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	<title>Vox Charta &#187; astro-ph</title>
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	<link>http://voxcharta.org</link>
	<description></description>
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		<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>The darkness that shaped the void: dark energy and cosmic voids</title>
		<link>http://voxcharta.org/2012/05/21/the-darkness-that-shaped-the-void-dark-energy-and-cosmic-voids/</link>
		<comments>http://voxcharta.org/2012/05/21/the-darkness-that-shaped-the-void-dark-energy-and-cosmic-voids/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:55:07 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bia]]></category>
		<category><![CDATA[body simulation]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[dark matter distribution]]></category>
		<category><![CDATA[darkness]]></category>
		<category><![CDATA[ellipticity]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[galaxy distribution]]></category>
		<category><![CDATA[galaxy redshift survey]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[morphological properties]]></category>
		<category><![CDATA[population]]></category>
		<category><![CDATA[redshift distortions]]></category>
		<category><![CDATA[shape]]></category>
		<category><![CDATA[sigma]]></category>
		<category><![CDATA[sparsity]]></category>
		<category><![CDATA[watershed]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/the-darkness-that-shaped-the-void-dark-energy-and-cosmic-voids/</guid>
		<description><![CDATA[Aims: We assess the sensitivity of void shapes to the nature of dark energy that was pointed out in recent studies. We investigate whether or not void shapes are useable as an observational probe in galaxy redshift surveys. We focus on the evolution of the mean void ellipticity and its underlying physical cause. Methods: We [...]]]></description>
			<content:encoded><![CDATA[<p>Aims: We assess the sensitivity of void shapes to the nature of dark energy that was pointed out in recent studies. We investigate whether or not void shapes are useable as an observational probe in galaxy redshift surveys. We focus on the evolution of the mean void ellipticity and its underlying physical cause. Methods: We analyse the morphological properties of voids in five sets of cosmological N-body simulations, each with a different nature of dark energy. Comparing voids in the dark matter distribution to those in the halo population, we address the question of whether galaxy redshift surveys yield sufficiently accurate void morphologies. Voids are identified using the parameter free Watershed Void Finder. The effect of redshift distortions is investigated as well. Results: We confirm the statistically significant sensitivity of voids in the dark matter distribution. We identify the level of clustering as measured by \sigma_8(z) as the main cause of differences in mean void shape . We find that in the halo and/or galaxy distribution it is practically unfeasible to distinguish at a statistically significant level between the various cosmologies due to the sparsity and spatial bias of the sample.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/the-darkness-that-shaped-the-void-dark-energy-and-cosmic-voids/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The optically unbiased GRB host (TOUGH) survey. VI. Radio observations at z&lt;1 and consistency with typical star-forming galaxies</title>
		<link>http://voxcharta.org/2012/05/21/the-optically-unbiased-grb-host-tough-survey-vi-radio-observations-at-z1-and-consistency-with-typical-star-forming-galaxies/</link>
		<comments>http://voxcharta.org/2012/05/21/the-optically-unbiased-grb-host-tough-survey-vi-radio-observations-at-z1-and-consistency-with-typical-star-forming-galaxies/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:54:52 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[radio observation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/the-optically-unbiased-grb-host-tough-survey-vi-radio-observations-at-z1-and-consistency-with-typical-star-forming-galaxies/</guid>
		<description><![CDATA[We present late-time Hubble Space Telescope imaging of the fields of six Swift GRBs lying at 5.0&#60;z&#60;9.5. Our data includes very deep observations of the field of the most distant spectroscopically confirmed burst, GRB 090423, at z=8.2. Using the precise positions afforded by their afterglows we can place stringent limits on the luminosities of their [...]]]></description>
			<content:encoded><![CDATA[<p>We present late-time Hubble Space Telescope imaging of the fields of six Swift GRBs lying at 5.0&lt;z&lt;9.5. Our data includes very deep observations of the field of the most distant spectroscopically confirmed burst, GRB 090423, at z=8.2. Using the precise positions afforded by their afterglows we can place stringent limits on the luminosities of their host galaxies. In one case, that of GRB 060522 at z=5.11, there is a marginal excess of flux close to the GRB position which may be a detection of a host at a magnitude J(AB)=28.5. None of the others are significantly detected meaning that all the hosts lie below L\star at their respective redshifts, with star formation rates SFR&lt;4Mo/yr in all cases. Indeed, stacking the five fields with WFC3-IR data we conclude a mean SFR&lt;0.17Mo/yr per galaxy. These results support the proposition that the bulk of star formation, and hence integrated UV luminosity, at high redshifts arises in galaxies below the detection limits of deep-field observations. Making the reasonable assumption that GRB rate is proportional to UV luminosity at early times allows us to compare our limits with expectations based on galaxy luminosity functions derived from the Hubble Ultra-Deep Field (HUDF) and other deep fields. We infer that a luminosity function which is evolving rapidly towards steeper faint-end slope (alpha) and decreasing characteristic luminosity (L\star), as suggested by some other studies, is consistent with our observations, whereas a non-evolving LF shape is ruled out at &gt;90% confidence. Although it is not yet possible to make stronger statements, in the future, with larger samples and a fuller understanding of the conditions required for GRB production, studies like this hold great potential for probing the nature of star formation, the shape of the galaxy luminosity function, and the supply of ionizing photons in the early universe.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/the-optically-unbiased-grb-host-tough-survey-vi-radio-observations-at-z1-and-consistency-with-typical-star-forming-galaxies/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>Self-accelerating Massive Gravity: Exact solutions for any isotropic matter distribution [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/21/self-accelerating-massive-gravity-exact-solutions-for-any-isotropic-matter-distribution-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/21/self-accelerating-massive-gravity-exact-solutions-for-any-isotropic-matter-distribution-cross-listing/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:54:28 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[arbitrary time]]></category>
		<category><![CDATA[cosmological constant]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[degrees of freedom]]></category>
		<category><![CDATA[exact solution]]></category>
		<category><![CDATA[graviton]]></category>
		<category><![CDATA[massive gravity]]></category>
		<category><![CDATA[matter distribution]]></category>
		<category><![CDATA[matter fields]]></category>
		<category><![CDATA[perturbation]]></category>
		<category><![CDATA[sources of stress]]></category>
		<category><![CDATA[symmetric distribution]]></category>
		<category><![CDATA[time dependence]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/self-accelerating-massive-gravity-exact-solutions-for-any-isotropic-matter-distribution-cross-listing/</guid>
		<description><![CDATA[We present an exact solution to the equations of massive gravity that display cosmological constant-like behavior for any spherically symmetric distribution of matter, including arbitrary time dependence. On this solution, the new degrees of freedom from the massive graviton generate a cosmological constant-like contribution to stress-energy that does not interact directly with other matter sources. [...]]]></description>
			<content:encoded><![CDATA[<p>We present an exact solution to the equations of massive gravity that display cosmological constant-like behavior for any spherically symmetric distribution of matter, including arbitrary time dependence. On this solution, the new degrees of freedom from the massive graviton generate a cosmological constant-like contribution to stress-energy that does not interact directly with other matter sources. When the effective cosmological constant contribution dominates over other sources of stress energy the cosmological expansion self-accelerates, even when no other dark-energy-like ingredients are present. The new degrees of freedom introduced by giving the graviton the mass do not respond to arbitrarily large radial or homogeneous perturbations from other matter fields on this solution. We comment on possible implications of this result.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/self-accelerating-massive-gravity-exact-solutions-for-any-isotropic-matter-distribution-cross-listing/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>The Correlated Formation Histories of Massive Galaxies and Their Dark Matter Halos</title>
		<link>http://voxcharta.org/2012/05/21/the-correlated-formation-histories-of-massive-galaxies-and-their-dark-matter-halos/</link>
		<comments>http://voxcharta.org/2012/05/21/the-correlated-formation-histories-of-massive-galaxies-and-their-dark-matter-halos/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:53:48 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[angular momentum]]></category>
		<category><![CDATA[central galaxy]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[cosmos field]]></category>
		<category><![CDATA[dark matter halo]]></category>
		<category><![CDATA[formation history]]></category>
		<category><![CDATA[independent source]]></category>
		<category><![CDATA[large scale]]></category>
		<category><![CDATA[massive galaxy]]></category>
		<category><![CDATA[morphology]]></category>
		<category><![CDATA[redshift range]]></category>
		<category><![CDATA[scale environment]]></category>
		<category><![CDATA[scales]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[stochastic process]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/the-correlated-formation-histories-of-massive-galaxies-and-their-dark-matter-halos/</guid>
		<description><![CDATA[Using observations in the COSMOS field, we report an intriguing correlation between the star formation activity of massive (~10^{11.4}\msol) central galaxies, their stellar masses, and the large-scale (~10 Mpc) environments of their group-mass (~10^{13.6}\msol) dark matter halos. Probing the redshift range z=[0.2,1.0], our measurements come from two independent sources: an X-ray detected group catalog and [...]]]></description>
			<content:encoded><![CDATA[<p>Using observations in the COSMOS field, we report an intriguing correlation between the star formation activity of massive (~10^{11.4}\msol) central galaxies, their stellar masses, and the large-scale (~10 Mpc) environments of their group-mass (~10^{13.6}\msol) dark matter halos. Probing the redshift range z=[0.2,1.0], our measurements come from two independent sources: an X-ray detected group catalog and constraints on the stellar-to-halo mass relation derived from a combination of clustering and weak lensing statistics. At z=1, we find that the stellar mass in star-forming centrals is a factor of two less than in passive centrals at the same halo mass. This implies that the presence or lack of star formation in group-scale centrals cannot be a stochastic process. By z=0, the offset reverses, probably as a result of the different growth rates of these objects. A similar but weaker trend is observed when dividing the sample by morphology rather than star formation. Remarkably, we find that star-forming centrals at z~1 live in groups that are significantly more clustered on 10 Mpc scales than similar mass groups hosting passive centrals. We discuss this signal in the context of halo assembly and recent simulations, suggesting that star-forming centrals prefer halos with higher angular momentum and/or formation histories with more recent growth; such halos are known to evolve in denser large-scale environments. If confirmed, this would be evidence of an early established link between the assembly history of halos on large scales and the future properties of the galaxies that form inside them.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/the-correlated-formation-histories-of-massive-galaxies-and-their-dark-matter-halos/feed/</wfw:commentRss>
		<slash:comments>1</slash:comments>
		</item>
		<item>
		<title>X-ray variability of 104 active galactic nuclei. XMM-Newton power-spectrum density profiles</title>
		<link>http://voxcharta.org/2012/05/21/x-ray-variability-of-104-active-galactic-nuclei-xmm-newton-power-spectrum-density-profiles/</link>
		<comments>http://voxcharta.org/2012/05/21/x-ray-variability-of-104-active-galactic-nuclei-xmm-newton-power-spectrum-density-profiles/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:53:36 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></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[correspondence]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[density profile]]></category>
		<category><![CDATA[Newton]]></category>
		<category><![CDATA[power spectra]]></category>
		<category><![CDATA[power spectrum]]></category>
		<category><![CDATA[ray binaries]]></category>
		<category><![CDATA[scales]]></category>
		<category><![CDATA[shape]]></category>
		<category><![CDATA[uniform analysis]]></category>
		<category><![CDATA[variability]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/x-ray-variability-of-104-active-galactic-nuclei-xmm-newton-power-spectrum-density-profiles/</guid>
		<description><![CDATA[AGN, powered by accretion onto SMBHs, are thought to be scaled up versions of Galactic black hole X-ray binaries (BH-XRBs). In the past few years evidence of such correspondence include similarities in the broadband shape of the X-ray variability power spectra, with characteristic bend times-scales scaling with mass. We have performed a uniform analysis of [...]]]></description>
			<content:encoded><![CDATA[<p>AGN, powered by accretion onto SMBHs, are thought to be scaled up versions of Galactic black hole X-ray binaries (BH-XRBs). In the past few years evidence of such correspondence include similarities in the broadband shape of the X-ray variability power spectra, with characteristic bend times-scales scaling with mass. We have performed a uniform analysis of the power spectrum densities (PSDs) of 104 nearby (z&lt;0.4) AGN using 209 XMM-Newton/pn observations. The PSDs have been estimated in three energy bands: 0.2-10, 0.2-2, and 2-10 keV. The sample comprises 61 Type-1 AGN, 21 Type-2 AGN, 15 NLSy1, and 7 BLLACS. We have fitted each PSD to two models: (1) a single power-law model and (2) a bending power-law model. Among the entire sample, 72% show significant variability in at least one of the three bands tested. A high percentage of low-luminosity AGN do not show any significant variability. The PSD of the majority of the variable AGN was well described by a simple power-law with a mean index of 2. In 15 sources we found that the bending power law model was preferred with a mean slope of 3 and a mean bend frequency of 2.E-04 Hz. Only KUG1031+398 (REJ1034+396) shows evidence for quasi-periodic oscillations. The `fundamental plane&#039; relating variability timescale, black hole mass, and luminosity is demonstrated using the new X-ray timing results presented here together with a compilation of the previously detected timescales from the literature. Both quantitative (i.e. scaling with BH mass) and qualitative (overall PSD shapes) found in this sample of AGN are in agreement with the expectations for the SMBHs and BH-XRBs being the same phenomenon scaled-up with the size of the BH. The steep PSD slopes above the high frequency bend bear a closer resemblance to those of the `soft/thermal dominated&#039; BH-XRB states than other states.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/x-ray-variability-of-104-active-galactic-nuclei-xmm-newton-power-spectrum-density-profiles/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Galaxies in X-ray Groups II: A Weak Lensing Study of Halo Centering</title>
		<link>http://voxcharta.org/2012/05/21/galaxies-in-x-ray-groups-ii-a-weak-lensing-study-of-halo-centering/</link>
		<comments>http://voxcharta.org/2012/05/21/galaxies-in-x-ray-groups-ii-a-weak-lensing-study-of-halo-centering/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:53:20 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bright galaxy]]></category>
		<category><![CDATA[consequence]]></category>
		<category><![CDATA[cosmos field]]></category>
		<category><![CDATA[dark matter halo]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[galaxy group]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[mass profiles]]></category>
		<category><![CDATA[massive galaxy]]></category>
		<category><![CDATA[plasma]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[tracers]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/galaxies-in-x-ray-groups-ii-a-weak-lensing-study-of-halo-centering/</guid>
		<description><![CDATA[Locating the centers of dark matter halos is critical for understanding the mass profiles of halos as well as the formation and evolution of the massive galaxies that they host. The task is observationally challenging because we cannot observe halos directly, and tracers such as bright galaxies or X-ray emission from hot plasma are imperfect. [...]]]></description>
			<content:encoded><![CDATA[<p>Locating the centers of dark matter halos is critical for understanding the mass profiles of halos as well as the formation and evolution of the massive galaxies that they host. The task is observationally challenging because we cannot observe halos directly, and tracers such as bright galaxies or X-ray emission from hot plasma are imperfect. In this paper we quantify the consequences of miscentering on the weak lensing signal from a sample of 129 X-ray selected galaxy groups in the COSMOS field with redshifts 0&lt;z&lt;1 and halo masses in the range 10^13 &#8211; 10^14 M_sun. By measuring the stacked lensing signal around eight different candidate centers (such as the brightest member galaxy, the mean position of all member galaxies, or the X-ray centroid), we determine which candidates best trace the center of mass in halos. In this sample of groups, we find that massive galaxies near the X-ray centroids trace the center of mass to &lt;~75 kpc, while the X-ray position and centroids based on the mean position of member galaxies have larger offsets primarily due to the statistical uncertainties in their positions (typically ~50-150 kpc). Approximately 30% of groups in our sample have ambiguous centers with multiple bright or massive galaxies, and these groups show disturbed mass profiles that are not well fit by standard models, suggesting that they are merging systems. We find halo mass estimates from stacked weak lensing can be biased low by 5-30% if inaccurate centers are used and the issue of miscentering is not addressed.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/galaxies-in-x-ray-groups-ii-a-weak-lensing-study-of-halo-centering/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A Public Set of Synthetic Spectra from Expanding Atmospheres for X-Ray Novae. I. Solar Abundances</title>
		<link>http://voxcharta.org/2012/05/21/a-public-set-of-synthetic-spectra-from-expanding-atmospheres-for-x-ray-novae-i-solar-abundances/</link>
		<comments>http://voxcharta.org/2012/05/21/a-public-set-of-synthetic-spectra-from-expanding-atmospheres-for-x-ray-novae-i-solar-abundances/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:53:03 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorption line]]></category>
		<category><![CDATA[abundance]]></category>
		<category><![CDATA[atmosphere]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[eff]]></category>
		<category><![CDATA[example application]]></category>
		<category><![CDATA[grating]]></category>
		<category><![CDATA[line profile]]></category>
		<category><![CDATA[mass loss]]></category>
		<category><![CDATA[model parameter]]></category>
		<category><![CDATA[SGR]]></category>
		<category><![CDATA[solar set]]></category>
		<category><![CDATA[static model]]></category>
		<category><![CDATA[stellar atmosphere]]></category>
		<category><![CDATA[synthetic spectra]]></category>
		<category><![CDATA[van rossum]]></category>
		<category><![CDATA[white dwarf]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/a-public-set-of-synthetic-spectra-from-expanding-atmospheres-for-x-ray-novae-i-solar-abundances/</guid>
