass seen through gravitational microlensing measurements in the region $0&#60;R&#60;R\sun$ is consistent with the dynamical mass ascertained from Galaxy rotation after subtraction of gas contribution. Since microlensing detects only compact objects, this result suggests [...]]]></description>
			<content:encoded><![CDATA[<p>The aim of this work is to show in the framework of a simple finite-width disk model that the amount of mass seen through gravitational microlensing measurements in the region $0&lt;R&lt;R\sun$ is consistent with the dynamical mass ascertained from Galaxy rotation after subtraction of gas contribution. Since microlensing detects only compact objects, this result suggests that non-baryonic mass component may be negligible in this region.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/29/gravitational-microlensing-as-a-test-of-a-finite-width-disk-model-of-the-galaxy-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Interacting dark matter contribution to the Galactic 511 keV gamma ray emission: constraining the morphology with INTEGRAL/SPI observations [Replacement]</title>
		<link>http://voxcharta.org/2012/04/29/interacting-dark-matter-contribution-to-the-galactic-511-kev-gamma-ray-emission-constraining-the-morphology-with-integralspi-observations-replacement/</link>
		<comments>http://voxcharta.org/2012/04/29/interacting-dark-matter-contribution-to-the-galactic-511-kev-gamma-ray-emission-constraining-the-morphology-with-integralspi-observations-replacement/#comments</comments>
		<pubDate>Mon, 30 Apr 2012 00:33:45 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[beta decay]]></category>
		<category><![CDATA[body simulation]]></category>
		<category><![CDATA[dark matter halo]]></category>
		<category><![CDATA[degrees of freedom]]></category>
		<category><![CDATA[excited state]]></category>
		<category><![CDATA[explanations]]></category>
		<category><![CDATA[galactic bulge]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gamma ray emission]]></category>
		<category><![CDATA[keV]]></category>
		<category><![CDATA[low energy]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[morphology]]></category>
		<category><![CDATA[pair]]></category>
		<category><![CDATA[profile]]></category>
		<category><![CDATA[scenarios]]></category>
		<category><![CDATA[shape]]></category>
		<category><![CDATA[sky]]></category>
		<category><![CDATA[spatial distribution]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/29/interacting-dark-matter-contribution-to-the-galactic-511-kev-gamma-ray-emission-constraining-the-morphology-with-integralspi-observations-replacement/</guid>
		<description><![CDATA[We compare the full-sky morphology of the 511 keV gamma ray excess measured by the INTEGRAL/SPI experiment to predictions of models based on dark matter (DM) scatterings that produce low-energy positrons: either MeV-scale DM that annihilates directly into e+e- pairs, or heavy DM that inelastically scatters into an excited state (XDM) followed by decay into [...]]]></description>
			<content:encoded><![CDATA[<p>We compare the full-sky morphology of the 511 keV gamma ray excess measured by the INTEGRAL/SPI experiment to predictions of models based on dark matter (DM) scatterings that produce low-energy positrons: either MeV-scale DM that annihilates directly into e+e- pairs, or heavy DM that inelastically scatters into an excited state (XDM) followed by decay into e+e- and the ground state.By direct comparison to the data, we find that such explanations are consistent with dark matter halo profiles predicted by numerical many-body simulations for a Milky Way-like galaxy. Our results favor an Einasto profile over the cuspier NFW distribution and exclude decaying dark matter scenarios whose predicted spatial distribution is too broad. We obtain a good fit to the shape of the signal using six fewer degrees of freedom than previous empirical fits to the 511 keV data. We find that the ratio of flux at Earth from the galactic bulge to that of the disk is between 1.9 and 2.4, taking into account that 73% of the disk contribution may be attributed to the beta decay of radioactive 26Al.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/29/interacting-dark-matter-contribution-to-the-galactic-511-kev-gamma-ray-emission-constraining-the-morphology-with-integralspi-observations-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>IAU (Maser) Symposium 287 Summary [Replacement]</title>
		<link>http://voxcharta.org/2012/04/29/iau-maser-symposium-287-summary-replacement/</link>
		<comments>http://voxcharta.org/2012/04/29/iau-maser-symposium-287-summary-replacement/#comments</comments>
		<pubDate>Mon, 30 Apr 2012 00:31:18 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cosmic masers]]></category>
		<category><![CDATA[iau]]></category>
		<category><![CDATA[maser]]></category>
		<category><![CDATA[oral presentations]]></category>
		<category><![CDATA[posters]]></category>
		<category><![CDATA[science]]></category>
		<category><![CDATA[stellenbosch south africa]]></category>
		<category><![CDATA[symposium]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/29/iau-maser-symposium-287-summary-replacement/</guid>
		<description><![CDATA[I&#8217;m trying to summarize the science communicated via oral presentations and by posters at the IAU Symposium 287 &#8220;Cosmic Masers &#8211; from OH to H_0&#8243;, which took place from January 29 to February 3, 2012 in Stellenbosch, South Africa.
]]></description>
			<content:encoded><![CDATA[<p>I&#8217;m trying to summarize the science communicated via oral presentations and by posters at the IAU Symposium 287 &#8220;Cosmic Masers &#8211; from OH to H_0&#8243;, which took place from January 29 to February 3, 2012 in Stellenbosch, South Africa.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/29/iau-maser-symposium-287-summary-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Ionization structure and chemical abundances of the Wolf-Rayet nebula NGC6888 with integral field spectroscopy</title>
		<link>http://voxcharta.org/2012/04/26/ionization-structure-and-chemical-abundances-of-the-wolf-rayet-nebula-ngc6888-with-integral-field-spectroscopy/</link>
		<comments>http://voxcharta.org/2012/04/26/ionization-structure-and-chemical-abundances-of-the-wolf-rayet-nebula-ngc6888-with-integral-field-spectroscopy/#comments</comments>
		<pubDate>Fri, 27 Apr 2012 00:55:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[2d analysis]]></category>
		<category><![CDATA[chemical composition]]></category>
		<category><![CDATA[electron density]]></category>
		<category><![CDATA[extinction]]></category>
		<category><![CDATA[field spectroscopy]]></category>
		<category><![CDATA[footprint]]></category>
		<category><![CDATA[frequency distribution]]></category>
		<category><![CDATA[integral field]]></category>
		<category><![CDATA[ism]]></category>
		<category><![CDATA[map]]></category>
		<category><![CDATA[nebula]]></category>
		<category><![CDATA[optical range]]></category>
		<category><![CDATA[ppak]]></category>
		<category><![CDATA[radial velocity]]></category>
		<category><![CDATA[shock models]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[stellar wind]]></category>
		<category><![CDATA[wolf]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/26/ionization-structure-and-chemical-abundances-of-the-wolf-rayet-nebula-ngc6888-with-integral-field-spectroscopy/</guid>
		<description><![CDATA[This work aims to search for the observational footprints of the interactions between the interstellar medium (ISM) and stellar winds in the Wolf-Rayet (WR) nebula NGC6888 in order to understand its ionization structure, chemical composition, and kinematics. We have collected a set of integral field spectroscopy observations across NGC6888, obtained with PPAK in the optical [...]]]></description>
			<content:encoded><![CDATA[<p>This work aims to search for the observational footprints of the interactions between the interstellar medium (ISM) and stellar winds in the Wolf-Rayet (WR) nebula NGC6888 in order to understand its ionization structure, chemical composition, and kinematics. We have collected a set of integral field spectroscopy observations across NGC6888, obtained with PPAK in the optical range performing both 2D and 1D analyses. Attending to the 2D analysis in the northeast part of NGC6888, we have generated maps of the extinction structure and electron density. We produced statistical frequency distributions of the radial velocity and diagnostic diagrams. We have found that the spectra of a localized region to the southwest of this pointing can be represented well by shock models. Furthermore, we performed a thorough study of integrated spectra in nine regions over the whole nebula. We derived electron densities ranging from &lt;100 to 360 cm^(-3). The electron temperature varies from ~7700 K to ~10200 K. A strong variation of up to a factor 10 between different regions in the nitrogen abundance has been found: N/H appears lower than the solar abundance in those positions observed at the edges and very enhanced in the observed inner parts. Oxygen appears slightly underabundant with respect to solar value, whereas the helium abundance is found to be above it. Finally, we provide a scenario for the evolution of NGC6888 to explain the features observed. This scheme consists of a structure of multiple shells.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/26/ionization-structure-and-chemical-abundances-of-the-wolf-rayet-nebula-ngc6888-with-integral-field-spectroscopy/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Dramatic infrared variability of WISE J1810-3305: catching early dust ejection during the thermal pulse of an AGB star?</title>
		<link>http://voxcharta.org/2012/04/26/dramatic-infrared-variability-of-wise-j1810-3305-catching-early-dust-ejection-during-the-thermal-pulse-of-an-agb-star/</link>
		<comments>http://voxcharta.org/2012/04/26/dramatic-infrared-variability-of-wise-j1810-3305-catching-early-dust-ejection-during-the-thermal-pulse-of-an-agb-star/#comments</comments>
		<pubDate>Fri, 27 Apr 2012 00:55:26 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[asymptotic giant branch]]></category>
		<category><![CDATA[colors]]></category>
		<category><![CDATA[confirmation]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[envelopes]]></category>
		<category><![CDATA[infrared measurements]]></category>
		<category><![CDATA[ira]]></category>
		<category><![CDATA[optical counterpart]]></category>
		<category><![CDATA[photographic plate]]></category>
		<category><![CDATA[photometric characteristics]]></category>
		<category><![CDATA[point source]]></category>
		<category><![CDATA[rarity]]></category>
		<category><![CDATA[source catalog]]></category>
		<category><![CDATA[spectral class]]></category>
		<category><![CDATA[spectral energy distribution]]></category>
		<category><![CDATA[stellar evolution]]></category>
		<category><![CDATA[thermal pulse]]></category>
		<category><![CDATA[variability]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/26/dramatic-infrared-variability-of-wise-j1810-3305-catching-early-dust-ejection-during-the-thermal-pulse-of-an-agb-star/</guid>
		<description><![CDATA[We present the discovery of a source with broadband infrared photometric characteristics similar to Sakurai&#8217;s Object. WISE J180956.27-330500.2 (hereafter, J1810-3305) shows very red WISE colors, but a very blue 2MASS [K] vs. WISE [W1 (3.4 micron)] color. It was not visible during the IRAS era, but now has a 12 micron flux well above the [...]]]></description>
			<content:encoded><![CDATA[<p>We present the discovery of a source with broadband infrared photometric characteristics similar to Sakurai&#8217;s Object. WISE J180956.27-330500.2 (hereafter, J1810-3305) shows very red WISE colors, but a very blue 2MASS [K] vs. WISE [W1 (3.4 micron)] color. It was not visible during the IRAS era, but now has a 12 micron flux well above the IRAS point source catalog detection limit. There are also indications of variability in historical optical photographic plates, as well as in multi-epoch AKARI mid-infrared measurements. The broadband infrared spectral energy distribution, post-IRAS brightening and multiwavelength variability are all characteristics also shared by Sakurai&#8217;s Object &#8211; a post asymptotic giant branch (post-AGB) star which underwent a late thermal pulse and recently ejected massive envelopes of dust that are currently expanding and cooling. Optical progenitor colors suggest that J1810-3305 may have been of late spectral class. Its dramatic infrared brightening, and the detection of a late-type optical counterpart are consistent with a scenario in which we have caught an extremely massive dust ejection event (in 1998 or shortly before) during the thermal pulse of an AGB star, thus providing a unique opportunity to observe stellar evolution in this phase. J1810-3305 is the only source in the entire WISE preliminary data release with similar infrared SED and variability, emphasizing the rarity of such sources. Confirmation of its nature is of great importance.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/26/dramatic-infrared-variability-of-wise-j1810-3305-catching-early-dust-ejection-during-the-thermal-pulse-of-an-agb-star/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Diagnostics of Baryonic Cooling in Lensing Galaxies</title>