		<description><![CDATA[X-ray grating observations have revealed great detail in the spectra of Novae in the Super Soft Source (SSS) phase. Notable features in the SSS spectra are blue-shifted absorption lines, P-Cygni line profiles, and the absence of strong ionization edges, all of which are indicators of an expanding atmosphere.   We present, and make publicly [...]]]></description>
			<content:encoded><![CDATA[<p>X-ray grating observations have revealed great detail in the spectra of Novae in the Super Soft Source (SSS) phase. Notable features in the SSS spectra are blue-shifted absorption lines, P-Cygni line profiles, and the absence of strong ionization edges, all of which are indicators of an expanding atmosphere.   We present, and make publicly available, a set of 672 wind-type (WT) synthetic spectra, obtained from the expanding NLTE SSS models introduced in Van Rossum 2010 with the PHOENIX stellar atmosphere code. The set presented in this paper is limited to solar abundances with the aim to focus on the basic model parameters and their effect on the spectra, providing the basis upon which abundance effects can be studied using a much bigger non-solar set in the next paper in this series.   We fit the WT spectra to the five grating spectra taken in the SSS phase of nova V4743 Sgr 2003 as an example application of the WT models. Within the limits of solar abundances we demonstrate that the following parameters are constrained by the data (in order of decreasing accuracy): column density N_H, bolometric luminosity L_bol, effective temperature T_eff, white dwarf radius R, wind asymptotic velocity v_inf, and the mass-loss rate M_dot. The models are also sensitive to the assumed white dwarf mass M_wd but the effect on the spectra can largely be compensated by the other model parameters. The WT spectra with solar abundances fit the data better than abundance optimized hydro-static models.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/a-public-set-of-synthetic-spectra-from-expanding-atmospheres-for-x-ray-novae-i-solar-abundances/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Discovery of bright z ~ 7 galaxies in the UltraVISTA survey</title>
		<link>http://voxcharta.org/2012/05/21/discovery-of-bright-z-7-galaxies-in-the-ultravista-survey/</link>
		<comments>http://voxcharta.org/2012/05/21/discovery-of-bright-z-7-galaxies-in-the-ultravista-survey/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:52:49 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cfht]]></category>
		<category><![CDATA[contamination]]></category>
		<category><![CDATA[cosmos field]]></category>
		<category><![CDATA[dwarf star]]></category>
		<category><![CDATA[galaxy luminosity function]]></category>
		<category><![CDATA[hst]]></category>
		<category><![CDATA[infrared imaging]]></category>
		<category><![CDATA[luminous galaxies]]></category>
		<category><![CDATA[lyman]]></category>
		<category><![CDATA[msun]]></category>
		<category><![CDATA[number density]]></category>
		<category><![CDATA[prime target]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[redshift galaxies]]></category>
		<category><![CDATA[rest frame]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[Spitzer]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[wavelength]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/discovery-of-bright-z-7-galaxies-in-the-ultravista-survey/</guid>
		<description><![CDATA[We have exploited the new, deep, near-infrared UltraVISTA imaging of the COSMOS field, in tandem with deep optical and mid-infrared imaging, to conduct a new search for luminous galaxies at redshifts z ~ 7. The unique multi-wavelength dataset provided by VISTA, CFHT, Subaru, HST and Spitzer over a common area of 1 deg^2 has allowed [...]]]></description>
			<content:encoded><![CDATA[<p>We have exploited the new, deep, near-infrared UltraVISTA imaging of the COSMOS field, in tandem with deep optical and mid-infrared imaging, to conduct a new search for luminous galaxies at redshifts z ~ 7. The unique multi-wavelength dataset provided by VISTA, CFHT, Subaru, HST and Spitzer over a common area of 1 deg^2 has allowed us to select galaxy candidates at z &gt; 6.5 by searching first for Y+J-detected ( 6.5 which we present in this paper. The first four of these appear to be robust galaxies at z &gt; 6.5, and fitting to their stacked SED yields z = 6.98+-0.05 with a stellar mass M* = 5&#215;10^9 Msun, and rest-frame UV spectral slope beta = -2.0+-0.2. The next three are also good candidates for z &gt; 6.5 galaxies, but the possibility that they are low-redshift galaxies or dwarf stars cannot be excluded. Our final subset of three additional candidates is afflicted not only by potential dwarf-star contamination, but also contains objects likely to lie at redshifts just below z = 6.5. We show that the three even-brighter z &gt; 7 galaxy candidates reported in the COSMOS field by Capak et al. (2011) in fact all lie at z ~ 1.5-3.5. Consequently the new z ~ 7 galaxies reported here are the first credible z ~ 7 Lyman-break galaxies discovered in the COSMOS field and, as the most UV-luminous discovered to date at these redshifts, are prime targets for deep follow-up spectroscopy. We explore their physical properties, and briefly consider the implications of their inferred number density for the form of the galaxy luminosity function at z = 7.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/discovery-of-bright-z-7-galaxies-in-the-ultravista-survey/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<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>A reduction in the UHE neutrino flux due to neutrino spin precession</title>
		<link>http://voxcharta.org/2012/05/21/a-reduction-in-the-uhe-neutrino-flux-due-to-neutrino-spin-precession/</link>
		<comments>http://voxcharta.org/2012/05/21/a-reduction-in-the-uhe-neutrino-flux-due-to-neutrino-spin-precession/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:51:36 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[astrophysical objects]]></category>
		<category><![CDATA[gamma ray burst]]></category>
		<category><![CDATA[intense magnetic field]]></category>
		<category><![CDATA[magnetic moment]]></category>
		<category><![CDATA[neutrino]]></category>
		<category><![CDATA[transition]]></category>
		<category><![CDATA[uhe]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/a-reduction-in-the-uhe-neutrino-flux-due-to-neutrino-spin-precession/</guid>
		<description><![CDATA[Motivated by the stringent flux limits for UHE neutrinos coming from gamma ray burst or active galactic nuclei, we explore the possibility that the active neutrinos generated in such astrophysical objects could oscillate to sterile right handed states due to a neutrino magnetic moment mu_nu. We find that a value as small as mu_nu ~1E-15 [...]]]></description>
			<content:encoded><![CDATA[<p>Motivated by the stringent flux limits for UHE neutrinos coming from gamma ray burst or active galactic nuclei, we explore the possibility that the active neutrinos generated in such astrophysical objects could oscillate to sterile right handed states due to a neutrino magnetic moment mu_nu. We find that a value as small as mu_nu ~1E-15 mu_B could produce such a transition thanks to the intense magnetic fields that are expected in these objects.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/a-reduction-in-the-uhe-neutrino-flux-due-to-neutrino-spin-precession/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>An Oxford SWIFT Integral Field Spectroscopy study of 14 early-type galaxies in the Coma cluster</title>
		<link>http://voxcharta.org/2012/05/21/an-oxford-swift-integral-field-spectroscopy-study-of-14-early-type-galaxies-in-the-coma-cluster/</link>
		<comments>http://voxcharta.org/2012/05/21/an-oxford-swift-integral-field-spectroscopy-study-of-14-early-type-galaxies-in-the-coma-cluster/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:51:23 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorption feature]]></category>
		<category><![CDATA[band photometry]]></category>
		<category><![CDATA[cluster core]]></category>
		<category><![CDATA[coma cluster]]></category>
		<category><![CDATA[comparable studies]]></category>
		<category><![CDATA[field spectroscopy]]></category>
		<category><![CDATA[fundamental plane]]></category>
		<category><![CDATA[integral field]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[nearby universe]]></category>
		<category><![CDATA[new oxford]]></category>
		<category><![CDATA[photometric data]]></category>
		<category><![CDATA[residuals]]></category>
		<category><![CDATA[rotators]]></category>
		<category><![CDATA[selection criteria]]></category>
		<category><![CDATA[spectroscopy study]]></category>
		<category><![CDATA[triplet]]></category>
		<category><![CDATA[type galaxy]]></category>
		<category><![CDATA[velocity dispersion]]></category>
		<category><![CDATA[virgo cluster]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/an-oxford-swift-integral-field-spectroscopy-study-of-14-early-type-galaxies-in-the-coma-cluster/</guid>
		<description><![CDATA[As a demonstration of the capabilities of the new Oxford SWIFT integral field spectrograph, we present first observations for a set of 14 early-type galaxies in the core of the Coma cluster. Our data consist of I- and z-band spatially resolved spectroscopy obtained with the Oxford SWIFT spectrograph, combined with r-band photometry from the SDSS [...]]]></description>
			<content:encoded><![CDATA[<p>As a demonstration of the capabilities of the new Oxford SWIFT integral field spectrograph, we present first observations for a set of 14 early-type galaxies in the core of the Coma cluster. Our data consist of I- and z-band spatially resolved spectroscopy obtained with the Oxford SWIFT spectrograph, combined with r-band photometry from the SDSS archive for 14 early- type galaxies. We derive spatially resolved kinematics for all objects from observations of the calcium triplet absorption features at \sim 8500 {AA} . Using this kinematic information we classify galaxies as either Fast Rotators or Slow Rotators. We compare the fraction of fast and slow rotators in our sample, representing the densest environment in the nearby Universe, to results from the ATLAS3D survey, finding the slow rotator fraction is \sim 50 per cent larger in the core of the Coma cluster than in the Virgo cluster or field, a 1.2 {\sigma} increase given our selection criteria. Comparing our sample to the Virgo cluster core only (which is 24 times less dense than the Coma core) we find no evidence of an increase in the slow rotator fraction. Combining measurements of the effective velocity dispersion {\sigma_e} with the photometric data we determine the Fundamental Plane for our sample of galaxies. We find the use of the average velocity dispersion within 1 effective radius, {\sigma_e}, reduces the residuals by 13 per cent with respect to comparable studies using central velocity dispersions, consistent with other recent integral field Fundamental Plane determinations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/an-oxford-swift-integral-field-spectroscopy-study-of-14-early-type-galaxies-in-the-coma-cluster/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>Modeling the Spatial Distribution of Neutron Stars in the Galaxy</title>
		<link>http://voxcharta.org/2012/05/21/modeling-the-spatial-distribution-of-neutron-stars-in-the-galaxy/</link>
		<comments>http://voxcharta.org/2012/05/21/modeling-the-spatial-distribution-of-neutron-stars-in-the-galaxy/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:49:52 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[galactic plane]]></category>
		<category><![CDATA[gamma function]]></category>
		<category><![CDATA[gravitational potential]]></category>
		<category><![CDATA[initial distribution]]></category>
		<category><![CDATA[initial velocity]]></category>
		<category><![CDATA[monte carlo simulation]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[progenitor]]></category>
		<category><![CDATA[radial dependence]]></category>
		<category><![CDATA[radial distribution]]></category>
		<category><![CDATA[radial expansion]]></category>
		<category><![CDATA[spatial distribution]]></category>
		<category><![CDATA[stars in the galaxy]]></category>
		<category><![CDATA[toru]]></category>
		<category><![CDATA[velocities]]></category>
		<category><![CDATA[velocity distribution]]></category>
		<category><![CDATA[vertical distribution]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/modeling-the-spatial-distribution-of-neutron-stars-in-the-galaxy/</guid>
		<description><![CDATA[In this paper we investigate the space and velocity distributions of old neutron stars (aged 109 to 1010 yr) in our Galaxy. Galactic old Neutron Stars (NSs) population fills a torus-like area extending to a few tens kiloparsecs above the galactic plane. The initial velocity distribution of NSs is not well known, in this work [...]]]></description>
			<content:encoded><![CDATA[<p>In this paper we investigate the space and velocity distributions of old neutron stars (aged 109 to 1010 yr) in our Galaxy. Galactic old Neutron Stars (NSs) population fills a torus-like area extending to a few tens kiloparsecs above the galactic plane. The initial velocity distribution of NSs is not well known, in this work we adopt a three component initial distribution, as given by the contribution of kick velocities, circular velocities and Maxwellian velocities. For the spatial initial distribution we use a Gamma function. We then use Monte Carlo simulations to follow the evolution of the NSs under the influence of the Paczy{\P}nski Galactic gravitational potential. Our calculations show that NS orbits have a very large Galactic radial expansion and that their radial distribution peak is quite close to their progenitors&#8217; one. We also study the NS vertical distribution and find that it can well be described by a double exponential low. Finally, we investigate the correlation of the vertical and radial distribution and study the radial dependence of scale-heights.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/modeling-the-spatial-distribution-of-neutron-stars-in-the-galaxy/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Systematic differences in simple stellar population model results: Application to the M31 globular-like cluster system</title>
		<link>http://voxcharta.org/2012/05/21/systematic-differences-in-simple-stellar-population-model-results-application-to-the-m31-globular-like-cluster-system/</link>
		<comments>http://voxcharta.org/2012/05/21/systematic-differences-in-simple-stellar-population-model-results-application-to-the-m31-globular-like-cluster-system/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:49:34 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[chabrier]]></category>
		<category><![CDATA[charlot]]></category>
		<category><![CDATA[cluster system]]></category>
		<category><![CDATA[environmental conditions]]></category>
		<category><![CDATA[external galaxy]]></category>
		<category><![CDATA[globular cluster]]></category>
		<category><![CDATA[initial mass function]]></category>
		<category><![CDATA[metallicity]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[minimisation]]></category>
		<category><![CDATA[model result]]></category>
		<category><![CDATA[plethora]]></category>
		<category><![CDATA[population model]]></category>
		<category><![CDATA[spectral energy distribution]]></category>
		<category><![CDATA[star cluster]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[systematic differences]]></category>
		<category><![CDATA[useful tools]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/systematic-differences-in-simple-stellar-population-model-results-application-to-the-m31-globular-like-cluster-system/</guid>
		<description><![CDATA[Simple stellar population (SSP) synthesis models are useful tools for studying the nature of unresolved star clusters in external galaxies. However, the plethora of currently available SSP models gives rise to significant and poorly documented systematic differences. Here we consider the outputs of the commonly used Bruzual &#38; Charlot and GALEV models, as well as [...]]]></description>
			<content:encoded><![CDATA[<p>Simple stellar population (SSP) synthesis models are useful tools for studying the nature of unresolved star clusters in external galaxies. However, the plethora of currently available SSP models gives rise to significant and poorly documented systematic differences. Here we consider the outputs of the commonly used Bruzual &amp; Charlot and GALEV models, as well as a recently updated SSP model suite which attempts to include the contributions of binary merger products in the form of blue straggler stars (BS-SSP). We rederive the ages, metallicities, extinction values and masses of 445 previously observed globular-like clusters in M31 based on chi-square minimisation of their spectral energy distributions with respect to these three different SSP models and adopting a Chabrier-like stellar initial mass function. A comparison between our new results and previous estimates of the same parameters shows that the Bruzual &amp; Charlot models yield the youngest ages and lowest masses, while adoption of the BS-SSP models results in the oldest ages and highest mass estimates. Similarly, the GALEV SSP models produce the lowest metallicities, with the highest values resulting from the BS-SSP model suite. These trends are caused by intrinsic differences associated with the models, and are not significantly affected by the well-known age-metallicity degeneracy. Finally, we note that the mass function of the massive M31 star clusters is similar to that of the Milky Way&#8217;s globular clusters, which implies that the two star cluster systems likely formed under similar environmental conditions.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/systematic-differences-in-simple-stellar-population-model-results-application-to-the-m31-globular-like-cluster-system/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>AE Aquarii represents a new subclass of Cataclysmic Variables</title>
		<link>http://voxcharta.org/2012/05/21/ae-aquarii-represents-a-new-subclass-of-cataclysmic-variables/</link>
		<comments>http://voxcharta.org/2012/05/21/ae-aquarii-represents-a-new-subclass-of-cataclysmic-variables/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:49:20 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[aqr]]></category>
		<category><![CDATA[binary system]]></category>
		<category><![CDATA[cataclysmic variables]]></category>
		<category><![CDATA[diffusion]]></category>
		<category><![CDATA[dwarf surface]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[intermediate polars]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetic moment]]></category>
		<category><![CDATA[mass exchange]]></category>
		<category><![CDATA[missing link]]></category>
		<category><![CDATA[plasma]]></category>
		<category><![CDATA[red dwarf]]></category>
		<category><![CDATA[subclass]]></category>
		<category><![CDATA[system component]]></category>
		<category><![CDATA[transition]]></category>
		<category><![CDATA[white dwarf]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/ae-aquarii-represents-a-new-subclass-of-cataclysmic-variables/</guid>
		<description><![CDATA[We analyze properties of the unique nova-like star AE Aquarii identified with a close binary system containing a red dwarf and a very fast rotating magnetized white dwarf. It cannot be assigned to any of the three commonly adopted sub-classes of Cataclysmic Variables: Polars, Intermediate Polars, and Accreting non-magnetized White Dwarfs. Our study has shown [...]]]></description>
			<content:encoded><![CDATA[<p>We analyze properties of the unique nova-like star AE Aquarii identified with a close binary system containing a red dwarf and a very fast rotating magnetized white dwarf. It cannot be assigned to any of the three commonly adopted sub-classes of Cataclysmic Variables: Polars, Intermediate Polars, and Accreting non-magnetized White Dwarfs. Our study has shown that the white dwarf in AE Aqr is in the ejector state and its dipole magnetic moment is $\mu ~ 1.5 \times 10^{34} G cm^3$. It switched into this state due to intensive mass exchange between the system components during a previous epoch. A high rate of disk accretion onto the white dwarf surface resulted in temporary screening of its magnetic field and spin-up of the white dwarf to its present spin period. Transition of the white dwarf to the ejector state had occurred at a final stage of the spin-up epoch as its magnetic field emerged from the accreted plasma due to diffusion. In the frame of this scenario AE Aqr represents a missing link in the chain of Polars evolution and the white dwarf resembles a recycled pulsar.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/ae-aquarii-represents-a-new-subclass-of-cataclysmic-variables/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Collisional Penrose process near the horizon of extreme Kerr black holes</title>
		<link>http://voxcharta.org/2012/05/21/collisional-penrose-process-near-the-horizon-of-extreme-kerr-black-holes/</link>
		<comments>http://voxcharta.org/2012/05/21/collisional-penrose-process-near-the-horizon-of-extreme-kerr-black-holes/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:49:03 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[center of mass]]></category>
		<category><![CDATA[collisional]]></category>