		<link>http://voxcharta.org/2012/04/26/diagnostics-of-baryonic-cooling-in-lensing-galaxies/</link>
		<comments>http://voxcharta.org/2012/04/26/diagnostics-of-baryonic-cooling-in-lensing-galaxies/#comments</comments>
		<pubDate>Fri, 27 Apr 2012 00:54:40 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[collapse]]></category>
		<category><![CDATA[concentration]]></category>
		<category><![CDATA[contraction]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[inverse proportionality]]></category>
		<category><![CDATA[mass loss]]></category>
		<category><![CDATA[mechanisms]]></category>
		<category><![CDATA[msun]]></category>
		<category><![CDATA[prescriptions]]></category>
		<category><![CDATA[radii]]></category>
		<category><![CDATA[ray analysis]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[scales]]></category>
		<category><![CDATA[structure formation]]></category>
		<category><![CDATA[theoretical study]]></category>
		<category><![CDATA[virial]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/26/diagnostics-of-baryonic-cooling-in-lensing-galaxies/</guid>
		<description><![CDATA[Theoretical studies of structure formation find an inverse proportionality between the concentration of dark matter haloes and virial mass. This trend has been recently confirmed for virial masses Mvir &#62; ~6e12 Msun by the observation of the X-ray emission from the hot halo gas. We present an alternative approach to this problem, exploring the concentration [...]]]></description>
			<content:encoded><![CDATA[<p>Theoretical studies of structure formation find an inverse proportionality between the concentration of dark matter haloes and virial mass. This trend has been recently confirmed for virial masses Mvir &gt; ~6e12 Msun by the observation of the X-ray emission from the hot halo gas. We present an alternative approach to this problem, exploring the concentration of dark matter haloes over galaxy scales on a sample of 18 early-type systems. Our c-Mvir relation is consistent with the X-ray analysis, extending towards lower virial masses, covering the range from ~4e11 Msun up to 5e12 Msun. A combination of the lensing analysis along with photometric data allows us to constrain the baryon fraction within a few effective radii, which is compared with prescriptions for adiabatic contraction (AC) of the dark matter haloes. We find that the standard methods for AC are strongly disfavored, requiring additional mechanisms &#8212; such as mass loss during the contraction process &#8212; to play a role during the phases following the collapse of the haloes.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/26/diagnostics-of-baryonic-cooling-in-lensing-galaxies/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Discovery of an Ultra-Faint Star Cluster in the Constellation of Ursa Minor</title>
		<link>http://voxcharta.org/2012/04/26/the-discovery-of-an-ultra-faint-star-cluster-in-the-constellation-of-ursa-minor/</link>
		<comments>http://voxcharta.org/2012/04/26/the-discovery-of-an-ultra-faint-star-cluster-in-the-constellation-of-ursa-minor/#comments</comments>
		<pubDate>Fri, 27 Apr 2012 00:54:15 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absolute magnitude]]></category>
		<category><![CDATA[angular separation]]></category>
		<category><![CDATA[canada france]]></category>
		<category><![CDATA[constellation]]></category>
		<category><![CDATA[deimos]]></category>
		<category><![CDATA[faint star]]></category>
		<category><![CDATA[globular cluster]]></category>
		<category><![CDATA[hawaii telescope]]></category>
		<category><![CDATA[heliocentric radial velocity]]></category>
		<category><![CDATA[imager]]></category>
		<category><![CDATA[keck]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[light radius]]></category>
		<category><![CDATA[maximum likelihood]]></category>
		<category><![CDATA[photometric properties]]></category>
		<category><![CDATA[segue 3]]></category>
		<category><![CDATA[star cluster]]></category>
		<category><![CDATA[stellar cluster]]></category>
		<category><![CDATA[stellar photometry]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/26/the-discovery-of-an-ultra-faint-star-cluster-in-the-constellation-of-ursa-minor/</guid>
		<description><![CDATA[We report the discovery of a new ultra-faint globular cluster in the constellation of Ursa Minor, based on stellar photometry from the MegaCam imager at the Canada-France-Hawaii Telescope (CFHT). We find that this cluster, Munoz 1, is located at a distance of 45 +/- 5 kpc and at a projected distance of only 45 arcmin [...]]]></description>
			<content:encoded><![CDATA[<p>We report the discovery of a new ultra-faint globular cluster in the constellation of Ursa Minor, based on stellar photometry from the MegaCam imager at the Canada-France-Hawaii Telescope (CFHT). We find that this cluster, Munoz 1, is located at a distance of 45 +/- 5 kpc and at a projected distance of only 45 arcmin from the center of the Ursa Minor dSph galaxy. Using a Maximum Likelihood technique we measure a half-light radius of 0.5 arcmin, or equivalently 7 pc and an ellipticity consistent with being zero. We estimate its absolute magnitude to be M_V=-0.4 +/- 0.9, which corresponds to L_V=120 (+160, -65) L_sun and we measure a heliocentric radial velocity of -137 +/- 4 km/s based on Keck/DEIMOS spectroscopy. This new satellite is separate from Ursa Minor by ~30 kpc and 110 km/s suggesting the cluster is not obviously associated with the dSph, despite the very close angular separation. Based on its photometric properties and structural parameters we conclude that Munoz 1 is a new ultra-faint stellar cluster. Along with Segue 3 this is one of the faintest stellar clusters known to date.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/26/the-discovery-of-an-ultra-faint-star-cluster-in-the-constellation-of-ursa-minor/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Carbon-rich dust production in metal-poor galaxies in the Local Group</title>
		<link>http://voxcharta.org/2012/04/26/carbon-rich-dust-production-in-metal-poor-galaxies-in-the-local-group/</link>
		<comments>http://voxcharta.org/2012/04/26/carbon-rich-dust-production-in-metal-poor-galaxies-in-the-local-group/#comments</comments>
		<pubDate>Fri, 27 Apr 2012 00:52:35 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorption]]></category>
		<category><![CDATA[acetylene]]></category>
		<category><![CDATA[asymptotic giant branch]]></category>
		<category><![CDATA[carbon budget]]></category>
		<category><![CDATA[carbon star]]></category>
		<category><![CDATA[dredge]]></category>
		<category><![CDATA[dust emission]]></category>
		<category><![CDATA[dwarf spheroidals]]></category>
		<category><![CDATA[fornax]]></category>
		<category><![CDATA[infrared spectrograph]]></category>
		<category><![CDATA[local group]]></category>
		<category><![CDATA[magellanic cloud]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[pulsation]]></category>
		<category><![CDATA[sculptor]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectral property]]></category>
		<category><![CDATA[spheroidal galaxy]]></category>
		<category><![CDATA[spitzer space telescope]]></category>
		<category><![CDATA[stellar core]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/26/carbon-rich-dust-production-in-metal-poor-galaxies-in-the-local-group/</guid>
		<description><![CDATA[We have observed a sample of 19 carbon stars in the Sculptor, Carina, Fornax, and Leo I dwarf spheroidal galaxies with the Infrared Spectrograph on the Spitzer Space Telescope. The spectra show significant quantities of dust around the carbon stars in Sculptor, Fornax, and Leo I, but little in Carina. Previous comparisons of carbon stars [...]]]></description>
			<content:encoded><![CDATA[<p>We have observed a sample of 19 carbon stars in the Sculptor, Carina, Fornax, and Leo I dwarf spheroidal galaxies with the Infrared Spectrograph on the Spitzer Space Telescope. The spectra show significant quantities of dust around the carbon stars in Sculptor, Fornax, and Leo I, but little in Carina. Previous comparisons of carbon stars with similar pulsation properties in the Galaxy and the Magellanic Clouds revealed no evidence that metallicity affected the production of dust by carbon stars. However, the more metal-poor stars in the current sample appear to be generating less dust. These data extend two known trends to lower metallicities. In more metal-poor samples, the SiC dust emission weakens, while the acetylene absorption strengthens. The bolometric magnitudes and infrared spectral properties of the carbon stars in Fornax are consistent with metallicities more similar to carbon stars in the Magellanic Clouds than in the other dwarf spheroidals in our sample. A study of the carbon budget in these stars reinforces previous considerations that the dredge-up of sufficient quantities of carbon from the stellar cores may trigger the final superwind phase, ending a star&#8217;s lifetime on the asymptotic giant branch.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/26/carbon-rich-dust-production-in-metal-poor-galaxies-in-the-local-group/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Using galaxy pairs as cosmological tracers</title>
		<link>http://voxcharta.org/2012/04/26/using-galaxy-pairs-as-cosmological-tracers/</link>
		<comments>http://voxcharta.org/2012/04/26/using-galaxy-pairs-as-cosmological-tracers/#comments</comments>
		<pubDate>Fri, 27 Apr 2012 00:51:49 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[alcock]]></category>
		<category><![CDATA[angular diameter]]></category>
		<category><![CDATA[collapsed system]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[curvature]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[expansion of the universe]]></category>
		<category><![CDATA[galaxy pair]]></category>
		<category><![CDATA[galaxy properties]]></category>
		<category><![CDATA[geometry]]></category>
		<category><![CDATA[Hubble]]></category>
		<category><![CDATA[interplay]]></category>
		<category><![CDATA[millennium]]></category>
		<category><![CDATA[peculiar velocity]]></category>
		<category><![CDATA[scales]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[tracers]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/26/using-galaxy-pairs-as-cosmological-tracers/</guid>
		<description><![CDATA[The Alcock-Paczynski (AP) effect uses the fact that, when analyzed with the correct geometry, we should observe structure that is statistically isotropic in the Universe. For structure undergoing cosmological expansion with the background, this constrains the product of the Hubble parameter and the angular diameter distance. However, the expansion of the Universe is inhomogeneous and [...]]]></description>
			<content:encoded><![CDATA[<p>The Alcock-Paczynski (AP) effect uses the fact that, when analyzed with the correct geometry, we should observe structure that is statistically isotropic in the Universe. For structure undergoing cosmological expansion with the background, this constrains the product of the Hubble parameter and the angular diameter distance. However, the expansion of the Universe is inhomogeneous and local curvature depends on density. We argue that this distorts the AP effect on small scales. After analyzing the dynamics of galaxy pairs in the Millennium simulation, we find an interplay between peculiar velocities, galaxy properties and local density that affects how pairs trace cosmological expansion. We find that only low mass, isolated galaxy pairs trace the average expansion with a minimum &#8220;correction&#8221; for peculiar velocities. Other pairs require larger, more cosmology and redshift dependent peculiar velocity corrections and, in the small-separation limit of being bound in a collapsed system, do not carry cosmological information.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/26/using-galaxy-pairs-as-cosmological-tracers/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>NGC 5466: a unique probe of the Galactic halo shape</title>
		<link>http://voxcharta.org/2012/04/26/ngc-5466-a-unique-probe-of-the-galactic-halo-shape/</link>
		<comments>http://voxcharta.org/2012/04/26/ngc-5466-a-unique-probe-of-the-galactic-halo-shape/#comments</comments>
		<pubDate>Fri, 27 Apr 2012 00:51:19 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[confidence level]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[dark matter halo]]></category>
		<category><![CDATA[galactic halo]]></category>
		<category><![CDATA[globular cluster]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[NGC]]></category>
		<category><![CDATA[oblate]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[probes]]></category>
		<category><![CDATA[shape]]></category>
		<category><![CDATA[streams]]></category>
		<category><![CDATA[tidal stream]]></category>
		<category><![CDATA[variation]]></category>
		<category><![CDATA[western edge]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/26/ngc-5466-a-unique-probe-of-the-galactic-halo-shape/</guid>
		<description><![CDATA[Stellar streams provide unique probes of galactic potentials, with the longer streams normally providing the cleaner measurements. In this paper, we show an example of a short tidal stream that is particularly sensitive to the shape of the Milky Way&#8217;s dark matter halo: the globular cluster tidal stream NGC 5466. This stream has an interesting [...]]]></description>