		<category><![CDATA[collisions]]></category>
		<category><![CDATA[cosmic accelerators]]></category>
		<category><![CDATA[energetic particle]]></category>
		<category><![CDATA[horizon]]></category>
		<category><![CDATA[infinity]]></category>
		<category><![CDATA[initial energy]]></category>
		<category><![CDATA[kerr]]></category>
		<category><![CDATA[mass energy]]></category>
		<category><![CDATA[particle accelerator]]></category>
		<category><![CDATA[penrose]]></category>
		<category><![CDATA[rotational energy]]></category>
		<category><![CDATA[suggestion]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/collisional-penrose-process-near-the-horizon-of-extreme-kerr-black-holes/</guid>
		<description><![CDATA[Collisions of particles in black holes&#8217; ergospheres may result in an arbitrarily large center of mass energy. This led recently to the suggestion (Banados et al., 2009) that black holes can act as ultimate particle accelerators. If the energy of an outgoing particle is larger than the total energy of the infalling particles the energy [...]]]></description>
			<content:encoded><![CDATA[<p>Collisions of particles in black holes&#8217; ergospheres may result in an arbitrarily large center of mass energy. This led recently to the suggestion (Banados et al., 2009) that black holes can act as ultimate particle accelerators. If the energy of an outgoing particle is larger than the total energy of the infalling particles the energy excess must come from the rotational energy of the black hole and hence this must involve a Penrose process. However, while the center of mass energy diverges the position of the collision makes it impossible for energetic particles to escape to infinity. Following an earlier work on collisional Penrose processes (Piran &amp; Shaham 1977) we show that even under the most favorable idealized conditions the maximal energy of an escaping particle is only a modest factor above the total initial energy of the colliding particles. This implies that one shouldn&#8217;t expect collisions around a black hole to act as spectacular cosmic accelerators.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/collisional-penrose-process-near-the-horizon-of-extreme-kerr-black-holes/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Spectral Analysis of the 13 keV Feature in XTE J1810-197: Implications for AXP Models</title>
		<link>http://voxcharta.org/2012/05/21/spectral-analysis-of-the-13-kev-feature-in-xte-j1810-197-implications-for-axp-models/</link>
		<comments>http://voxcharta.org/2012/05/21/spectral-analysis-of-the-13-kev-feature-in-xte-j1810-197-implications-for-axp-models/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:48:50 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[atmosphere]]></category>
		<category><![CDATA[atomic emission]]></category>
		<category><![CDATA[axp]]></category>
		<category><![CDATA[coincidence]]></category>
		<category><![CDATA[compact object]]></category>
		<category><![CDATA[disk model]]></category>
		<category><![CDATA[emission processes]]></category>
		<category><![CDATA[fall back]]></category>
		<category><![CDATA[keV]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[quark]]></category>
		<category><![CDATA[rubidium]]></category>
		<category><![CDATA[spectral analysis]]></category>
		<category><![CDATA[spectrum]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/spectral-analysis-of-the-13-kev-feature-in-xte-j1810-197-implications-for-axp-models/</guid>
		<description><![CDATA[During 2003 and 2004 the Anomalous X-Ray Pulsar XTE J1810-197 went through a series of four bursts. The spectrum in the tail of one of these bursts shows a strong, significant emission feature ~13 keV, thereby encoding a wealth of information about the environment surrounding this object. In this paper we analyse this emission feature [...]]]></description>
			<content:encoded><![CDATA[<p>During 2003 and 2004 the Anomalous X-Ray Pulsar XTE J1810-197 went through a series of four bursts. The spectrum in the tail of one of these bursts shows a strong, significant emission feature ~13 keV, thereby encoding a wealth of information about the environment surrounding this object. In this paper we analyse this emission feature considering both cyclotron and atomic emission processes and weigh our findings against three leading AXP models: the Magnetar model, Fall-back disk model and the Quark nova model. We find that atomic emission from Rubidium within a Keplerian ring ($\sim$15 km from a compact object of $\sim 2M_\odot$) is the most consistent scenario with the observations, supporting the Quark nova model. Cyclotron emission from an atmosphere a few hundred meters thick also fits the feature well, but is ruled out on account of its positional coincidence in three separate AXP sources.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/spectral-analysis-of-the-13-kev-feature-in-xte-j1810-197-implications-for-axp-models/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Monster black holes</title>
		<link>http://voxcharta.org/2012/05/21/monster-black-holes/</link>
		<comments>http://voxcharta.org/2012/05/21/monster-black-holes/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:48:37 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[monster]]></category>
		<category><![CDATA[monsters co]]></category>
		<category><![CDATA[nearby universe]]></category>
		<category><![CDATA[solar mass]]></category>
		<category><![CDATA[spacecraft observations]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/monster-black-holes/</guid>
		<description><![CDATA[A combination of ground-based and spacecraft observations has uncovered two black holes of 10 billion solar masses in the nearby Universe. The finding sheds light on how these cosmic monsters co-evolve with galaxies.
]]></description>
			<content:encoded><![CDATA[<p>A combination of ground-based and spacecraft observations has uncovered two black holes of 10 billion solar masses in the nearby Universe. The finding sheds light on how these cosmic monsters co-evolve with galaxies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/monster-black-holes/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Contributions to the cross shock electric field at supercritical perpendicular shocks: Impact of the pickup ions [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/21/contributions-to-the-cross-shock-electric-field-at-supercritical-perpendicular-shocks-impact-of-the-pickup-ions-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/21/contributions-to-the-cross-shock-electric-field-at-supercritical-perpendicular-shocks-impact-of-the-pickup-ions-cross-listing/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:48:23 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[gyro]]></category>
		<category><![CDATA[ion dynamics]]></category>
		<category><![CDATA[lorentz]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[pickup ions]]></category>
		<category><![CDATA[pis]]></category>
		<category><![CDATA[preliminary results]]></category>
		<category><![CDATA[ramp]]></category>
		<category><![CDATA[reformation]]></category>
		<category><![CDATA[shock]]></category>
		<category><![CDATA[shock front]]></category>
		<category><![CDATA[solar wind ions]]></category>
		<category><![CDATA[stationary foot]]></category>
		<category><![CDATA[striking point]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/contributions-to-the-cross-shock-electric-field-at-supercritical-perpendicular-shocks-impact-of-the-pickup-ions-cross-listing/</guid>
		<description><![CDATA[A particle-in-cell code is used to examine contributions of the pickup ions (PIs) and the solar wind ions (SWs) to the cross shock electric field at the supercritical, perpendicular shocks. The code treats the pickup ions self-consistently as a third component. Herein, two different runs with relative pickup ion density of 25% and 55% are [...]]]></description>
			<content:encoded><![CDATA[<p>A particle-in-cell code is used to examine contributions of the pickup ions (PIs) and the solar wind ions (SWs) to the cross shock electric field at the supercritical, perpendicular shocks. The code treats the pickup ions self-consistently as a third component. Herein, two different runs with relative pickup ion density of 25% and 55% are presented in this paper. Present preliminary results show that: (1) in the low percentage (25%) pickup ion case, the shock front is nonstationary. During the evolution of this perpendicular shock, a nonstationary foot resulting from the reflected solar wind ions is formed in front of the old ramp, and its amplitude becomes larger and larger. At last, the nonstationary foot grows up into a new ramp and exceeds the old one. Such a nonstationary process can be formed periodically. hen the new ramp begins to be formed in front of the old ramp, the Hall term mainly contributed by the solar wind ions becomes more and more important. The electric field Ex is dominated by the Hall term when the new ramp exceeds the old one. Furthermore, an extended and stationary foot in pickup ion gyro-scale is located upstream of the nonstationary/self-reforming region within the shock front, and is always dominated by the Lorentz term contributed by the pickup ions; (2) in the high percentage (55%) pickup ion case, the amplitude of the stationary foot is increased as expected. One striking point is that the nonstationary region of the shock front evidenced by the self-reformation disappears. Instead, a stationary extended foot dominated by Lorentz term contributed by the pickup ions, and a tationary ramp dominated by Hall term contributed by the solar wind ions are clearly evidenced. The significance of the cross electric field on ion dynamics is also discussed.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/contributions-to-the-cross-shock-electric-field-at-supercritical-perpendicular-shocks-impact-of-the-pickup-ions-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Energy-dependent orbital modulation of X-rays and a constraint on emission of the jet in Cyg X-3</title>
		<link>http://voxcharta.org/2012/05/21/energy-dependent-orbital-modulation-of-x-rays-and-a-constraint-on-emission-of-the-jet-in-cyg-x-3/</link>
		<comments>http://voxcharta.org/2012/05/21/energy-dependent-orbital-modulation-of-x-rays-and-a-constraint-on-emission-of-the-jet-in-cyg-x-3/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:48:09 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorption]]></category>
		<category><![CDATA[compton]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[continuum]]></category>
		<category><![CDATA[cyg]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[increasing energy]]></category>
		<category><![CDATA[inferior conjunction]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[modulation depth]]></category>
		<category><![CDATA[optical depth]]></category>
		<category><![CDATA[shape]]></category>
		<category><![CDATA[soft x]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectral states]]></category>
		<category><![CDATA[stellar wind]]></category>
		<category><![CDATA[superior conjunction]]></category>
		<category><![CDATA[unprecedented accuracy]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/energy-dependent-orbital-modulation-of-x-rays-and-a-constraint-on-emission-of-the-jet-in-cyg-x-3/</guid>
		<description><![CDATA[We study orbital modulation of X-rays from Cyg X-3, using data from Swift, INTEGRAL and RXTE. Given the wealth of the presently available data and an improved calculation method, we obtain energy-dependent folded and averaged light curves with unprecedented accuracy. We find that above ~5 keV, the modulation depth decreases with the increasing energy, which [...]]]></description>
			<content:encoded><![CDATA[<p>We study orbital modulation of X-rays from Cyg X-3, using data from Swift, INTEGRAL and RXTE. Given the wealth of the presently available data and an improved calculation method, we obtain energy-dependent folded and averaged light curves with unprecedented accuracy. We find that above ~5 keV, the modulation depth decreases with the increasing energy, which is consistent with the modulation being caused by both bound-free absorption and Compton scattering in the stellar wind of the donor, with minima corresponding to the highest optical depth, which occurs around the superior conjunction. We find a decrease of the depth below ~3 keV, which appears to be due to re-emission of the absorbed continuum by the wind in soft X-ray lines. Based on the shape of the folded light curves, any X-ray contribution from the jet in Cyg X-3, which emits gamma-rays detected at energies $&gt;0.1$ GeV in soft spectral states, is found to be minor up to ~100 keV. We also calculate phase-resolved RXTE X-ray spectra, and show the difference between the spectra corresponding to phases around the superior and inferior conjunctions can indeed be accounted for by a combined effect of bound-free absorption in an ionized medium and Compton scattering.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/energy-dependent-orbital-modulation-of-x-rays-and-a-constraint-on-emission-of-the-jet-in-cyg-x-3/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Towards p-Adic Matter in the Universe [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/21/towards-p-adic-matter-in-the-universe-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/21/towards-p-adic-matter-in-the-universe-cross-listing/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:47:58 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[adic]]></category>
		<category><![CDATA[energy term]]></category>
		<category><![CDATA[evolution of the universe]]></category>
		<category><![CDATA[field solution]]></category>
		<category><![CDATA[kinetic energy]]></category>
		<category><![CDATA[lagrangian]]></category>
		<category><![CDATA[non locality]]></category>
		<category><![CDATA[scalar field]]></category>
		<category><![CDATA[space time]]></category>
		<category><![CDATA[string theory]]></category>
		<category><![CDATA[string world]]></category>
		<category><![CDATA[time dimension]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/towards-p-adic-matter-in-the-universe-cross-listing/</guid>
		<description><![CDATA[Starting from p-adic string theory with tachyons, we introduce a new kind of non-tachyonic matter which may play an important role in evolution of the Universe. This matter retains nonlocal and nonlinear p-adic string dynamics, but does not suffer of negative square mass. In space-time dimensions D = 2 + 4k, what includes D = [...]]]></description>
			<content:encoded><![CDATA[<p>Starting from p-adic string theory with tachyons, we introduce a new kind of non-tachyonic matter which may play an important role in evolution of the Universe. This matter retains nonlocal and nonlinear p-adic string dynamics, but does not suffer of negative square mass. In space-time dimensions D = 2 + 4k, what includes D = 6, 10, &#8230;, 26, the kinetic energy term also maintains correct sign. In these spaces this p-adic matter provides negative cosmological constant and time-dependent scalar field solution with negative potential. Their possible cosmological role is discussed. We have also connected non-locality with string world-sheet in effective Lagrangian for p-adic string.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/towards-p-adic-matter-in-the-universe-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>On energetics of particle collisions near black holes: BSW effect versus Penrose process [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/21/on-energetics-of-particle-collisions-near-black-holes-bsw-effect-versus-penrose-process-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/21/on-energetics-of-particle-collisions-near-black-holes-bsw-effect-versus-penrose-process-cross-listing/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:47:48 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[centre of mass]]></category>
		<category><![CDATA[dependence]]></category>
		<category><![CDATA[distant observer]]></category>
		<category><![CDATA[energetics]]></category>
		<category><![CDATA[energy particle]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[horizon]]></category>
		<category><![CDATA[mass frame]]></category>
		<category><![CDATA[particle collision]]></category>
		<category><![CDATA[penrose]]></category>
		<category><![CDATA[upper bound]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/on-energetics-of-particle-collisions-near-black-holes-bsw-effect-versus-penrose-process-cross-listing/</guid>
		<description><![CDATA[If two particles collide near the horizon of a rotating or charged black hole, under certain conditions the energy E_{c.m.} in the centre of mass frame can grow without limit (the so-called BSW effect). Let collision produce two another particles. We show that for an outgoing particle detected by a distant observer, there exist upper [...]]]></description>
			<content:encoded><![CDATA[<p>If two particles collide near the horizon of a rotating or charged black hole, under certain conditions the energy E_{c.m.} in the centre of mass frame can grow without limit (the so-called BSW effect). Let collision produce two another particles. We show that for an outgoing particle detected by a distant observer, there exist upper bounds on the mass and energy E_{out}. For a static charged black hole, the dependence of E_{out} on the energy E_{in} of an ingoing &#8220;critical&#8221; particle (responsible for the BSW effect) is decreasing. For neutral rotating black holes it is increasing but for the high-energy particles the ratio E_{out}/E_{in}&lt;1. As a result, the BSW effect is inconsistent with the Penrose process. The obtained results suggest astrophysical limits on possibility of observation of the products of the BSW effect. From the other hand, collisions with finite E_{c.m.} can produce particles with unbound ratio E_{out}/E_{in}.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/on-energetics-of-particle-collisions-near-black-holes-bsw-effect-versus-penrose-process-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Infrared observations of the recurrent nova T Pyxidis: ancient dust basks in the warm glow of the 2011 outburst</title>
		<link>http://voxcharta.org/2012/05/21/infrared-observations-of-the-recurrent-nova-t-pyxidis-ancient-dust-basks-in-the-warm-glow-of-the-2011-outburst/</link>
		<comments>http://voxcharta.org/2012/05/21/infrared-observations-of-the-recurrent-nova-t-pyxidis-ancient-dust-basks-in-the-warm-glow-of-the-2011-outburst/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:47:20 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accumulation]]></category>
		<category><![CDATA[herschel]]></category>
		<category><![CDATA[infrared observation]]></category>
		<category><![CDATA[infrared photometry]]></category>
		<category><![CDATA[interstellar dust]]></category>
		<category><![CDATA[nebulosity]]></category>
		<category><![CDATA[outburst]]></category>
		<category><![CDATA[pyx]]></category>
		<category><![CDATA[recurrent nova]]></category>
		<category><![CDATA[space observatory]]></category>
		<category><![CDATA[space telescope]]></category>
		<category><![CDATA[warm glow]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/infrared-observations-of-the-recurrent-nova-t-pyxidis-ancient-dust-basks-in-the-warm-glow-of-the-2011-outburst/</guid>
		<description><![CDATA[We present Spitzer Space Telescope and Herschel Space Observatory infrared observations of the recurrent nova T Pyx during its 2011 eruption, complemented by ground-base optical-infrared photometry. We find that the eruption has heated dust in the pre-existing nebulosity associated with T Pyx. This is most likely interstellar dust swept up by T Pyx &#8211; either [...]]]></description>
			<content:encoded><![CDATA[<p>We present Spitzer Space Telescope and Herschel Space Observatory infrared observations of the recurrent nova T Pyx during its 2011 eruption, complemented by ground-base optical-infrared photometry. We find that the eruption has heated dust in the pre-existing nebulosity associated with T Pyx. This is most likely interstellar dust swept up by T Pyx &#8211; either during previous eruptions or by a wind &#8211; rather than the accumulation of dust produced during eruptions.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/infrared-observations-of-the-recurrent-nova-t-pyxidis-ancient-dust-basks-in-the-warm-glow-of-the-2011-outburst/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Nitrogen line spectroscopy in O-stars &#8212; III. The earliest O-stars</title>
		<link>http://voxcharta.org/2012/05/21/nitrogen-line-spectroscopy-in-o-stars-iii-the-earliest-o-stars/</link>
		<comments>http://voxcharta.org/2012/05/21/nitrogen-line-spectroscopy-in-o-stars-iii-the-earliest-o-stars/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:46:24 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[classification scheme]]></category>
		<category><![CDATA[dwarf]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[line profile]]></category>
		<category><![CDATA[line ratio]]></category>
		<category><![CDATA[lmc]]></category>
		<category><![CDATA[low wind]]></category>
		<category><![CDATA[luminosity class]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[model prediction]]></category>
		<category><![CDATA[nitrogen content]]></category>
		<category><![CDATA[o star]]></category>
		<category><![CDATA[spectral type]]></category>
		<category><![CDATA[supergiant]]></category>
		<category><![CDATA[synthetic spectra]]></category>
		<category><![CDATA[theoretical prediction]]></category>
		<category><![CDATA[type star]]></category>
		<category><![CDATA[wind parameters]]></category>
		<category><![CDATA[wind strength]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/nitrogen-line-spectroscopy-in-o-stars-iii-the-earliest-o-stars/</guid>
		<description><![CDATA[This is the third paper in a series aiming at the analysis of nitrogen abundances in O-type stars, to enable further constraints on the early evolution of massive stars. We provide first theoretical predictions for the NIV4058/NIII4640 emission line ratio in dependence of various parameters, and confront them with results from the analysis of a [...]]]></description>
			<content:encoded><![CDATA[<p>This is the third paper in a series aiming at the analysis of nitrogen abundances in O-type stars, to enable further constraints on the early evolution of massive stars. We provide first theoretical predictions for the NIV4058/NIII4640 emission line ratio in dependence of various parameters, and confront them with results from the analysis of a sample of early LMC/SMC O-stars. Stellar and wind parameters are determined by line profile fitting of H/He/N lines, exploiting the helium and nitrogen ionization balance. Corresponding synthetic spectra are calculated using the NLTE atmospheric code FASTWIND. Though there is a monotonic relationship between the emission line ratio and Teff, all other parameters being equal, theoretical predictions indicate additional dependencies, most notably, on the nitrogen abundance. These basic predictions are confirmed by results from atmospheric code CMFGEN. The effective temperatures for the earliest O-stars, inferred from the nitrogen ionization balance, are partly considerably hotter than indicated by previous studies. Consistent with earlier results, effective temperatures increase from supergiants to dwarfs for all spectral types in the LMC. The relation between observed NIV4058/NIII4640 emission line ratio and Teff, for a given luminosity class, turned out to be quite monotonic for our sample stars, and fairly consistent with our model predictions. The scatter within a spectral sub-type is mainly produced by abundance effects. Our findings suggest that the Walborn et al. (2002) classification scheme is able to provide a meaningful relation between spectral type and Teff, provided that it is possible to discriminate for the luminosity class. This might be difficult to achieve in low-Z environments such as the SMC, owing to rather low wind-strengths. According to our predictions, the major bias of the classification scheme is due to nitrogen content.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/nitrogen-line-spectroscopy-in-o-stars-iii-the-earliest-o-stars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Data analysis recipes: Probability calculus for inference [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/21/data-analysis-recipes-probability-calculus-for-inference-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/21/data-analysis-recipes-probability-calculus-for-inference-cross-listing/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:46:12 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[applications of probability]]></category>
		<category><![CDATA[dimensional analysis]]></category>
		<category><![CDATA[marginalized]]></category>
		<category><![CDATA[probabilistic inference]]></category>
		<category><![CDATA[probability]]></category>
		<category><![CDATA[probability calculus]]></category>
		<category><![CDATA[probability distribution function]]></category>
		<category><![CDATA[recipes]]></category>
		<category><![CDATA[valuable tool]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/data-analysis-recipes-probability-calculus-for-inference-cross-listing/</guid>
		<description><![CDATA[In this pedagogical text aimed at those wanting to start thinking about or brush up on probabilistic inference, I review the rules by which probability distribution functions can (and cannot) be combined. I connect these rules to the operations performed in probabilistic data analysis. Dimensional analysis is emphasized as a valuable tool for helping to [...]]]></description>
			<content:encoded><![CDATA[<p>In this pedagogical text aimed at those wanting to start thinking about or brush up on probabilistic inference, I review the rules by which probability distribution functions can (and cannot) be combined. I connect these rules to the operations performed in probabilistic data analysis. Dimensional analysis is emphasized as a valuable tool for helping to construct non-wrong probabilistic statements. The applications of probability calculus in constructing likelihoods, marginalized likelihoods, posterior probabilities, and posterior predictions are all discussed.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/data-analysis-recipes-probability-calculus-for-inference-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Baroclinic Instability on Hot Extrasolar Planets</title>
		<link>http://voxcharta.org/2012/05/21/baroclinic-instability-on-hot-extrasolar-planets/</link>
		<comments>http://voxcharta.org/2012/05/21/baroclinic-instability-on-hot-extrasolar-planets/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:45:55 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[artificial viscosity]]></category>
		<category><![CDATA[circulation model]]></category>
		<category><![CDATA[circulation studies]]></category>
		<category><![CDATA[curvature]]></category>
		<category><![CDATA[cyclones and anticyclones]]></category>
		<category><![CDATA[equator]]></category>
		<category><![CDATA[extrasolar giant planet]]></category>
		<category><![CDATA[extrasolar planet]]></category>
		<category><![CDATA[flank]]></category>
		<category><![CDATA[gcm simulations]]></category>
		<category><![CDATA[initial value]]></category>
		<category><![CDATA[linear analysis]]></category>
		<category><![CDATA[mode analysis]]></category>
		<category><![CDATA[primitive equations]]></category>
		<category><![CDATA[rotation]]></category>
		<category><![CDATA[scale variability]]></category>
		<category><![CDATA[timescale]]></category>
		<category><![CDATA[unstable mode]]></category>
		<category><![CDATA[value calculations]]></category>
		<category><![CDATA[weather systems]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/baroclinic-instability-on-hot-extrasolar-planets/</guid>
		<description><![CDATA[We investigate baroclinic instability in flow conditions relevant to hot extrasolar planets. The instability is important for transporting and mixing heat, as well as for influencing large-scale variability on the planets. Both linear normal mode analysis and non-linear initial value calculations are carried out &#8212; focusing on the freely-evolving, adiabatic situation. Using a high-resolution general [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate baroclinic instability in flow conditions relevant to hot extrasolar planets. The instability is important for transporting and mixing heat, as well as for influencing large-scale variability on the planets. Both linear normal mode analysis and non-linear initial value calculations are carried out &#8212; focusing on the freely-evolving, adiabatic situation. Using a high-resolution general circulation model (GCM) which solves the traditional primitive equations, we show that large-scale jets similar to those observed in current GCM simulations of hot extrasolar giant planets are likely to be baroclinically unstable on a timescale of few to few tens of planetary rotations, generating cyclones and anticyclones that drive weather systems. The growth rate and scale of the most unstable mode obtained in the linear analysis are in qualitative, good agreement with the full non-linear calculations. In general, unstable jets evolve differently depending on their signs (eastward or westward), due to the change in sign of the jet curvature. For jets located at or near the equator, instability is strong at the flanks &#8212; but not at the core. Crucially, the instability is either poorly or not at all captured in simulations with low resolution and/or high artificial viscosity. Hence, the instability has not been observed or emphasized in past circulation studies of hot extrasolar planets.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/baroclinic-instability-on-hot-extrasolar-planets/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>CfA4: Light Curves for 94 Type Ia Supernovae</title>
		<link>http://voxcharta.org/2012/05/21/cfa4-light-curves-for-94-type-ia-supernovae/</link>
		<comments>http://voxcharta.org/2012/05/21/cfa4-light-curves-for-94-type-ia-supernovae/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:45:42 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accuracy level]]></category>
		<category><![CDATA[bvr]]></category>
		<category><![CDATA[comparison star]]></category>
		<category><![CDATA[cramer]]></category>
		<category><![CDATA[curve points]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[departures]]></category>
		<category><![CDATA[energy error]]></category>
		<category><![CDATA[error budget]]></category>
		<category><![CDATA[hubble flow]]></category>
		<category><![CDATA[light curve]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[optical path]]></category>
		<category><![CDATA[optical photometry]]></category>
		<category><![CDATA[redshift range]]></category>
		<category><![CDATA[sn ia]]></category>
		<category><![CDATA[statistical sampling error]]></category>
		<category><![CDATA[systematic error]]></category>
		<category><![CDATA[systematic uncertainty]]></category>
		<category><![CDATA[wavelength]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/cfa4-light-curves-for-94-type-ia-supernovae/</guid>
		<description><![CDATA[We present multi-band optical photometry of 94 spectroscopically-confirmed Type Ia supernovae (SN Ia) in the redshift range 0.0055 to 0.073, obtained between 2006 and 2011. There are a total of 5522 light curve points. We show that our natural system SN photometry has a precision of roughly 0.03 mag or better in BVr&#8217;i', 0.06 mag [...]]]></description>
			<content:encoded><![CDATA[<p>We present multi-band optical photometry of 94 spectroscopically-confirmed Type Ia supernovae (SN Ia) in the redshift range 0.0055 to 0.073, obtained between 2006 and 2011. There are a total of 5522 light curve points. We show that our natural system SN photometry has a precision of roughly 0.03 mag or better in BVr&#8217;i', 0.06 mag in u&#8217;, and 0.07 mag in U for points brighter than 17.5 mag and estimate that it has a systematic uncertainty of 0.014, 0.010, 0.012, 0.014, 0.046, and 0.073 mag in BVr&#8217;i'u&#8217;U, respectively. Comparisons of our standard system photometry with published SN Ia light curves and comparison stars reveal mean agreement across samples in the range of ~0.00-0.03 mag. We discuss the recent measurements of our telescope-plus-detector throughput by direct monochromatic illumination by Cramer et al (in prep.). This technique measures the whole optical path through the telescope, auxiliary optics, filters, and detector under the same conditions used to make SN measurements. Extremely well-characterized natural-system passbands (both in wavelength and over time) are crucial for the next generation of SN Ia photometry to reach the 0.01 mag accuracy level. The current sample of low-z SN Ia is now sufficiently large to remove most of the statistical sampling error from the dark energy error budget. But pursuing the dark-energy systematic errors by determining highly-accurate detector passbands, combining optical and near-infrared (NIR) photometry and spectra, using the nearby sample to illuminate the population properties of SN Ia, and measuring the local departures from the Hubble flow will benefit from larger, carefully measured nearby samples.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/cfa4-light-curves-for-94-type-ia-supernovae/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<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>
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		<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>The Durham adaptive optics real-time controller: Capability and ELT suitability</title>
		<link>http://voxcharta.org/2012/05/21/the-durham-adaptive-optics-real-time-controller-capability-and-elt-suitability/</link>
		<comments>http://voxcharta.org/2012/05/21/the-durham-adaptive-optics-real-time-controller-capability-and-elt-suitability/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:44:41 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[adaptive optics system]]></category>
		<category><![CDATA[astronomical adaptive optics]]></category>
		<category><![CDATA[capability]]></category>
		<category><![CDATA[hardware implementation]]></category>
		<category><![CDATA[high performance]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[new feature]]></category>
		<category><![CDATA[performance improvement]]></category>
		<category><![CDATA[real time control]]></category>
		<category><![CDATA[suitability]]></category>
		<category><![CDATA[Telescope]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/the-durham-adaptive-optics-real-time-controller-capability-and-elt-suitability/</guid>
		<description><![CDATA[The Durham adaptive optics real-time controller is a generic, high performance real-time control system for astronomical adaptive optics systems. It has recently had new features added as well as performance improvements, and here we give details of these, as well as ways in which optimisations can be made for specific adaptive optics systems and hardware [...]]]></description>
			<content:encoded><![CDATA[<p>The Durham adaptive optics real-time controller is a generic, high performance real-time control system for astronomical adaptive optics systems. It has recently had new features added as well as performance improvements, and here we give details of these, as well as ways in which optimisations can be made for specific adaptive optics systems and hardware implementations. We also present new measurements that show how this real-time control system could be used with any existing adaptive optics system, and also show that when used with modern hardware, it has high enough performance to be used with most Extremely Large Telescope adaptive optics systems.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/the-durham-adaptive-optics-real-time-controller-capability-and-elt-suitability/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Sunspot rotation, filament, and flare: The event on 2000 February 10</title>
		<link>http://voxcharta.org/2012/05/21/sunspot-rotation-filament-and-flare-the-event-on-2000-february-10/</link>
		<comments>http://voxcharta.org/2012/05/21/sunspot-rotation-filament-and-flare-the-event-on-2000-february-10/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:44:28 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[c class]]></category>
		<category><![CDATA[chromosphere]]></category>
		<category><![CDATA[class flare]]></category>
		<category><![CDATA[corona]]></category>
		<category><![CDATA[filament channel]]></category>
		<category><![CDATA[filament eruption]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[magnetic flux]]></category>
		<category><![CDATA[mass ejection]]></category>
		<category><![CDATA[photosphere]]></category>
		<category><![CDATA[polarity]]></category>
		<category><![CDATA[rapid increase]]></category>
		<category><![CDATA[region ar]]></category>
		<category><![CDATA[rotation rate]]></category>
		<category><![CDATA[sunspot]]></category>
		<category><![CDATA[twenty four hours]]></category>
		<category><![CDATA[umbrae]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/sunspot-rotation-filament-and-flare-the-event-on-2000-february-10/</guid>
		<description><![CDATA[We find that a sunspot with positive polarity had an obvious counter-clockwise rotation and resulted in the formation and eruption of an inverse S-shaped filament in NOAA active region (AR) 08858 from 2000 February 9 to 10. The sunspot had two umbrae which rotated around each other by 195 degrees within about twenty-four hours. The [...]]]></description>
			<content:encoded><![CDATA[<p>We find that a sunspot with positive polarity had an obvious counter-clockwise rotation and resulted in the formation and eruption of an inverse S-shaped filament in NOAA active region (AR) 08858 from 2000 February 9 to 10. The sunspot had two umbrae which rotated around each other by 195 degrees within about twenty-four hours. The average rotation rate was nearly 8 degrees per hour. The fastest rotation in the photosphere took place during 14:00UT to 22:01UT on February 9, with the rotation rate of nearly 16 degrees per hour. The fastest rotation in the chromosphere and the corona took place during 15:28UT to 19:00UT on February 9, with the rotation rate of nearly 20 degrees per hour. Interestingly, the rapid increase of the positive magnetic flux just occurred during the fastest rotation of the rotating sunspot, the bright loop-shaped structure and the filament. During the sunspot rotation, the inverse S-shaped filament gradually formed in the EUV filament channel. The filament experienced two eruptions. In the first eruption, the filament rose quickly and then the filament loops carrying the cool and the hot material were seen to spiral into the sunspot counterclockwise. About ten minutes later, the filament became active and finally erupted. The filament eruption was accompanied with a C-class flare and a halo coronal mass ejection (CME). These results provide evidence that sunspot rotation plays an important role in the formation and eruption of the sigmoidal active-region filament.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/sunspot-rotation-filament-and-flare-the-event-on-2000-february-10/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>IR-derived covering factors for a large sample of quasars from WISE-UKIDSS-SDSS</title>
		<link>http://voxcharta.org/2012/05/21/ir-derived-covering-factors-for-a-large-sample-of-quasars-from-wise-ukidss-sdss/</link>
		<comments>http://voxcharta.org/2012/05/21/ir-derived-covering-factors-for-a-large-sample-of-quasars-from-wise-ukidss-sdss/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:44:12 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion disk]]></category>
		<category><![CDATA[bia]]></category>
		<category><![CDATA[dependant]]></category>
		<category><![CDATA[estimates]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[micron]]></category>
		<category><![CDATA[quasar]]></category>
		<category><![CDATA[relationship]]></category>
		<category><![CDATA[sdss]]></category>
		<category><![CDATA[standard deviation]]></category>
		<category><![CDATA[survey]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/ir-derived-covering-factors-for-a-large-sample-of-quasars-from-wise-ukidss-sdss/</guid>
		<description><![CDATA[We investigate the range of covering factors (determined from the ratio of IR to UV/optical luminosity) seen in luminous quasars using a combination of data from the WISE, UKIDSS and SDSS surveys. Accretion disk (UV/optical) and obscuring dust (IR) luminosities are measured via the use of a simple three component SED model. We use these [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate the range of covering factors (determined from the ratio of IR to UV/optical luminosity) seen in luminous quasars using a combination of data from the WISE, UKIDSS and SDSS surveys. Accretion disk (UV/optical) and obscuring dust (IR) luminosities are measured via the use of a simple three component SED model. We use these estimates to investigate the distribution of covering factors and its relationship to both accretion luminosity and IR SED shape. The distribution of covering factors (f_C) is observed to be log-normal, with a bias-corrected mean of =-0.48 and standard deviation of 0.19. The fraction of IR luminosity emitted in the near-IR (1&#8211;5 micron) is found to be high (~40 per cent), and dependant on covering factor.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/ir-derived-covering-factors-for-a-large-sample-of-quasars-from-wise-ukidss-sdss/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The role of radiative losses in the late evolution of pulse-heated coronal loops/strands</title>
		<link>http://voxcharta.org/2012/05/21/the-role-of-radiative-losses-in-the-late-evolution-of-pulse-heated-coronal-loopsstrands/</link>
		<comments>http://voxcharta.org/2012/05/21/the-role-of-radiative-losses-in-the-late-evolution-of-pulse-heated-coronal-loopsstrands/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:43:43 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[curve]]></category>
		<category><![CDATA[curves]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[hydrodynamic simulation]]></category>
		<category><![CDATA[plasma]]></category>
		<category><![CDATA[plasma density]]></category>
		<category><![CDATA[radiative loss]]></category>
		<category><![CDATA[rate increase]]></category>
		<category><![CDATA[slope]]></category>
		<category><![CDATA[solar corona]]></category>