			<content:encoded><![CDATA[<p>Stellar streams provide unique probes of galactic potentials, with the longer streams normally providing the cleaner measurements. In this paper, we show an example of a short tidal stream that is particularly sensitive to the shape of the Milky Way&#8217;s dark matter halo: the globular cluster tidal stream NGC 5466. This stream has an interesting deviation from a smooth orbit at its western edge. We show that such a deviation favours an underlying oblate or triaxial halo (irrespective of plausible variations in the Milky Way disc properties and the specific halo parametrisation chosen); spherical or prolate halo shapes can be excluded at a high confidence level. Therefore, more extensive data sets along the NGC 5466 tidal stream promise strong constraints on the Milky Way halo shape.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/26/ngc-5466-a-unique-probe-of-the-galactic-halo-shape/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Galaxies with Background QSOs, I: A Search for Strong Galactic H-alpha Lines</title>
		<link>http://voxcharta.org/2012/04/26/galaxies-with-background-qsos-i-a-search-for-strong-galactic-h-alpha-lines/</link>
		<comments>http://voxcharta.org/2012/04/26/galaxies-with-background-qsos-i-a-search-for-strong-galactic-h-alpha-lines/#comments</comments>
		<pubDate>Fri, 27 Apr 2012 00:50:51 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[alpha emission]]></category>
		<category><![CDATA[cm 2]]></category>
		<category><![CDATA[colors]]></category>
		<category><![CDATA[digital sky survey]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[foreground]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[impact parameter]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[qso]]></category>
		<category><![CDATA[quasar]]></category>
		<category><![CDATA[quasar images]]></category>
		<category><![CDATA[sloan digital]]></category>
		<category><![CDATA[spectra]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/26/galaxies-with-background-qsos-i-a-search-for-strong-galactic-h-alpha-lines/</guid>
		<description><![CDATA[A search for emission lines in foreground galaxies in quasar spectra (z(gal) &#60; z(QSO)) of the Sloan Digital Sky Survey (SDSS) data release 5 (DR5) reveals 23 examples of quasars shining through low redshift, foreground galaxies at small impact parameters (&#60; 10 kpc). About 74,000 quasar spectra were examined by searching for narrow H{\alpha} emission [...]]]></description>
			<content:encoded><![CDATA[<p>A search for emission lines in foreground galaxies in quasar spectra (z(gal) &lt; z(QSO)) of the Sloan Digital Sky Survey (SDSS) data release 5 (DR5) reveals 23 examples of quasars shining through low redshift, foreground galaxies at small impact parameters (&lt; 10 kpc). About 74,000 quasar spectra were examined by searching for narrow H{\alpha} emission lines at z &lt; 0.38, at a flux level greater than 5 \times 10^-17 ergs cm^-2 s^-1, then confirming that other expected emission lines of the H II regions in the galaxy are detected. The galaxies were deblended from the quasar images to get colors and morphologies. For cases that allow the galaxy and the quasar to be deblended, the galaxies are blue (0.95 &lt;(u-r)&lt; 1.95). Extinction and reddening through the galaxies is determined from the (g-i) color excesses of the quasars. These reddening values are compared with the flux ratio of H{\alpha} to H{\beta}, which reflect the extinction for an undetermined fraction of the sightline through each galaxy. No trends were found relating E(B-V)_(g-i), impact parameter (b), and (u-r) for the galaxies or between E(B-V) derived from (g-i) and that derived from H{\alpha}/H{\beta}. Comparison with previous studies of quasar absorption systems indicate our sample is more reddened, suggesting disk-dominated absorber galaxies. Measurement or limits on galactic, interstellar Ca II and Na I absorption lines are given from the quasar spectrum. No trends were found relating Ca II equivalent width (W (Ca II)) or Na I equivalent width (W (Na I)) to b, but a correlation of r_s = -0.77 ({\alpha} = 0.05) was found relating W (Ca II) and E(B-V)(g-i) .</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/26/galaxies-with-background-qsos-i-a-search-for-strong-galactic-h-alpha-lines/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Discovery of Multiple Shells Around the Planetary Nebula IC 418</title>
		<link>http://voxcharta.org/2012/04/26/discovery-of-multiple-shells-around-the-planetary-nebula-ic-418/</link>
		<comments>http://voxcharta.org/2012/04/26/discovery-of-multiple-shells-around-the-planetary-nebula-ic-418/#comments</comments>
		<pubDate>Fri, 27 Apr 2012 00:49:50 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[concentric ring]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[filament]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[ic 418]]></category>
		<category><![CDATA[ir images]]></category>
		<category><![CDATA[ir imaging]]></category>
		<category><![CDATA[outer halo]]></category>
		<category><![CDATA[planetary nebula]]></category>
		<category><![CDATA[shell]]></category>
		<category><![CDATA[surface brightness]]></category>
		<category><![CDATA[time lapse]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/26/discovery-of-multiple-shells-around-the-planetary-nebula-ic-418/</guid>
		<description><![CDATA[We have analysed optical, near-, and mid-IR images of the bright planetary nebula (PN) IC 418. These images probe unambiguously for the first time a number of low surface brightness structures and shells around the bright main nebula, including radial filaments or rays, a system of three concentric rings, and two detached haloes with sizes [...]]]></description>
			<content:encoded><![CDATA[<p>We have analysed optical, near-, and mid-IR images of the bright planetary nebula (PN) IC 418. These images probe unambiguously for the first time a number of low surface brightness structures and shells around the bright main nebula, including radial filaments or rays, a system of three concentric rings, and two detached haloes with sizes ~ 150&#8243; and 220&#8243;\times250&#8243;, respectively. The main nebula is slightly off-centered with respect to the elliptical outer halo. The time-lapse between the two haloes is 10,000-50,000 yr, whereas the time-lapse between the three concentric rings is ~ 630 yr. We emphasize the advantages of near- and mid-IR imaging for the detection of faint structures and shells around optically bright nebulae.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/26/discovery-of-multiple-shells-around-the-planetary-nebula-ic-418/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>IAU (Maser) Symposium 285 Summary</title>
		<link>http://voxcharta.org/2012/04/26/iau-maser-symposium-285-summary/</link>
		<comments>http://voxcharta.org/2012/04/26/iau-maser-symposium-285-summary/#comments</comments>
		<pubDate>Fri, 27 Apr 2012 00:46:51 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cosmic masers]]></category>
		<category><![CDATA[iau]]></category>
		<category><![CDATA[maser]]></category>
		<category><![CDATA[oral presentations]]></category>
		<category><![CDATA[posters]]></category>
		<category><![CDATA[science]]></category>
		<category><![CDATA[stellenbosch south africa]]></category>
		<category><![CDATA[symposium]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/26/iau-maser-symposium-285-summary/</guid>
		<description><![CDATA[I&#8217;m trying to summarize the science communicated via oral presentations and by posters at the IAU Symposium 285 &#8220;Cosmic Masers &#8211; from OH to H_0&#8243;, which took place from January 29 to February 3, 2012 in Stellenbosch, South Africa.
]]></description>
			<content:encoded><![CDATA[<p>I&#8217;m trying to summarize the science communicated via oral presentations and by posters at the IAU Symposium 285 &#8220;Cosmic Masers &#8211; from OH to H_0&#8243;, which took place from January 29 to February 3, 2012 in Stellenbosch, South Africa.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/26/iau-maser-symposium-285-summary/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The physics and the structure of the quasar-driven outflow in Mrk 231</title>
		<link>http://voxcharta.org/2012/04/26/the-physics-and-the-structure-of-the-quasar-driven-outflow-in-mrk-231/</link>
		<comments>http://voxcharta.org/2012/04/26/the-physics-and-the-structure-of-the-quasar-driven-outflow-in-mrk-231/#comments</comments>
		<pubDate>Fri, 27 Apr 2012 00:44:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[AGN]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[critical density]]></category>
		<category><![CDATA[dense clump]]></category>
		<category><![CDATA[diffuse cloud]]></category>
		<category><![CDATA[diffuse component]]></category>
		<category><![CDATA[distance]]></category>
		<category><![CDATA[evolutionary model]]></category>
		<category><![CDATA[excitation]]></category>
		<category><![CDATA[hole accretion]]></category>
		<category><![CDATA[latter result]]></category>
		<category><![CDATA[molecular outflow]]></category>
		<category><![CDATA[radiation pressure]]></category>
		<category><![CDATA[red wing]]></category>
		<category><![CDATA[shock]]></category>
		<category><![CDATA[sigma]]></category>
		<category><![CDATA[significance level]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[transition]]></category>
		<category><![CDATA[velocities]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/26/the-physics-and-the-structure-of-the-quasar-driven-outflow-in-mrk-231/</guid>
		<description><![CDATA[Massive AGN-driven outflows are invoked by AGN-galaxy co-evolutionary models to suppress both star formation and black hole accretion. Massive molecular outflows have recently been revealed in some AGN hosts. However, the physical properties and structure of these AGN-driven molecular outflows are still poorly constrained. Here we present new IRAM PdBI observations of Mrk231, the closest [...]]]></description>
			<content:encoded><![CDATA[<p>Massive AGN-driven outflows are invoked by AGN-galaxy co-evolutionary models to suppress both star formation and black hole accretion. Massive molecular outflows have recently been revealed in some AGN hosts. However, the physical properties and structure of these AGN-driven molecular outflows are still poorly constrained. Here we present new IRAM PdBI observations of Mrk231, the closest quasar known, targeting both the CO(1-0) and CO(2-1) transitions. We detect broad wings in both transitions, tracing a massive molecular outflow with velocities up to 800 km/s. The wings are spatially resolved at high significance level (5-11 sigma), indicating that the molecular outflow extends on the kpc scale. The CO(2-1)/CO(1-0) ratio of the red broad wings is consistent with the ratio observed in the narrow core, while the blue broad wing is less excited than the core. The latter result suggests that quasar driven outflow models invoking shocks (which would predict higher gas excitation) are not appropriate to describe the bulk of the outflow in Mrk231. However, we note that within the central 700 pc the CO(2-1)/CO(1-0) ratio of the red wing is slightly, but significantly, higher than in the line core, suggesting that shocks may play a role in the central region. We also find that the average size of the outflow anticorrelates with the critical density of the transition used as a wind tracer. This indicates that, although diffuse and dense clumps coexist in the outflowing gas, dense outflowing clouds have shorter lifetime and that they evaporate into the diffuse component along the outflow or, more simply, that diffuse clouds are more efficiently accelerated to larger distances by radiation pressure.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/26/the-physics-and-the-structure-of-the-quasar-driven-outflow-in-mrk-231/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Remarkable High Pressure of the Local Leo Cold Cloud</title>
		<link>http://voxcharta.org/2012/04/26/the-remarkable-high-pressure-of-the-local-leo-cold-cloud/</link>
		<comments>http://voxcharta.org/2012/04/26/the-remarkable-high-pressure-of-the-local-leo-cold-cloud/#comments</comments>
		<pubDate>Fri, 27 Apr 2012 00:40:35 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[background star]]></category>
		<category><![CDATA[cloud temperature]]></category>
		<category><![CDATA[cold cloud]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[dense structure]]></category>
		<category><![CDATA[density variation]]></category>
		<category><![CDATA[depletion pattern]]></category>
		<category><![CDATA[hubble space telescope]]></category>
		<category><![CDATA[interstellar cloud]]></category>
		<category><![CDATA[llcc]]></category>
		<category><![CDATA[motion background]]></category>
		<category><![CDATA[proper motion]]></category>
		<category><![CDATA[sightline]]></category>
		<category><![CDATA[space telescope imaging]]></category>
		<category><![CDATA[stis]]></category>
		<category><![CDATA[two stars]]></category>
		<category><![CDATA[ultraviolet spectra]]></category>
		<category><![CDATA[warm cloud]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/26/the-remarkable-high-pressure-of-the-local-leo-cold-cloud/</guid>
		<description><![CDATA[Using the Space Telescope Imaging Spectrograph (STIS) onboard the Hubble Space Telescope, we have obtained high-resolution ultraviolet spectra of the C I absorption toward two stars behind the Local Leo Cold Cloud (LLCC). At a distance (~20 pc) that places it well inside the Local Bubble, the LLCC is the nearest example of the coldest [...]]]></description>
			<content:encoded><![CDATA[<p>Using the Space Telescope Imaging Spectrograph (STIS) onboard the Hubble Space Telescope, we have obtained high-resolution ultraviolet spectra of the C I absorption toward two stars behind the Local Leo Cold Cloud (LLCC). At a distance (~20 pc) that places it well inside the Local Bubble, the LLCC is the nearest example of the coldest known (T~20 K) diffuse interstellar clouds. The STIS measurements of the C I fine-structure excitation toward HD 85259 and HD 83023 indicate that the thermal gas pressure of the LLCC is much greater than that of the warm clouds in the Local Bubble. The mean LLCC pressure measured toward these two stars (60,000 cm$^{-3}$ K) implies an H I density of ~3000 cm$^{-3}$ and a cloud thickness of ~200 AU at the 20 K cloud temperature. Such a thin, cold, dense structure could arise at the collision interface between converging flows of warm gas. However, the measured LLCC pressure is appreciably higher than that expected in the colliding cloud interpretation given the velocity and column density constraints on warm clouds in the HD 85259 and HD 83023 sightlines. Additional STIS measurements of the Zn II, Ni II, and Cr II column densities toward HD 85259 indicate that the LLCC has a modest &#8220;warm cloud&#8221; dust depletion pattern consistent with its low dust-to-gas ratio determined from H I 21 cm and 100 micron observations. In support of the inferred sheet-like geometry for the LLCC, a multi-epoch comparison of the Na I absorption toward a high-proper-motion background star reveals a 40% column density variation indicative of LLCC Na I structure on a scale of ~50 AU.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/26/the-remarkable-high-pressure-of-the-local-leo-cold-cloud/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Non-Equilibrium Chemistry of Dynamically Evolving Prestellar Cores: I. Basic Magnetic and Non-Magnetic Models and Parameter Studies [Replacement]</title>