		<category><![CDATA[spectral line]]></category>
		<category><![CDATA[spectral model]]></category>
		<category><![CDATA[strand]]></category>
		<category><![CDATA[temperature]]></category>
		<category><![CDATA[temperature dependence]]></category>
		<category><![CDATA[threshold value]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/the-role-of-radiative-losses-in-the-late-evolution-of-pulse-heated-coronal-loopsstrands/</guid>
		<description><![CDATA[Radiative losses from optically thin plasma are an important ingredient for modeling plasma confined in the solar corona. Spectral models are continuously updated to include the emission from more spectral lines, with significant effects on radiative losses, especially around 1 MK. We investigate the effect of changing the radiative losses temperature dependence due to upgrading [...]]]></description>
			<content:encoded><![CDATA[<p>Radiative losses from optically thin plasma are an important ingredient for modeling plasma confined in the solar corona. Spectral models are continuously updated to include the emission from more spectral lines, with significant effects on radiative losses, especially around 1 MK. We investigate the effect of changing the radiative losses temperature dependence due to upgrading of spectral codes on predictions obtained from modeling plasma confined in the solar corona. The hydrodynamic simulation of a pulse-heated loop strand is revisited comparing results using an old and a recent radiative losses function. We find significant changes in the plasma evolution during the late phases of plasma cooling: when the recent radiative loss curve is used, the plasma cooling rate increases significantly when temperatures reach 1-2 MK. Such more rapid cooling occurs when the plasma density is larger than a threshold value, and therefore in impulsive heating models that cause the loop plasma to become overdense. The fast cooling has the effect of steepening the slope of the emission measure distribution of coronal plasmas with temperature at temperatures lower than ~2 MK. The effects of changes in the radiative losses curves can be important for modeling the late phases of the evolution of pulse-heated coronal loops, and, more in general, of thermally unstable optically thin plasmas.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/the-role-of-radiative-losses-in-the-late-evolution-of-pulse-heated-coronal-loopsstrands/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Comparison of star formation rates from Halpha and infrared luminosities as seen by Herschel</title>
		<link>http://voxcharta.org/2012/05/21/comparison-of-star-formation-rates-from-halpha-and-infrared-luminosities-as-seen-by-herschel/</link>
		<comments>http://voxcharta.org/2012/05/21/comparison-of-star-formation-rates-from-halpha-and-infrared-luminosities-as-seen-by-herschel/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:43:27 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[best fit]]></category>
		<category><![CDATA[dex]]></category>
		<category><![CDATA[dispersion]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[estimators]]></category>
		<category><![CDATA[extinction]]></category>
		<category><![CDATA[far ir]]></category>
		<category><![CDATA[herschel]]></category>
		<category><![CDATA[intrinsic property]]></category>
		<category><![CDATA[line measurement]]></category>
		<category><![CDATA[metallicity]]></category>
		<category><![CDATA[morphological type]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[sfr]]></category>
		<category><![CDATA[sigma level]]></category>
		<category><![CDATA[slope]]></category>
		<category><![CDATA[spiral galaxy]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[theoretical model]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/comparison-of-star-formation-rates-from-halpha-and-infrared-luminosities-as-seen-by-herschel/</guid>
		<description><![CDATA[We empirically test the relation between the SFR(LIR) derived from the infrared luminosity, LIR, and the SFR(Ha) derived from the Ha emission line luminosity using simple conversion relations. We use a sample of 474 galaxies at z = 0.06 &#8211; 0.46 with both Ha detection (from 20k zCOSMOS survey) and new far-IR Herschel data (100 [...]]]></description>
			<content:encoded><![CDATA[<p>We empirically test the relation between the SFR(LIR) derived from the infrared luminosity, LIR, and the SFR(Ha) derived from the Ha emission line luminosity using simple conversion relations. We use a sample of 474 galaxies at z = 0.06 &#8211; 0.46 with both Ha detection (from 20k zCOSMOS survey) and new far-IR Herschel data (100 and 160 {\mu}m). We derive SFR(Ha) from the Ha extinction corrected emission line luminosity. We find a very clear trend between E(B &#8211; V) and LIR that allows to estimate extinction values for each galaxy even if the Ha emission line measurement is not reliable. We calculate the LIR by integrating from 8 up to 1000 {\mu}m the SED that is best fitting our data. We compare SFR(Ha) with the SFR(LIR). We find a very good agreement between the two SFR estimates, with a slope of m = 1.01 \pm 0.03 in the SFR(LIR) vs SFR(Ha) diagram, a normalization constant of a = -0.08 \pm 0.03 and a dispersion of sigma = 0.28 dex.We study the effect of some intrinsic properties of the galaxies in the SFR(LIR)-SFR(Ha) relation, such as the redshift, the mass, the SSFR or the metallicity. The metallicity is the parameter that affects most the SFR comparison. The mean ratio of the two SFR estimators log[SFR(LIR)/SFR(Ha)] varies by approx. 0.6 dex from metal-poor to metal-rich galaxies (8.1 &lt; log(O/H) + 12 &lt; 9.2). This effect is consistent with the prediction of a theoretical model for the dust evolution in spiral galaxies. Considering different morphological types, we find a very good agreement between the two SFR indicators for the Sa, Sb and Sc morphologically classified galaxies, both in slope and normalization. For the Sd, irregular sample (Sd/Irr), the formal best-fit slope becomes much steeper (m = 1.62 \pm 0.43), but it is still consistent with 1 at the 1.5 sigma level, because of the reduced statistics of this sub-sample.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/comparison-of-star-formation-rates-from-halpha-and-infrared-luminosities-as-seen-by-herschel/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The structure of phase space close to fixed points in a 4D symplectic map [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/21/the-structure-of-phase-space-close-to-fixed-points-in-a-4d-symplectic-map-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/21/the-structure-of-phase-space-close-to-fixed-points-in-a-4d-symplectic-map-cross-listing/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:43:15 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[dynamical system]]></category>
		<category><![CDATA[hamiltonian system]]></category>
		<category><![CDATA[neighborhood]]></category>
		<category><![CDATA[periodic orbit]]></category>
		<category><![CDATA[phase space]]></category>
		<category><![CDATA[representations]]></category>
		<category><![CDATA[rotation method]]></category>
		<category><![CDATA[surface]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/the-structure-of-phase-space-close-to-fixed-points-in-a-4d-symplectic-map-cross-listing/</guid>
		<description><![CDATA[We study the dynamics in the neighborhood of fixed points in a 4D symplectic map by means of the color and rotation method. We compare the results with the corresponding cases encountered in galactic type potentials and we find that they are in good agreement. The fact that the 4D phase space close to fixed [...]]]></description>
			<content:encoded><![CDATA[<p>We study the dynamics in the neighborhood of fixed points in a 4D symplectic map by means of the color and rotation method. We compare the results with the corresponding cases encountered in galactic type potentials and we find that they are in good agreement. The fact that the 4D phase space close to fixed points is similar to the 4D representations of the surfaces of section close to periodic orbits, indicates an archetypical 4D pattern for each kind of (in)stability, not only in 3D autonomous Hamiltonian systems with galactic type potentials but for a larger class of dynamical systems. This pattern is successfully visualized with the method we use in the paper.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/the-structure-of-phase-space-close-to-fixed-points-in-a-4d-symplectic-map-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Remarks on the Cosmological Constant</title>
		<link>http://voxcharta.org/2012/05/21/remarks-on-the-cosmological-constant/</link>
		<comments>http://voxcharta.org/2012/05/21/remarks-on-the-cosmological-constant/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:43:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cosmological constant]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[einstein]]></category>
		<category><![CDATA[general relativity]]></category>
		<category><![CDATA[general theory of relativity]]></category>
		<category><![CDATA[Lambda]]></category>
		<category><![CDATA[mass energy]]></category>
		<category><![CDATA[observational data]]></category>
		<category><![CDATA[planck units]]></category>
		<category><![CDATA[radius]]></category>
		<category><![CDATA[theory of relativity]]></category>
		<category><![CDATA[visible universe]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/remarks-on-the-cosmological-constant/</guid>
		<description><![CDATA[Assuming only Einstein&#8217;s general theory of relativity, it is shown that the present observational data make it inevitable that (i) the cosmological constant Lambda must be non-zero and (ii) must be positive and less or of order $10^{-124}$ in Planck units. The co-moving radius R(t_0) of the spherical visible universe which is bounded by the [...]]]></description>
			<content:encoded><![CDATA[<p>Assuming only Einstein&#8217;s general theory of relativity, it is shown that the present observational data make it inevitable that (i) the cosmological constant Lambda must be non-zero and (ii) must be positive and less or of order $10^{-124}$ in Planck units. The co-moving radius R(t_0) of the spherical visible universe which is bounded by the surface of the last scatter, and the mass-energy M(t_0) contained therein lead to an outwardly accelerating cosmological expansion corresponding to that observed. The dark energy does not require a modification of general relativity but follows from it.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/remarks-on-the-cosmological-constant/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Proton, Electron, and Ion Heating in the Fast Solar Wind from Nonlinear Coupling Between Alfvenic and Fast-Mode Turbulence</title>
		<link>http://voxcharta.org/2012/05/21/proton-electron-and-ion-heating-in-the-fast-solar-wind-from-nonlinear-coupling-between-alfvenic-and-fast-mode-turbulence/</link>
		<comments>http://voxcharta.org/2012/05/21/proton-electron-and-ion-heating-in-the-fast-solar-wind-from-nonlinear-coupling-between-alfvenic-and-fast-mode-turbulence/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:42:32 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[advection]]></category>
		<category><![CDATA[coulomb]]></category>
		<category><![CDATA[diffusion equation]]></category>
		<category><![CDATA[energy input]]></category>
		<category><![CDATA[energy transfer]]></category>
		<category><![CDATA[frequency waves]]></category>
		<category><![CDATA[heavy ion]]></category>
		<category><![CDATA[interplanetary space]]></category>
		<category><![CDATA[ion cyclotron resonance]]></category>
		<category><![CDATA[ion populations]]></category>
		<category><![CDATA[mhd turbulence]]></category>
		<category><![CDATA[particle species]]></category>
		<category><![CDATA[proton electron]]></category>
		<category><![CDATA[situ measurement]]></category>
		<category><![CDATA[slow mode]]></category>
		<category><![CDATA[solar corona]]></category>
		<category><![CDATA[solar wind]]></category>
		<category><![CDATA[thermal equilibrium]]></category>
		<category><![CDATA[velocity distribution]]></category>
		<category><![CDATA[wave power]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/proton-electron-and-ion-heating-in-the-fast-solar-wind-from-nonlinear-coupling-between-alfvenic-and-fast-mode-turbulence/</guid>
		<description><![CDATA[In the parts of the solar corona and solar wind that experience the fewest Coulomb collisions, the component proton, electron, and heavy ion populations are not in thermal equilibrium with one another. Observed differences in temperatures, outflow speeds, and velocity distribution anisotropies are useful constraints on proposed explanations for how the plasma is heated and [...]]]></description>
			<content:encoded><![CDATA[<p>In the parts of the solar corona and solar wind that experience the fewest Coulomb collisions, the component proton, electron, and heavy ion populations are not in thermal equilibrium with one another. Observed differences in temperatures, outflow speeds, and velocity distribution anisotropies are useful constraints on proposed explanations for how the plasma is heated and accelerated. This paper presents new predictions of the rates of collisionless heating for each particle species, in which the energy input is assumed to come from magnetohydrodynamic (MHD) turbulence. We first created an empirical description of the radial evolution of Alfven, fast-mode, and slow-mode MHD waves. This model provides the total wave power in each mode as a function of distance along an expanding flux tube in the high-speed solar wind. Next we solved a set of cascade advection-diffusion equations that give the time-steady wavenumber spectra at each distance. An approximate term for nonlinear coupling between the Alfven and fast-mode fluctuations is included. For reasonable choices of the parameters, our model contains enough energy transfer from the fast mode to the Alfven mode to excite the high-frequency ion cyclotron resonance. This resonance is efficient at heating protons and other ions in the direction perpendicular to the background magnetic field, and our model predicts heating rates for these species that agree well with both spectroscopic and in situ measurements. Nonetheless, the high-frequency waves comprise only a small part of the total Alfvenic fluctuation spectrum, which remains highly two-dimensional as is observed in interplanetary space.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/proton-electron-and-ion-heating-in-the-fast-solar-wind-from-nonlinear-coupling-between-alfvenic-and-fast-mode-turbulence/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Impact cratering on Mercury: consequences for the spin evolution</title>
		<link>http://voxcharta.org/2012/05/21/impact-cratering-on-mercury-consequences-for-the-spin-evolution/</link>
		<comments>http://voxcharta.org/2012/05/21/impact-cratering-on-mercury-consequences-for-the-spin-evolution/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:42:16 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[asteroids]]></category>
		<category><![CDATA[collisional]]></category>
		<category><![CDATA[consequence]]></category>
		<category><![CDATA[diameter]]></category>
		<category><![CDATA[dissipation]]></category>
		<category><![CDATA[early solar system]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[flyby]]></category>
		<category><![CDATA[images]]></category>
		<category><![CDATA[mariner 10]]></category>
		<category><![CDATA[mercury]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[resonance]]></category>
		<category><![CDATA[spin state]]></category>
		<category><![CDATA[synchronous rotation]]></category>
		<category><![CDATA[variation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/impact-cratering-on-mercury-consequences-for-the-spin-evolution/</guid>
		<description><![CDATA[Impact basins identified by Mariner 10 and Messenger flyby images provide us a fossilized record of the impactor flux of asteroids on Mercury during the last stages of the early Solar System. The distribution of these basins is not uniform across the surface, and is consistent with a primordial synchronous rotation (Wieczorek et al. 2012). [...]]]></description>
			<content:encoded><![CDATA[<p>Impact basins identified by Mariner 10 and Messenger flyby images provide us a fossilized record of the impactor flux of asteroids on Mercury during the last stages of the early Solar System. The distribution of these basins is not uniform across the surface, and is consistent with a primordial synchronous rotation (Wieczorek et al. 2012). By analyzing the size of the impacts, we show that the distribution for asteroid diameters D &lt; 110 km is compatible with an index power law of 1.2, a value that matches the predicted primordial distribution of the main-belt. We then derive a simple collisional model coherent with the observations, and when combining it with the secular evolution of the spin of Mercury, we are able to reproduce the present 3/2 spin-orbit resonance (about 50% of chances), as well as a primordial synchronous rotation. This result is robust with respect to variations in the dissipation and collisional models, or in the initial spin state of the planet.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/impact-cratering-on-mercury-consequences-for-the-spin-evolution/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Effect of metallicity on the gravitational-wave signal from the cosmological population of compact binary coalescences</title>
		<link>http://voxcharta.org/2012/05/21/effect-of-metallicity-on-the-gravitational-wave-signal-from-the-cosmological-population-of-compact-binary-coalescences/</link>
		<comments>http://voxcharta.org/2012/05/21/effect-of-metallicity-on-the-gravitational-wave-signal-from-the-cosmological-population-of-compact-binary-coalescences/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:42:04 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[compact binaries]]></category>
		<category><![CDATA[compact object]]></category>
		<category><![CDATA[einstein]]></category>
		<category><![CDATA[first peak]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[gravitational wave signal]]></category>
		<category><![CDATA[ligo]]></category>
		<category><![CDATA[metallicity]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[stellar evolution]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[synthesis]]></category>
		<category><![CDATA[Telescope]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/effect-of-metallicity-on-the-gravitational-wave-signal-from-the-cosmological-population-of-compact-binary-coalescences/</guid>
		<description><![CDATA[Recent studies on stellar evolution have shown that the properties of compact objects strongly depend on metallicity of the environment in which they were formed. In this work, we study how the metallicity of the stellar population can affect unresolved gravitational waves background from extragalactic compact binaries. We obtain a suit of models of compact [...]]]></description>
			<content:encoded><![CDATA[<p>Recent studies on stellar evolution have shown that the properties of compact objects strongly depend on metallicity of the environment in which they were formed. In this work, we study how the metallicity of the stellar population can affect unresolved gravitational waves background from extragalactic compact binaries. We obtain a suit of models of compact binaries using population synthesis code and estimate the gravitational wave background they produce. Our results show a double peaked structure for all considered models with the first peak between 30-100Hz caused by the binary black holes population and the second between 500-1000Hz corresponding to the double neutron stars population. We discuss the detectability of gravitational waves background with second (Advanced LIGO, Advanced Virgo) and third (Einstein Telescope) generation detectors.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/effect-of-metallicity-on-the-gravitational-wave-signal-from-the-cosmological-population-of-compact-binary-coalescences/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Cosmic Flows surveys and CLUES simulations</title>
		<link>http://voxcharta.org/2012/05/21/cosmic-flows-surveys-and-clues-simulations/</link>
		<comments>http://voxcharta.org/2012/05/21/cosmic-flows-surveys-and-clues-simulations/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:41:47 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cosmic flow]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[definitive answer]]></category>
		<category><![CDATA[deviations]]></category>
		<category><![CDATA[dipole]]></category>
		<category><![CDATA[expansion of the universe]]></category>
		<category><![CDATA[fundamental discoveries]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[galaxy distances]]></category>
		<category><![CDATA[microwave background]]></category>
		<category><![CDATA[reconstruction]]></category>
		<category><![CDATA[resultant velocity]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[survey]]></category>
		<category><![CDATA[synergy]]></category>
		<category><![CDATA[systematic error]]></category>
		<category><![CDATA[unsolved problem]]></category>
		<category><![CDATA[velocity field]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/cosmic-flows-surveys-and-clues-simulations/</guid>
		<description><![CDATA[Cosmic Flows is a program to determine galaxy distances for 30,000 galaxies with systematic errors below 2%, almost ten times the number currently known and a five-fold improvement in systematics. The resultant velocity field will provide input for constrained local universe simulations: CLUES (www.clues-project.org). The observed and the simulated universe are then comparatively studied. This [...]]]></description>
			<content:encoded><![CDATA[<p>Cosmic Flows is a program to determine galaxy distances for 30,000 galaxies with systematic errors below 2%, almost ten times the number currently known and a five-fold improvement in systematics. The resultant velocity field will provide input for constrained local universe simulations: CLUES (<a href="http://www.clues-project.org">www.clues-project.org</a>). The observed and the simulated universe are then comparatively studied. This synergy of observations and theory distinguishes the program, and should lead to fundamental discoveries regarding the sources of deviations from the expansion of the universe. Specifically, the program should give a definitive answer to one of the most outstanding unsolved problem in cosmology: the cause of the motion of 630 km/s of our Galaxy manifested in the microwave background dipole. This paper presents current results with particular emphasis on the &#8220;great attractor&#8221; reconstruction.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/cosmic-flows-surveys-and-clues-simulations/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A note on the observational evidence for the existence of event horizons in astrophysical black hole candidates [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/21/a-note-on-the-observational-evidence-for-the-existence-of-event-horizons-in-astrophysical-black-hole-candidates-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/21/a-note-on-the-observational-evidence-for-the-existence-of-event-horizons-in-astrophysical-black-hole-candidates-cross-listing/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:41:34 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[astrophysical observations]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[electromagnetic radiation]]></category>
		<category><![CDATA[event horizon]]></category>
		<category><![CDATA[existence]]></category>
		<category><![CDATA[hole candidate]]></category>
		<category><![CDATA[observation]]></category>
		<category><![CDATA[observational evidence]]></category>
		<category><![CDATA[universe today]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/a-note-on-the-observational-evidence-for-the-existence-of-event-horizons-in-astrophysical-black-hole-candidates-cross-listing/</guid>
		<description><![CDATA[Black holes have the peculiar and intriguing property of having an event horizon, a one-way membrane causally separating their internal region from the rest of the Universe. Today astrophysical observations provide some evidence for the existence of event horizons in astrophysical black hole candidates. In this short paper, I compare the constraint we can infer [...]]]></description>
			<content:encoded><![CDATA[<p>Black holes have the peculiar and intriguing property of having an event horizon, a one-way membrane causally separating their internal region from the rest of the Universe. Today astrophysical observations provide some evidence for the existence of event horizons in astrophysical black hole candidates. In this short paper, I compare the constraint we can infer from the non-observation of electromagnetic radiation from the putative surface of these objects with the bound coming from the ergoregion instability, pointing out the respective assumptions and limitations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/a-note-on-the-observational-evidence-for-the-existence-of-event-horizons-in-astrophysical-black-hole-candidates-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Fermi Gamma Ray Line at 130 GeV from Axion-Mediated Dark Matter [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/21/fermi-gamma-ray-line-at-130-gev-from-axion-mediated-dark-matter-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/21/fermi-gamma-ray-line-at-130-gev-from-axion-mediated-dark-matter-cross-listing/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:41:02 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[annihilation]]></category>
		<category><![CDATA[anomaly]]></category>
		<category><![CDATA[cross section]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[Fermi]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[interaction]]></category>
		<category><![CDATA[interplay]]></category>
		<category><![CDATA[mediation]]></category>
		<category><![CDATA[photon line]]></category>
		<category><![CDATA[scalar]]></category>
		<category><![CDATA[singlet]]></category>
		<category><![CDATA[symmetry]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/fermi-gamma-ray-line-at-130-gev-from-axion-mediated-dark-matter-cross-listing/</guid>
		<description><![CDATA[We consider a singlet fermion dark matter with PQ symmetry. A singlet complex scalar is introduced to mediate between dark matter and the SM through Higgs portal interaction and electroweak PQ anomalies. We show that dark matter annihilation with axion mediation can explain a monochromatic photon line of the Fermi LAT data at 130 GeV [...]]]></description>
			<content:encoded><![CDATA[<p>We consider a singlet fermion dark matter with PQ symmetry. A singlet complex scalar is introduced to mediate between dark matter and the SM through Higgs portal interaction and electroweak PQ anomalies. We show that dark matter annihilation with axion mediation can explain a monochromatic photon line of the Fermi LAT data at 130 GeV by anomaly interactions while the annihilation cross section with Higgs portal interaction is p-wave suppressed. We discuss the interplay between direct detection of the fermion dark matter and the collider search of Higgs-like scalars. We also present a ultra-violet completion of the dark matter model into the NMSSM with PQ symmetry.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/fermi-gamma-ray-line-at-130-gev-from-axion-mediated-dark-matter-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Testing some f(R,T) gravity models from energy conditions [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/21/testing-some-frt-gravity-models-from-energy-conditions-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/21/testing-some-frt-gravity-models-from-energy-conditions-cross-listing/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:40:50 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[curvature]]></category>
		<category><![CDATA[einstein]]></category>
		<category><![CDATA[energy conditions]]></category>
		<category><![CDATA[energy momentum tensor]]></category>
		<category><![CDATA[expression]]></category>
		<category><![CDATA[gravity model]]></category>
		<category><![CDATA[hilbert]]></category>
		<category><![CDATA[input parameter]]></category>
		<category><![CDATA[momentum]]></category>
		<category><![CDATA[satis]]></category>
		<category><![CDATA[theory of gravity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/testing-some-frt-gravity-models-from-energy-conditions-cross-listing/</guid>
		<description><![CDATA[We consider f(R; T) theory of gravity, where R is the curvature scalar and T the trace of the energy momentum tensor. Attention is attached to the special case, f(R; T) = R + 2f(T) as a f(T) correction to the Einstein-Hilbert term. Two expressions are assumed for the function f(T), $\frac{a_1T^n+b_1}{a_2T^n+b_2}$ and $a_3ln^q(b_3T^m)$, where [...]]]></description>
			<content:encoded><![CDATA[<p>We consider f(R; T) theory of gravity, where R is the curvature scalar and T the trace of the energy momentum tensor. Attention is attached to the special case, f(R; T) = R + 2f(T) as a f(T) correction to the Einstein-Hilbert term. Two expressions are assumed for the function f(T), $\frac{a_1T^n+b_1}{a_2T^n+b_2}$ and $a_3ln^q(b_3T^m)$, where $a1$, $a2$, $b1$, $b2$, $n$, $a3$, $b3$, $q$ and $m$ are input parameters. We observe that by adjusting suitably these input parameters, energy conditions are satis?fied and viable f(R; T) models corresponding to the two assumptions of f(T) may be obtained.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/testing-some-frt-gravity-models-from-energy-conditions-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A combined measurement of cosmic growth and expansion from clusters of galaxies, the CMB and galaxy clustering</title>
		<link>http://voxcharta.org/2012/05/21/a-combined-measurement-of-cosmic-growth-and-expansion-from-clusters-of-galaxies-the-cmb-and-galaxy-clustering/</link>
		<comments>http://voxcharta.org/2012/05/21/a-combined-measurement-of-cosmic-growth-and-expansion-from-clusters-of-galaxies-the-cmb-and-galaxy-clustering/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:40:37 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[chandra x ray]]></category>
		<category><![CDATA[clusters of galaxies]]></category>
		<category><![CDATA[cold dark matter]]></category>
		<category><![CDATA[cosmic expansion]]></category>
		<category><![CDATA[cosmic microwave background]]></category>
		<category><![CDATA[digital sky survey]]></category>
		<category><![CDATA[energy density]]></category>
		<category><![CDATA[galaxy cluster]]></category>
		<category><![CDATA[galaxy survey]]></category>
		<category><![CDATA[general relativity]]></category>
		<category><![CDATA[growth parameters]]></category>
		<category><![CDATA[matter density]]></category>
		<category><![CDATA[mean matter]]></category>
		<category><![CDATA[microwave anisotropy probe]]></category>
		<category><![CDATA[model parameter]]></category>
		<category><![CDATA[ray observatory]]></category>
		<category><![CDATA[sloan digital]]></category>
		<category><![CDATA[systematic uncertainty]]></category>
		<category><![CDATA[wilkinson microwave anisotropy]]></category>
		<category><![CDATA[wilkinson microwave anisotropy probe]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/a-combined-measurement-of-cosmic-growth-and-expansion-from-clusters-of-galaxies-the-cmb-and-galaxy-clustering/</guid>
		<description><![CDATA[Combining galaxy cluster data from the ROSAT All-Sky Survey and the Chandra X-ray Observatory, cosmic microwave background data from the Wilkinson Microwave Anisotropy Probe, and galaxy clustering data from the WiggleZ Dark Energy Survey, the 6-degree Field Galaxy Survey and the Sloan Digital Sky Survey III, we test for consistency the cosmic growth of structure [...]]]></description>
			<content:encoded><![CDATA[<p>Combining galaxy cluster data from the ROSAT All-Sky Survey and the Chandra X-ray Observatory, cosmic microwave background data from the Wilkinson Microwave Anisotropy Probe, and galaxy clustering data from the WiggleZ Dark Energy Survey, the 6-degree Field Galaxy Survey and the Sloan Digital Sky Survey III, we test for consistency the cosmic growth of structure predicted by General Relativity (GR) and the cosmic expansion history predicted by the cosmological constant plus cold dark matter paradigm (LCDM). The combination of these three independent, well studied measurements of the evolution of the mean energy density and its fluctuations is able to break strong degeneracies between model parameters. We model the key properties of cosmic growth with the normalization of the matter power spectrum, sigma_8, and the cosmic growth index, gamma, and those of cosmic expansion with the mean matter density, Omega_m, the Hubble constant, H_0, and a kinematical parameter equivalent to that for the dark energy equation of state, w. To further tighten constraints on the expansion parameters, we also include supernova, baryon acoustic oscillation and Cepheid variable data. For a spatially flat geometry, w=-1, and allowing for systematic uncertainties, we obtain sigma_8=0.787+-0.019 and gamma=0.576+0.058-0.059 (at the 68.3 per cent confidence level). Allowing w to vary, we find Omega_m=0.256+-0.011, H_0=71.5+-1.3 km s^-1 Mpc^-1 and w=-0.968+-0.049 for the expansion parameters, and sigma_8=0.783+0.020-0.019 and gamma=0.546+0.071-0.072 for the growth parameters. These results are in excellent agreement with GR+LCDM (gamma~0.55; w=-1) and represent the tightest and most robust simultaneous constraint on cosmic growth and expansion to date.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/a-combined-measurement-of-cosmic-growth-and-expansion-from-clusters-of-galaxies-the-cmb-and-galaxy-clustering/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Is the transition redshift a new cosmological number?</title>
		<link>http://voxcharta.org/2012/05/21/is-the-transition-redshift-a-new-cosmological-number/</link>
		<comments>http://voxcharta.org/2012/05/21/is-the-transition-redshift-a-new-cosmological-number/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:40:21 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accelerating universe]]></category>
		<category><![CDATA[acceleration]]></category>
		<category><![CDATA[baryon]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[deceleration]]></category>
		<category><![CDATA[differential]]></category>
		<category><![CDATA[discriminator]]></category>
		<category><![CDATA[drift]]></category>
		<category><![CDATA[dynamic phase]]></category>
		<category><![CDATA[dynamic role]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gravitational theory]]></category>
		<category><![CDATA[intermediate redshift]]></category>
		<category><![CDATA[line of sight]]></category>
		<category><![CDATA[parameter space]]></category>
		<category><![CDATA[phase transition]]></category>
		<category><![CDATA[principle]]></category>
		<category><![CDATA[realistic model]]></category>
		<category><![CDATA[spectral line]]></category>
		<category><![CDATA[type ia]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/is-the-transition-redshift-a-new-cosmological-number/</guid>
		<description><![CDATA[Observations from Supernovae Type Ia (SNe Ia) provided strong evidence for an expanding accelerating Universe at intermediate redshifts. This means that the Universe underwent a dynamic phase transition from deceleration to acceleration at a transition redshift $z_t$ of the order unity whose value in principle depends on the cosmology as well as on the assumed [...]]]></description>
			<content:encoded><![CDATA[<p>Observations from Supernovae Type Ia (SNe Ia) provided strong evidence for an expanding accelerating Universe at intermediate redshifts. This means that the Universe underwent a dynamic phase transition from deceleration to acceleration at a transition redshift $z_t$ of the order unity whose value in principle depends on the cosmology as well as on the assumed gravitational theory. Since cosmological accelerating models endowed with a transition redshift are extremely degenerated, in principle, it is interesting to know whether the value of $z_t$ itself can be observationally used as a new cosmic discriminator. After a brief discussion of the potential dynamic role played by the transition redshift, it is argued that future observations combining SNe Ia, the line-of-sight (or &#8220;radial&#8221;) baryon acoustic oscillations, the differential age of galaxies, as well as the redshift drift of the spectral lines may tightly constrain $z_t$, thereby helping to narrow the parameter space for the most realistic models describing the accelerating Universe.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/is-the-transition-redshift-a-new-cosmological-number/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Evolution of the baryon fraction in the Local Group: accretion versus feedback at low and high z</title>
		<link>http://voxcharta.org/2012/05/21/evolution-of-the-baryon-fraction-in-the-local-group-accretion-versus-feedback-at-low-and-high-z/</link>
		<comments>http://voxcharta.org/2012/05/21/evolution-of-the-baryon-fraction-in-the-local-group-accretion-versus-feedback-at-low-and-high-z/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:39:42 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[AGN]]></category>
		<category><![CDATA[baryonic]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[galaxy formation]]></category>
		<category><![CDATA[group type]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[local group]]></category>
		<category><![CDATA[mass budget]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[physical mechanism]]></category>
		<category><![CDATA[present time]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[tidal disruption]]></category>
		<category><![CDATA[type galaxy]]></category>
		<category><![CDATA[universal value]]></category>
		<category><![CDATA[whim]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/evolution-of-the-baryon-fraction-in-the-local-group-accretion-versus-feedback-at-low-and-high-z/</guid>
		<description><![CDATA[Using hydrodynamical zoom simulations in the standard LCDM cosmology, we investigate the evolution of the distribution of baryons (gas and stars) in a local group-type universe. First, with standard star formation and supernova feedback prescriptions, we find that the mean baryonic fraction value estimated at the virial radius of the two main central objects (i.e. [...]]]></description>
			<content:encoded><![CDATA[<p>Using hydrodynamical zoom simulations in the standard LCDM cosmology, we investigate the evolution of the distribution of baryons (gas and stars) in a local group-type universe. First, with standard star formation and supernova feedback prescriptions, we find that the mean baryonic fraction value estimated at the virial radius of the two main central objects (i.e. the Milky Way and Andromeda) is decreasing over time, and is 10-15% lower than the universal value, 0.166, at z=0. This decrease is mainly due to the fact that the amount of accretion of dissipative gas onto the halo, especially at low redshift, is in general much lower than that of the dissipationless dark matter. Indeed, a significant part of the baryons does not collapse onto the haloes and remains in their outskirts, mainly in the form of warm-hot intergalactic medium (WHIM). Moreover, during the formation of each object, some dark matter and baryons are also be expelled through merger events via tidal disruption. In contrast to baryons, expelled dark matter can be more efficiently re-accreted onto the halo, enhancing both the reduction of fb inside Rv, and the increase of the mass of WHIM outside Rv. Varying the efficiency of supernovae feedback at low redshift does not seem to significantly affect these trends. Alternatively, when a significant fraction of the initial gas in the main objects is released at high redshifts by more powerful sources of feedback, such as AGN from intermediate mass black holes in lower mass galaxies, the baryonic fraction at the virial radius can have a lower value (fb~0.12) at low redshift. Hence physical mechanisms able to slow down the accretion of gas at high redshifts will have a stronger impact on the deficit of baryons in the mass budget of Milky Way type-galaxies at present times than those that expel the gas in the longer, late phases of galaxy formation.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/evolution-of-the-baryon-fraction-in-the-local-group-accretion-versus-feedback-at-low-and-high-z/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>VLSS Redux: Software Improvements applied to the Very Large Array Low-frequency Sky Survey</title>
		<link>http://voxcharta.org/2012/05/21/vlss-redux-software-improvements-applied-to-the-very-large-array-low-frequency-sky-survey/</link>
		<comments>http://voxcharta.org/2012/05/21/vlss-redux-software-improvements-applied-to-the-very-large-array-low-frequency-sky-survey/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:39:29 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accuracy]]></category>
		<category><![CDATA[angular size]]></category>
		<category><![CDATA[bia]]></category>
		<category><![CDATA[bright source]]></category>
		<category><![CDATA[data processing]]></category>
		<category><![CDATA[fluctuation]]></category>
		<category><![CDATA[low frequency]]></category>
		<category><![CDATA[obit]]></category>
		<category><![CDATA[peeling]]></category>
		<category><![CDATA[radio frequency interference]]></category>
		<category><![CDATA[resolution reference]]></category>
		<category><![CDATA[sky survey]]></category>
		<category><![CDATA[software improvements]]></category>
		<category><![CDATA[source catalog]]></category>
		<category><![CDATA[substantial improvement]]></category>
		<category><![CDATA[survey area]]></category>
		<category><![CDATA[technical improvement]]></category>
		<category><![CDATA[very large array]]></category>
		<category><![CDATA[windowing]]></category>
		<category><![CDATA[zernike]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/vlss-redux-software-improvements-applied-to-the-very-large-array-low-frequency-sky-survey/</guid>
		<description><![CDATA[We present details of improvements to data processing and analysis which were recently used for a re-reduction of the Very Large Array (VLA) Low-frequency Sky Survey (VLSS) data. Algorithms described are implemented in the data-reduction package Obit, and include smart-windowing to reduce clean bias, improved automatic radio frequency interference removal, improved bright-source peeling, and higher-order [...]]]></description>