		<link>http://voxcharta.org/2012/04/26/non-equilibrium-chemistry-of-dynamically-evolving-prestellar-cores-i-basic-magnetic-and-non-magnetic-models-and-parameter-studies-replacement/</link>
		<comments>http://voxcharta.org/2012/04/26/non-equilibrium-chemistry-of-dynamically-evolving-prestellar-cores-i-basic-magnetic-and-non-magnetic-models-and-parameter-studies-replacement/#comments</comments>
		<pubDate>Fri, 27 Apr 2012 00:38:12 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[central density]]></category>
		<category><![CDATA[collapse]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[delay time]]></category>
		<category><![CDATA[dynamical model]]></category>
		<category><![CDATA[equilibrium]]></category>
		<category><![CDATA[evolutionary stage]]></category>
		<category><![CDATA[hcn]]></category>
		<category><![CDATA[hco]]></category>
		<category><![CDATA[magnetic cores]]></category>
		<category><![CDATA[magnetic model]]></category>
		<category><![CDATA[magnetic support]]></category>
		<category><![CDATA[model parameter]]></category>
		<category><![CDATA[molecular cloud core]]></category>
		<category><![CDATA[nh2]]></category>
		<category><![CDATA[nh3]]></category>
		<category><![CDATA[outer layers]]></category>
		<category><![CDATA[parameter studies]]></category>
		<category><![CDATA[quantitative difference]]></category>
		<category><![CDATA[timescale]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/26/non-equilibrium-chemistry-of-dynamically-evolving-prestellar-cores-i-basic-magnetic-and-non-magnetic-models-and-parameter-studies-replacement/</guid>
		<description><![CDATA[We combine dynamical and non-equilibrium chemical modeling of evolving prestellar molecular cloud cores, and explore the evolution of molecular abundances in the contracting core. We model both magnetic cores, with varying degrees of initial magnetic support, and non-magnetic cores, with varying collapse delay times. We explore, through a parameter study, the competing effects of various [...]]]></description>
			<content:encoded><![CDATA[<p>We combine dynamical and non-equilibrium chemical modeling of evolving prestellar molecular cloud cores, and explore the evolution of molecular abundances in the contracting core. We model both magnetic cores, with varying degrees of initial magnetic support, and non-magnetic cores, with varying collapse delay times. We explore, through a parameter study, the competing effects of various model parameters in the evolving molecular abundances, including the elemental C/O ratio, the temperature, and the cosmic-ray ionization rate. We find that different models show their largest quantitative differences at the center of the core, whereas the outer layers, which evolve slower, have abundances which are severely degenerate among different dynamical models. There is a large range of possible abundance values for different models at a fixed evolutionary stage (central density), which demonstrates the large potential of chemical differentiation in prestellar cores. However, degeneracies among different models, compounded with uncertainties induced by other model parameters, make it difficult to discriminate among dynamical models. To address these difficulties, we identify abundance ratios between particular molecules, the measurement of which would have maximal potential for discrimination among the different models examined here. In particular, we find that the ratios between NH3 and CO; NH2 and CO; NH3 and HCO+ are sensitive to the evolutionary timescale, and that the ratio between HCN and OH is sensitive to the C/O ratio. Finally, we demonstrate that measurements of the central deviation (central depletion or enhancement) of abundances of certain molecules are good indicators of the dynamics of the core.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/26/non-equilibrium-chemistry-of-dynamically-evolving-prestellar-cores-i-basic-magnetic-and-non-magnetic-models-and-parameter-studies-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Herschel Observations of a Potential Core Forming Clump: Perseus B1-E [Replacement]</title>
		<link>http://voxcharta.org/2012/04/26/herschel-observations-of-a-potential-core-forming-clump-perseus-b1-e-replacement-2/</link>
		<comments>http://voxcharta.org/2012/04/26/herschel-observations-of-a-potential-core-forming-clump-perseus-b1-e-replacement-2/#comments</comments>
		<pubDate>Fri, 27 Apr 2012 00:37:41 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[clump]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[continuum observations]]></category>
		<category><![CDATA[core formation]]></category>
		<category><![CDATA[dense core]]></category>
		<category><![CDATA[e region]]></category>
		<category><![CDATA[green bank telescope]]></category>
		<category><![CDATA[herschel]]></category>
		<category><![CDATA[initial condition]]></category>
		<category><![CDATA[loose grouping]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[measure temperature]]></category>
		<category><![CDATA[micron]]></category>
		<category><![CDATA[myr]]></category>
		<category><![CDATA[nearest neighbour]]></category>
		<category><![CDATA[solar mass]]></category>
		<category><![CDATA[spectral line observations]]></category>
		<category><![CDATA[substructure]]></category>
		<category><![CDATA[timescale]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/26/herschel-observations-of-a-potential-core-forming-clump-perseus-b1-e-replacement-2/</guid>
		<description><![CDATA[We present continuum observations of the Perseus B1-E region from the Herschel Gould Belt Survey. These Herschel data reveal a loose grouping of substructures at 160 &#8211; 500 micron not seen in previous submillimetre observations. We measure temperature and column density from these data and select the nine densest and coolest substructures for follow-up spectral [...]]]></description>
			<content:encoded><![CDATA[<p>We present continuum observations of the Perseus B1-E region from the Herschel Gould Belt Survey. These Herschel data reveal a loose grouping of substructures at 160 &#8211; 500 micron not seen in previous submillimetre observations. We measure temperature and column density from these data and select the nine densest and coolest substructures for follow-up spectral line observations with the Green Bank Telescope. We find that the B1-E clump has a mass of ~ 100 solar masses and appears to be gravitationally bound. Furthermore, of the nine substructures examined here, one substructure (B1-E2) appears to be itself bound. The substructures are typically less than a Jeans length from their nearest neighbour and thus, may interact on a timescale of ~ 1 Myr. We propose that B1-E may be forming a first generation of dense cores, which could provide important constraints on the initial conditions of prestellar core formation. Our results suggest that B1-E may be influenced by a strong, localized magnetic field, but further observations are still required.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/04/26/herschel-observations-of-a-potential-core-forming-clump-perseus-b1-e-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Non-Thermal Insights on Mass and Energy Flows Through the Galactic Centre and into the Fermi Bubbles [Replacement]</title>
		<link>http://voxcharta.org/2012/04/26/non-thermal-insights-on-mass-and-energy-flows-through-the-galactic-centre-and-into-the-fermi-bubbles-replacement/</link>
		<comments>http://voxcharta.org/2012/04/26/non-thermal-insights-on-mass-and-energy-flows-through-the-galactic-centre-and-into-the-fermi-bubbles-replacement/#comments</comments>