			<content:encoded><![CDATA[<p>We present details of improvements to data processing and analysis which were recently used for a re-reduction of the Very Large Array (VLA) Low-frequency Sky Survey (VLSS) data. Algorithms described are implemented in the data-reduction package Obit, and include smart-windowing to reduce clean bias, improved automatic radio frequency interference removal, improved bright-source peeling, and higher-order Zernike fits to model the ionospheric phase contributions. An additional, but less technical improvement was using the original VLSS catalog as a same-frequency/same-resolution reference for calculating ionospheric corrections, allowing more accuracy and a higher percentage of data for which solutions are found. We also discuss new algorithms for extracting a source catalog and analyzing ionospheric fluctuations present in the data. The improved reduction techniques led to substantial improvements including images of six previously unpublished fields (1% of the survey area) and reducing the clean bias by 50%. The largest angular size imaged has been roughly doubled, and the number of cataloged sources is increased by 35% to 95,000.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/vlss-redux-software-improvements-applied-to-the-very-large-array-low-frequency-sky-survey/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Spectral and spatial variations of the diffuse gamma-ray background in the vicinity of the Galactic plane and possible nature of the feature at 130 GeV</title>
		<link>http://voxcharta.org/2012/05/21/spectral-and-spatial-variations-of-the-diffuse-gamma-ray-background-in-the-vicinity-of-the-galactic-plane-and-possible-nature-of-the-feature-at-130-gev/</link>
		<comments>http://voxcharta.org/2012/05/21/spectral-and-spatial-variations-of-the-diffuse-gamma-ray-background-in-the-vicinity-of-the-galactic-plane-and-possible-nature-of-the-feature-at-130-gev/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:39:06 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[confidence]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[diffuse background]]></category>
		<category><![CDATA[dips]]></category>
		<category><![CDATA[excesses]]></category>
		<category><![CDATA[features change]]></category>
		<category><![CDATA[galactic center]]></category>
		<category><![CDATA[galactic plane]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[law component]]></category>
		<category><![CDATA[shape]]></category>
		<category><![CDATA[sky]]></category>
		<category><![CDATA[smooth power]]></category>
		<category><![CDATA[spatial variation]]></category>
		<category><![CDATA[spectral feature]]></category>
		<category><![CDATA[spectrum]]></category>
		<category><![CDATA[vicinity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/spectral-and-spatial-variations-of-the-diffuse-gamma-ray-background-in-the-vicinity-of-the-galactic-plane-and-possible-nature-of-the-feature-at-130-gev/</guid>
		<description><![CDATA[We study the properties of the diffuse gamma-ray background around the Galactic plane at energies 60 &#8211; 200 GeV. We find that the spectrum of this emission possesses spacial variations having significant features (excesses and dips) as compared to the average smooth (power law) component. The positions and shapes of these spectral features change with [...]]]></description>
			<content:encoded><![CDATA[<p>We study the properties of the diffuse gamma-ray background around the Galactic plane at energies 60 &#8211; 200 GeV. We find that the spectrum of this emission possesses spacial variations having significant features (excesses and dips) as compared to the average smooth (power law) component. The positions and shapes of these spectral features change with direction on the sky. We therefore argue, that the spectral feature around 130 GeV, found in several regions around the Galactic Center and the Galactic plane in [1204.2797,1205.1045], can not be interpreted with confidence as a gamma-ray line, but may be a component of the diffuse background and can be of instrumental or astrophysical origin. Therefore, the dark matter origin of this spectral feature becomes dubious.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/spectral-and-spatial-variations-of-the-diffuse-gamma-ray-background-in-the-vicinity-of-the-galactic-plane-and-possible-nature-of-the-feature-at-130-gev/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>
		</item>
		<item>
		<title>X-Ray And Optical Flux Ratio Anomalies In Quadruply Lensed Quasars. II. Mapping the Dark Matter Content in Elliptical Galaxies [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/x-ray-and-optical-flux-ratio-anomalies-in-quadruply-lensed-quasars-ii-mapping-the-dark-matter-content-in-elliptical-galaxies-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/x-ray-and-optical-flux-ratio-anomalies-in-quadruply-lensed-quasars-ii-mapping-the-dark-matter-content-in-elliptical-galaxies-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:38:41 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[anomaly]]></category>
		<category><![CDATA[bayesian analysis]]></category>
		<category><![CDATA[chandra observation]]></category>
		<category><![CDATA[dark matter content]]></category>
		<category><![CDATA[elliptical galaxy]]></category>
		<category><![CDATA[ensembles]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[impact parameter]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[lensed quasar]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[optical flux]]></category>
		<category><![CDATA[quasar images]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/x-ray-and-optical-flux-ratio-anomalies-in-quadruply-lensed-quasars-ii-mapping-the-dark-matter-content-in-elliptical-galaxies-replacement/</guid>
		<description><![CDATA[We present a microlensing analysis of 61 Chandra observations of 14 quadruply lensed quasars. X-ray flux measurements of the individual quasar images give a clean determination of the microlensing effects in the lensing galaxy and thus offer a direct assessment of the local fraction of stellar matter making up the total integrated mass along the [...]]]></description>
			<content:encoded><![CDATA[<p>We present a microlensing analysis of 61 Chandra observations of 14 quadruply lensed quasars. X-ray flux measurements of the individual quasar images give a clean determination of the microlensing effects in the lensing galaxy and thus offer a direct assessment of the local fraction of stellar matter making up the total integrated mass along the lines of sight through the lensing galaxy. A Bayesian analysis of the ensemble of lensing galaxies gives a most likely local stellar fraction of 7%, with the other 93% in a smooth, dark matter component, at an average impact parameter R_c of 6.6 kpc from the center of the lensing galaxy. We divide the systems into smaller ensembles based on R_c and find that the most likely local stellar fraction varies qualitatively and quantitatively as expected, decreasing as a function of R_c.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/x-ray-and-optical-flux-ratio-anomalies-in-quadruply-lensed-quasars-ii-mapping-the-dark-matter-content-in-elliptical-galaxies-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A new signature of primordial non-Gaussianities from the abundance of galaxy clusters [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/a-new-signature-of-primordial-non-gaussianities-from-the-abundance-of-galaxy-clusters-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/a-new-signature-of-primordial-non-gaussianities-from-the-abundance-of-galaxy-clusters-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:38:30 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abundance]]></category>
		<category><![CDATA[appearance]]></category>
		<category><![CDATA[characterization]]></category>
		<category><![CDATA[cluster counts]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[density perturbations]]></category>
		<category><![CDATA[deviations]]></category>
		<category><![CDATA[discontinuity]]></category>
		<category><![CDATA[early universe]]></category>
		<category><![CDATA[energy equation]]></category>
		<category><![CDATA[equation of state]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[galaxy cluster]]></category>
		<category><![CDATA[inflationary scenarios]]></category>
		<category><![CDATA[initial condition]]></category>
		<category><![CDATA[physical processes]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[signature]]></category>
		<category><![CDATA[statistical properties]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/a-new-signature-of-primordial-non-gaussianities-from-the-abundance-of-galaxy-clusters-replacement/</guid>
		<description><![CDATA[The evolution with time of the abundance of galaxy clusters is very sensitive to the statistical properties of the primordial density perturbations. It can thus be used to probe small deviations from Gaussianity in the initial conditions. The characterization of such deviations would help distinguish between different inflationary scenarios, and provide us with information on [...]]]></description>
			<content:encoded><![CDATA[<p>The evolution with time of the abundance of galaxy clusters is very sensitive to the statistical properties of the primordial density perturbations. It can thus be used to probe small deviations from Gaussianity in the initial conditions. The characterization of such deviations would help distinguish between different inflationary scenarios, and provide us with information on physical processes which took place in the early Universe. We have found that when the information contained in the galaxy cluster counts is used to reconstruct the dark energy equation of state as a function of redshift, assuming erroneously that no primordial non-Gaussianities exist, an apparent evolution with time in the effective dark energy equation of state arises,characterized by the appearance of a clear discontinuity.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/a-new-signature-of-primordial-non-gaussianities-from-the-abundance-of-galaxy-clusters-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<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>
		</item>
		<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>
		</item>
		<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>Constraining mean-field models of the nuclear matter equation of state at low densities [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/constraining-mean-field-models-of-the-nuclear-matter-equation-of-state-at-low-densities-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/constraining-mean-field-models-of-the-nuclear-matter-equation-of-state-at-low-densities-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:37:05 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astrophysical applications]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[coupling]]></category>
		<category><![CDATA[degrees of freedom]]></category>
		<category><![CDATA[dense nuclear matter]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[dependent properties]]></category>
		<category><![CDATA[equation of state]]></category>
		<category><![CDATA[expansion]]></category>
		<category><![CDATA[field model]]></category>
		<category><![CDATA[light nuclei]]></category>
		<category><![CDATA[low density]]></category>
		<category><![CDATA[meson]]></category>
		<category><![CDATA[neutron]]></category>
		<category><![CDATA[nucleon]]></category>
		<category><![CDATA[phase shift]]></category>
		<category><![CDATA[relativistic effects]]></category>
		<category><![CDATA[saturation]]></category>
		<category><![CDATA[veos]]></category>
		<category><![CDATA[virial equation of state]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/constraining-mean-field-models-of-the-nuclear-matter-equation-of-state-at-low-densities-replacement/</guid>
		<description><![CDATA[An extension of the generalized relativistic mean-field (gRMF) model with density dependent couplings is introduced in order to describe thermodynamical properties and the composition of dense nuclear matter for astrophysical applications. Bound states of light nuclei and two-nucleon scattering correlations are considered as explicit degrees of freedom in the thermodynamical potential. They are represented by [...]]]></description>
			<content:encoded><![CDATA[<p>An extension of the generalized relativistic mean-field (gRMF) model with density dependent couplings is introduced in order to describe thermodynamical properties and the composition of dense nuclear matter for astrophysical applications. Bound states of light nuclei and two-nucleon scattering correlations are considered as explicit degrees of freedom in the thermodynamical potential. They are represented by quasiparticles with medium-dependent properties. The model describes the correct low-density limit given by the virial equation of state (VEoS) and reproduces RMF results around nuclear saturation density where clusters are dissolved. A comparison between the fugacity expansions of the VEoS and the gRMF model provides consistency relations between the quasiparticles properties, the nucleon-nucleon scattering phase shifts and the meson-nucleon couplings of the gRMF model at zero density. Relativistic effects are found to be important at temperatures that are typical in astrophysical applications. Neutron matter and symmetric matter are studied in detail.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/constraining-mean-field-models-of-the-nuclear-matter-equation-of-state-at-low-densities-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Neutrinos and the stars [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/neutrinos-and-the-stars-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/neutrinos-and-the-stars-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:36:46 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[energy loss]]></category>
		<category><![CDATA[high density]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[mass particle]]></category>
		<category><![CDATA[Measurement]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[neutrino]]></category>
		<category><![CDATA[oscillation]]></category>
		<category><![CDATA[sn 1987a]]></category>
		<category><![CDATA[statistic]]></category>
		<category><![CDATA[Sun]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/neutrinos-and-the-stars-replacement/</guid>
		<description><![CDATA[The role of neutrinos in stars is introduced for students with little prior astrophysical exposure. We begin with neutrinos as an energy-loss channel in ordinary stars and conversely, how stars provide information on neutrinos and possible other low-mass particles. Next we turn to the Sun as a measurable source of neutrinos and other particles. Finally [...]]]></description>
			<content:encoded><![CDATA[<p>The role of neutrinos in stars is introduced for students with little prior astrophysical exposure. We begin with neutrinos as an energy-loss channel in ordinary stars and conversely, how stars provide information on neutrinos and possible other low-mass particles. Next we turn to the Sun as a measurable source of neutrinos and other particles. Finally we discuss supernova (SN) neutrinos, the SN 1987A measurements, and the quest for a high-statistics neutrino measurement from the next nearby SN. We also touch on the subject of neutrino oscillations in the high-density SN context.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/neutrinos-and-the-stars-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Star formation in LINER host galaxies at z~0.3 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/star-formation-in-liner-host-galaxies-at-z0-3-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/star-formation-in-liner-host-galaxies-at-z0-3-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:36:21 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[AGN]]></category>
		<category><![CDATA[agns]]></category>
		<category><![CDATA[alpha emission]]></category>
		<category><![CDATA[dusty star]]></category>
		<category><![CDATA[extinction]]></category>
		<category><![CDATA[galex]]></category>
		<category><![CDATA[herschel]]></category>
		<category><![CDATA[host galaxy]]></category>
		<category><![CDATA[main sequence]]></category>
		<category><![CDATA[o star]]></category>
		<category><![CDATA[orders of magnitude]]></category>
		<category><![CDATA[pac]]></category>
		<category><![CDATA[photometry]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[stellar system]]></category>
		<category><![CDATA[typical star]]></category>
		<category><![CDATA[uv emission]]></category>
		<category><![CDATA[uv source]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/star-formation-in-liner-host-galaxies-at-z0-3-replacement/</guid>
		<description><![CDATA[We present the results of a Herschel-PACS study of a sample of 97 LINERs at redshift z\sim 0.3 selected from the zCOSMOS survey. Of these sources, 34 are detected in a least one PACS band, enabling reliable estimates of the far-infrared L(FIR) luminosities, and a comparison to the FIR luminosities of local LINERs. Many of [...]]]></description>
			<content:encoded><![CDATA[<p>We present the results of a Herschel-PACS study of a sample of 97 LINERs at redshift z\sim 0.3 selected from the zCOSMOS survey. Of these sources, 34 are detected in a least one PACS band, enabling reliable estimates of the far-infrared L(FIR) luminosities, and a comparison to the FIR luminosities of local LINERs. Many of our PACS-detected LINERs are also UV sources detected by Galex. Assuming that the FIR is produced in young dusty star-forming regions, the typical star-formation rates (SFRs) for the host galaxies in our sample is \sim 10 M_Sun yr-1, 1-2 orders of magnitude larger than in many local LINERs. Given stellar masses inferred from optical/NIR photometry of the (unobscured) evolved stellar populations, we find that the entire sample lies close to the star-forming &#8220;main sequence&#8221; for galaxies at redshift 0.3. For young star-forming regions, the H\alpha- and UV-based estimates of the SFRs are much smaller than the FIR-based estimates, by factors \sim 30, even assuming that all of the H\alpha\ emission is produced by O-star ionization rather than by the AGNs. These discrepancies may be due to large (and uncertain) extinctions towards the young stellar systems. Alternatively, the H\alpha\ and UV emissions could be tracing residual star-formation in an older less obscured population with decaying star formation. We also compare L(SF) and L(AGN) in local LINERs and in our sample and comment on the problematic use of several line diagnostic diagrams in cases similar to the sample under study.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/star-formation-in-liner-host-galaxies-at-z0-3-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Constraining neutrino superluminality from searches for sterile neutrino decays [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/constraining-neutrino-superluminality-from-searches-for-sterile-neutrino-decays-replacement-2/</link>
		<comments>http://voxcharta.org/2012/05/21/constraining-neutrino-superluminality-from-searches-for-sterile-neutrino-decays-replacement-2/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:36:10 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absence]]></category>
		<category><![CDATA[cern]]></category>
		<category><![CDATA[energy range]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[opera]]></category>
		<category><![CDATA[pair production]]></category>
		<category><![CDATA[signature]]></category>
		<category><![CDATA[sn1987a]]></category>
		<category><![CDATA[sterile neutrino]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/constraining-neutrino-superluminality-from-searches-for-sterile-neutrino-decays-replacement-2/</guid>
		<description><![CDATA[Superluminal neutrinos are expected to lose energy due to bremstrauhlung. It is dominated by e+e&#8211;pair production if kinematically allowed. The same signature was used in searches for 3-body decays of hypothetical heavy sterile neutrinos. From the absence of these processes in CERN PS191 and CHARM experiments we set upper limits on the neutrino velocity in [...]]]></description>
			<content:encoded><![CDATA[<p>Superluminal neutrinos are expected to lose energy due to bremstrauhlung. It is dominated by e+e&#8211;pair production if kinematically allowed. The same signature was used in searches for 3-body decays of hypothetical heavy sterile neutrinos. From the absence of these processes in CERN PS191 and CHARM experiments we set upper limits on the neutrino velocity in the energy range from 0.2 GeV to 280 GeV. Our limits are well below the neutrino velocity favored by the recent OPERA results. For energy-independent neutrino velocity the limits obtained in this paper are stronger than those coming from ICARUS experiment and observations of Supernova SN1987a.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/constraining-neutrino-superluminality-from-searches-for-sterile-neutrino-decays-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>SN 2006oz: rise of a super-luminous supernova observed by the SDSS-II SN Survey [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/sn-2006oz-rise-of-a-super-luminous-supernova-observed-by-the-sdss-ii-sn-survey-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/sn-2006oz-rise-of-a-super-luminous-supernova-observed-by-the-sdss-ii-sn-survey-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:35:50 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absolute magnitude]]></category>