		<pubDate>Fri, 27 Apr 2012 00:35:53 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[condensation]]></category>
		<category><![CDATA[coronal gas]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[energy flow]]></category>
		<category><![CDATA[galactic centre]]></category>
		<category><![CDATA[galactic halo]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[gyr]]></category>
		<category><![CDATA[inner galaxy]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[msun]]></category>
		<category><![CDATA[nuclear bulge]]></category>
		<category><![CDATA[outflow]]></category>
		<category><![CDATA[quiescent state]]></category>
		<category><![CDATA[radio continuum]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[sustenance]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/26/non-thermal-insights-on-mass-and-energy-flows-through-the-galactic-centre-and-into-the-fermi-bubbles-replacement/</guid>
		<description><![CDATA[We construct a simple model of the star-formation- (and resultant supernova-) driven mass and energy flows through the inner ~200 pc (in diameter) of the Galaxy. Our modelling is constrained, in particular, by the non-thermal radio continuum and {\gamma}-ray signals detected from the region. The modelling points to a current star-formation rate of 0.04 &#8211; [...]]]></description>
			<content:encoded><![CDATA[<p>We construct a simple model of the star-formation- (and resultant supernova-) driven mass and energy flows through the inner ~200 pc (in diameter) of the Galaxy. Our modelling is constrained, in particular, by the non-thermal radio continuum and {\gamma}-ray signals detected from the region. The modelling points to a current star-formation rate of 0.04 &#8211; 0.12 M\msun/year at 2{\sigma} confidence within the region with best-fit value in the range 0.08 &#8211; 0.12 M\msun/year which &#8211; if sustained over 10 Gyr &#8211; would fill out the ~ 10^9 M\msun stellar population of the nuclear bulge. Mass is being accreted on to the Galactic centre (GC) region at a rate ~0.3M\msun/year. The region&#8217;s star-formation activity drives an outflow of plasma, cosmic rays, and entrained, cooler gas. Neither the plasma nor the entrained gas reaches the gravitational escape speed, however, and all this material fountains back on to the inner Galaxy. The system we model can naturally account for the recently-observed ~&gt; 10^6 &#8216;halo&#8217; of molecular gas surrounding the Central Molecular Zone out to 100-200 pc heights. The injection of cooler, high-metallicity material into the Galactic halo above the GC may catalyse the subsequent cooling and condensation of hot plasma out of this region and explain the presence of relatively pristine, nuclear-unprocessed gas in the GC. The plasma outflow from the GC reaches a height of a few kpc and is compellingly related to the recently-discovered Fermi Bubbles. Our modelling demonstrates that ~ 10^9 M\msun of hot gas is processed through the GC over 10 Gyr. We speculate that the continual star-formation in the GC over the age of the Milky Way has kept the SMBH in a quiescent state thus preventing it from significantly heating the coronal gas, allowing for the continual accretion of gas on to the disk and the sustenance of star formation on much wider scales in the Galaxy [abridged].</p>
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			<wfw:commentRss>http://voxcharta.org/2012/04/26/non-thermal-insights-on-mass-and-energy-flows-through-the-galactic-centre-and-into-the-fermi-bubbles-replacement/feed/</wfw:commentRss>
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		<title>Sizes, Half-Mass Densities, and Mass Functions of Star Clusters in the Merger Remnant NGC 1316: Clues to the Fate of Second-Generation Globular Clusters [Replacement]</title>
		<link>http://voxcharta.org/2012/04/26/sizes-half-mass-densities-and-mass-functions-of-star-clusters-in-the-merger-remnant-ngc-1316-clues-to-the-fate-of-second-generation-globular-clusters-replacement-2/</link>
		<comments>http://voxcharta.org/2012/04/26/sizes-half-mass-densities-and-mass-functions-of-star-clusters-in-the-merger-remnant-ngc-1316-clues-to-the-fate-of-second-generation-globular-clusters-replacement-2/#comments</comments>
		<pubDate>Fri, 27 Apr 2012 00:33:50 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[age population]]></category>
		<category><![CDATA[body relaxation]]></category>
		<category><![CDATA[density rho]]></category>
		<category><![CDATA[faint fuzzies]]></category>
		<category><![CDATA[galaxy ngc]]></category>
		<category><![CDATA[globular cluster]]></category>
		<category><![CDATA[gyr]]></category>
		<category><![CDATA[initial distribution]]></category>
		<category><![CDATA[initial mass function]]></category>
		<category><![CDATA[inner regions]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[lenticular galaxy]]></category>
		<category><![CDATA[luminosity function]]></category>
		<category><![CDATA[mass density]]></category>
		<category><![CDATA[mass function]]></category>
		<category><![CDATA[maximum value]]></category>
		<category><![CDATA[radii]]></category>
		<category><![CDATA[remnant]]></category>
		<category><![CDATA[star cluster]]></category>
		<category><![CDATA[type galaxy]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/04/26/sizes-half-mass-densities-and-mass-functions-of-star-clusters-in-the-merger-remnant-ngc-1316-clues-to-the-fate-of-second-generation-globular-clusters-replacement-2/</guid>
		<description><![CDATA[We study mass functions of globular clusters derived from HST/ACS images of the early-type merger remnant galaxy NGC 1316 which hosts a significant population of metal-rich globular clusters of intermediate age (~3 Gyr). For the old, metal-poor (`blue&#8217;) clusters, the peak mass of the mass function M_p increases with internal half-mass density rho_h as (M_p [...]]]></description>
			<content:encoded><![CDATA[<p>We study mass functions of globular clusters derived from HST/ACS images of the early-type merger remnant galaxy NGC 1316 which hosts a significant population of metal-rich globular clusters of intermediate age (~3 Gyr). For the old, metal-poor (`blue&#8217;) clusters, the peak mass of the mass function M_p increases with internal half-mass density rho_h as (M_p proportional to rho_h^0.44) whereas it stays approximately constant with galactocentric distance R_gal. The mass functions of these clusters are consistent with a simple scenario in which they formed with a Schechter initial mass function and evolved subsequently by internal two-body relaxation. For the intermediate-age population of metal-rich (&#8220;red&#8221;) clusters, the faint end of the previously reported power-law luminosity function of the clusters with R_gal &gt; 9 kpc is due to many of those clusters having radii larger than the theoretical maximum value imposed by the tidal field of NGC 1316 at their R_gal. This renders disruption by two-body relaxation ineffective. Only a few such diffuse clusters are found in the inner regions of NGC 1316. Completeness tests indicate that this is a physical effect. Using comparisons with star clusters in other galaxies and cluster disruption calculations using published models, we hypothesize that most red clusters in the low-rho_h tail of the initial distribution have already been destroyed in the inner regions of NGC 1316 by tidal shocking, and that several remaining low-rho_h clusters will evolve dynamically to become similar to &#8220;faint fuzzies&#8221; that exist in several lenticular galaxies. Finally, we discuss the nature of diffuse red clusters in early-type galaxies.</p>
]]></content:encoded>
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