		<category><![CDATA[absolute peak]]></category>
		<category><![CDATA[body functions]]></category>
		<category><![CDATA[common property]]></category>
		<category><![CDATA[deep imaging]]></category>
		<category><![CDATA[explosion models]]></category>
		<category><![CDATA[host galaxy]]></category>
		<category><![CDATA[light curve]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[magnetar]]></category>
		<category><![CDATA[maximum light]]></category>
		<category><![CDATA[optical spectrum]]></category>
		<category><![CDATA[peak luminosity]]></category>
		<category><![CDATA[photosphere]]></category>
		<category><![CDATA[radioactive decay]]></category>
		<category><![CDATA[rest frame]]></category>
		<category><![CDATA[rise time]]></category>
		<category><![CDATA[sdss]]></category>
		<category><![CDATA[starburst galaxy]]></category>
		<category><![CDATA[u band]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/sn-2006oz-rise-of-a-super-luminous-supernova-observed-by-the-sdss-ii-sn-survey-replacement/</guid>
		<description><![CDATA[We study SN 2006oz, a newly-recognized member of the class of H-poor, super-luminous supernovae. We present multi-color light curves from the SDSS-II SN Survey, that cover the rise time, as well as an optical spectrum that shows that the explosion occurred at z~0.376. We fitted black body functions to estimate the temperature and radius evolution [...]]]></description>
			<content:encoded><![CDATA[<p>We study SN 2006oz, a newly-recognized member of the class of H-poor, super-luminous supernovae. We present multi-color light curves from the SDSS-II SN Survey, that cover the rise time, as well as an optical spectrum that shows that the explosion occurred at z~0.376. We fitted black body functions to estimate the temperature and radius evolution of the photosphere and used the parametrized code SYNOW to model the spectrum. We constructed a bolometric light curve and compared it with explosion models. The very early light curves show a dip in the g- and r-bands and a possible initial cooling phase in the u-band before rising to maximum light. The bolometric light curve shows a precursor plateau with a duration of 6-10 days in the rest-frame. A lower limit of M_u &lt; -21.5 can be placed on the absolute peak luminosity of the SN, while the rise time is constrained to be at least 29 days. During our observations, the emitting sphere doubled its radius to 2&#215;10^15 cm, while the temperature remained hot at 15000 K. As for other similar SNe, the spectrum is best modeled with elements including O II and Mg II, while we tentatively suggest that Fe III might be present. We suggest that the precursor plateau might be related to a recombination wave in a circumstellar medium (CSM) and discuss whether this is a common property of all similar explosions. The subsequent rise can be equally well described by input from a magnetar or by ejecta-CSM interaction, but the models are not well constrained owing to the lack of post-maximum observations, and CSM interaction has difficulties accounting for the precursor plateau self-consistently. Radioactive decay is less likely to be the mechanism that powers the luminosity. The host galaxy, detected in deep imaging with the 10 m GTC, is a moderately young and star-forming, but not a starburst, galaxy. It has an absolute magnitude of M_g = -16.9.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/sn-2006oz-rise-of-a-super-luminous-supernova-observed-by-the-sdss-ii-sn-survey-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Star formation in the early universe: beyond the tip of the iceberg [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/star-formation-in-the-early-universe-beyond-the-tip-of-the-iceberg-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/star-formation-in-the-early-universe-beyond-the-tip-of-the-iceberg-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:35:02 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[early universe]]></category>
		<category><![CDATA[grbs]]></category>
		<category><![CDATA[hubble space telescope]]></category>
		<category><![CDATA[hubble space telescope imaging]]></category>
		<category><![CDATA[space telescope imaging]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[tip of the iceberg]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/star-formation-in-the-early-universe-beyond-the-tip-of-the-iceberg-replacement/</guid>
		<description><![CDATA[We present late-time Hubble Space Telescope imaging of the fields of six Swift GRBs lying at 5.0&#60;z&#60;9.5. Our data includes very deep observations of the field of the most distant spectroscopically confirmed burst, GRB 090423, at z=8.2. Using the precise positions afforded by their afterglows we can place stringent limits on the luminosities of their [...]]]></description>
			<content:encoded><![CDATA[<p>We present late-time Hubble Space Telescope imaging of the fields of six Swift GRBs lying at 5.0&lt;z&lt;9.5. Our data includes very deep observations of the field of the most distant spectroscopically confirmed burst, GRB 090423, at z=8.2. Using the precise positions afforded by their afterglows we can place stringent limits on the luminosities of their host galaxies. In one case, that of GRB 060522 at z=5.11, there is a marginal excess of flux close to the GRB position which may be a detection of a host at a magnitude J(AB)=28.5. None of the others are significantly detected meaning that all the hosts lie below L\star at their respective redshifts, with star formation rates SFR&lt;4Mo/yr in all cases. Indeed, stacking the five fields with WFC3-IR data we conclude a mean SFR90% confidence. Although it is not yet possible to make stronger statements, in the future, with larger samples and a fuller understanding of the conditions required for GRB production, studies like this hold great potential for probing the nature of star formation, the shape of the galaxy luminosity function, and the supply of ionizing photons in the early universe.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/star-formation-in-the-early-universe-beyond-the-tip-of-the-iceberg-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Effective theories of single field inflation when heavy fields matter [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/effective-theories-of-single-field-inflation-when-heavy-fields-matter-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/effective-theories-of-single-field-inflation-when-heavy-fields-matter-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:34:51 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[boson]]></category>
		<category><![CDATA[coupling]]></category>
		<category><![CDATA[degrees of freedom]]></category>
		<category><![CDATA[deviates]]></category>
		<category><![CDATA[eft]]></category>
		<category><![CDATA[field theory]]></category>
		<category><![CDATA[formalism]]></category>
		<category><![CDATA[inflation]]></category>
		<category><![CDATA[invariance]]></category>
		<category><![CDATA[low energy]]></category>
		<category><![CDATA[perturbation]]></category>
		<category><![CDATA[power spectrum]]></category>
		<category><![CDATA[primordial power]]></category>
		<category><![CDATA[scalar field]]></category>
		<category><![CDATA[scenarios]]></category>
		<category><![CDATA[signature]]></category>
		<category><![CDATA[speed of sound]]></category>
		<category><![CDATA[symmetry]]></category>
		<category><![CDATA[trajectory]]></category>
		<category><![CDATA[validity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/effective-theories-of-single-field-inflation-when-heavy-fields-matter-replacement/</guid>
		<description><![CDATA[We compute the low energy effective field theory (EFT) expansion for single-field inflationary models that descend from a parent theory containing multiple other scalar fields. By assuming that all other degrees of freedom in the parent theory are sufficiently massive relative to the inflaton, it is possible to derive an EFT valid to arbitrary order [...]]]></description>
			<content:encoded><![CDATA[<p>We compute the low energy effective field theory (EFT) expansion for single-field inflationary models that descend from a parent theory containing multiple other scalar fields. By assuming that all other degrees of freedom in the parent theory are sufficiently massive relative to the inflaton, it is possible to derive an EFT valid to arbitrary order in perturbations, provided certain generalized adiabaticity conditions are respected. These conditions permit a consistent low energy EFT description even when the inflaton deviates off its adiabatic minimum along its slowly rolling trajectory. By generalizing the formalism that identifies the adiabatic mode with the Goldstone boson of this spontaneously broken time translational symmetry prior to the integration of the heavy fields, we show that this invariance of the parent theory dictates the entire non-perturbative structure of the descendent EFT. The couplings of this theory can be written entirely in terms of the reduced speed of sound of adiabatic perturbations. The resulting operator expansion is distinguishable from that of other scenarios, such as standard single inflation or DBI inflation. In particular, we re-derive how certain operators can become transiently strongly coupled along the inflaton trajectory, consistent with slow-roll and the validity of the EFT expansion, imprinting features in the primordial power spectrum, and we deduce the relevant cubic operators that imply distinct signatures in the primordial bispectrum which may soon be constrained by observations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/effective-theories-of-single-field-inflation-when-heavy-fields-matter-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Acceleration of particles by black holes as a result of deceleration: ultimate manifestation of kinematic nature of BSW effect [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/acceleration-of-particles-by-black-holes-as-a-result-of-deceleration-ultimate-manifestation-of-kinematic-nature-of-bsw-effect-replacement-2/</link>
		<comments>http://voxcharta.org/2012/05/21/acceleration-of-particles-by-black-holes-as-a-result-of-deceleration-ultimate-manifestation-of-kinematic-nature-of-bsw-effect-replacement-2/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:34:40 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[deceleration]]></category>
		<category><![CDATA[horizon surface]]></category>
		<category><![CDATA[manifestation]]></category>
		<category><![CDATA[mass frame]]></category>
		<category><![CDATA[massive particle]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[repulsion]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/acceleration-of-particles-by-black-holes-as-a-result-of-deceleration-ultimate-manifestation-of-kinematic-nature-of-bsw-effect-replacement-2/</guid>
		<description><![CDATA[The recently discovered so-called BSW effect consists in the unbound growth of the energy E_{c.m.} in the centre of mass frame of two colliding particles near the black hole horizon. We consider a new type of the corresponding scenario when one of two particles (&#8220;critical&#8221;) remains at rest near the horizon of the charged near-extremal [...]]]></description>
			<content:encoded><![CDATA[<p>The recently discovered so-called BSW effect consists in the unbound growth of the energy E_{c.m.} in the centre of mass frame of two colliding particles near the black hole horizon. We consider a new type of the corresponding scenario when one of two particles (&#8220;critical&#8221;) remains at rest near the horizon of the charged near-extremal black hole due to balance between the attractive and repulsion forces. The other one hits it with a speed close to that of light. This scenario shows in a most pronounced way the kinematic nature of the BSW effect. In the extremal limit, one would gain formally infinite E_{c.m.} but this does not happen since it would have require the critical massive particle to remain at rest on the null horizon surface that is impossible. We also discuss the BSW effect in the metric of the extremal Reissner-Nordstr\&#8221;om black hole when the critical particle remains at rest near the horizon.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/acceleration-of-particles-by-black-holes-as-a-result-of-deceleration-ultimate-manifestation-of-kinematic-nature-of-bsw-effect-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>The clustering of galaxies as a function of their photometrically-estimated atomic gas content [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/the-clustering-of-galaxies-as-a-function-of-their-photometrically-estimated-atomic-gas-content-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/the-clustering-of-galaxies-as-a-function-of-their-photometrically-estimated-atomic-gas-content-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:34:15 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[atomic gas]]></category>
		<category><![CDATA[gas content]]></category>
		<category><![CDATA[gradient]]></category>
		<category><![CDATA[linear combination]]></category>
		<category><![CDATA[mass density]]></category>
		<category><![CDATA[mass fraction]]></category>
		<category><![CDATA[nearby galaxy]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[stellar surface]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/the-clustering-of-galaxies-as-a-function-of-their-photometrically-estimated-atomic-gas-content-replacement/</guid>
		<description><![CDATA[We introduce a new photometric estimator of the HI mass fraction (M_HI/M_*) in local galaxies, which is a linear combination of four parameters: stellar mass, stellar surface mass density, NUV-r colour, and g-i colour gradient. It is calibrated using samples of nearby galaxies (0.025&#60;z&#60;0.05) with HI line detections from the GASS and ALFALFA surveys, and [...]]]></description>
			<content:encoded><![CDATA[<p>We introduce a new photometric estimator of the HI mass fraction (M_HI/M_*) in local galaxies, which is a linear combination of four parameters: stellar mass, stellar surface mass density, NUV-r colour, and g-i colour gradient. It is calibrated using samples of nearby galaxies (0.025&lt;z&lt;0.05) with HI line detections from the GASS and ALFALFA surveys, and it is demonstrated to provide unbiased M_HI/M_* estimates even for HI-rich galaxies. We apply this estimator to a sample of ~24,000 galaxies from the SDSS/DR7 in the same redshift range. We then bin these galaxies by stellar mass and HI mass fraction and compute projected two point cross-correlation functions with respect to a reference galaxy sample. Results are compared with predictions from current semi-analytic models of galaxy formation. The agreement is good for galaxies with stellar masses larger than 10^10 M_sun, but not for lower mass systems. We then extend the analysis by studying the bias in the clustering of HI-poor or HI-rich galaxies with respect to galaxies with normal HI content on scales between 100 kpc and ~5 Mpc. For the HI-deficient population, the strongest bias effects arise when the HI-deficiency is defined in comparison to galaxies of the same stellar mass and size. This is not reproduced by the semi-analytic models, where the quenching of star formation in satellites occurs by &quot;starvation&quot; and does not depend on their internal structure. HI-rich galaxies with masses greater than 10^10 M_sun are found to be anti-biased compared to galaxies with &quot;normal&quot; HI content. Interestingly, no such effect is found for lower mass galaxies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/the-clustering-of-galaxies-as-a-function-of-their-photometrically-estimated-atomic-gas-content-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The survival of nuclei in jets associated with core-collapse supernovae [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/the-survival-of-nuclei-in-jets-associated-with-core-collapse-supernovae-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/the-survival-of-nuclei-in-jets-associated-with-core-collapse-supernovae-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:33:30 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cocoon]]></category>
		<category><![CDATA[core collapse supernovae]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[jet parameters]]></category>
		<category><![CDATA[jets]]></category>
		<category><![CDATA[launch]]></category>
		<category><![CDATA[lorentz]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[multi messenger]]></category>
		<category><![CDATA[nickel]]></category>
		<category><![CDATA[nuclei]]></category>
		<category><![CDATA[propagation]]></category>
		<category><![CDATA[signal]]></category>
		<category><![CDATA[spallation]]></category>
		<category><![CDATA[stellar material]]></category>
		<category><![CDATA[survival]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/the-survival-of-nuclei-in-jets-associated-with-core-collapse-supernovae-replacement/</guid>
		<description><![CDATA[Heavy nuclei such as nickel-56 are synthesized in a wide range of core-collapse supernovae (CCSN), including energetic supernovae associated with gamma-ray bursts (GRBs). Recent studies suggest that jet-like outflows are a common feature of CCSN. These outflows may entrain synthesized nuclei at launch or during propagation, and provide interesting multi-messenger signals including heavy ultra-high energy [...]]]></description>
			<content:encoded><![CDATA[<p>Heavy nuclei such as nickel-56 are synthesized in a wide range of core-collapse supernovae (CCSN), including energetic supernovae associated with gamma-ray bursts (GRBs). Recent studies suggest that jet-like outflows are a common feature of CCSN. These outflows may entrain synthesized nuclei at launch or during propagation, and provide interesting multi-messenger signals including heavy ultra-high energy cosmic rays. Here, we investigate the destruction processes of nuclei during crossing from the stellar material into the jet material via a cocoon, and during propagation after being successfully loaded into the jet. We find that nuclei can survive for a range of jet parameters because collisional cooling is faster than spallation. While canonical high-luminosity GRB jets may contain nuclei, magnetic dominated models or low-luminosity jets with small bulk Lorentz factors are more favorable for having a more significant heavy nuclei component.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/the-survival-of-nuclei-in-jets-associated-with-core-collapse-supernovae-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Innovative Demodulation Scheme for Coherent Detectors in CMB Experiments [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/innovative-demodulation-scheme-for-coherent-detectors-in-cmb-experiments-replacement-2/</link>
		<comments>http://voxcharta.org/2012/05/21/innovative-demodulation-scheme-for-coherent-detectors-in-cmb-experiments-replacement-2/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:33:12 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cmb experiments]]></category>
		<category><![CDATA[cosmic microwave background]]></category>
		<category><![CDATA[high pass filter]]></category>
		<category><![CDATA[modulation and demodulation]]></category>
		<category><![CDATA[noise floor]]></category>
		<category><![CDATA[numerical differentiation]]></category>
		<category><![CDATA[polarization]]></category>
		<category><![CDATA[signal]]></category>
		<category><![CDATA[significant improvement]]></category>
		<category><![CDATA[suppression]]></category>
		<category><![CDATA[white noise]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/innovative-demodulation-scheme-for-coherent-detectors-in-cmb-experiments-replacement-2/</guid>
		<description><![CDATA[We propose an innovative demodulation scheme for coherent detectors used in cosmic microwave background polarization experiments. Removal of non-white noise, e.g., narrow-band noise, in detectors is one of the key requirements for the experiments. A combination of modulation and demodulation is used to extract polarization signals as well as to suppress such noise. Traditional demodulation, [...]]]></description>
			<content:encoded><![CDATA[<p>We propose an innovative demodulation scheme for coherent detectors used in cosmic microwave background polarization experiments. Removal of non-white noise, e.g., narrow-band noise, in detectors is one of the key requirements for the experiments. A combination of modulation and demodulation is used to extract polarization signals as well as to suppress such noise. Traditional demodulation, which is based on the two- point numerical differentiation, works as a first-order high pass filter for the noise. The proposed demodulation is based on the three-point numerical differentiation. It works as a second-order high pass filter. By using a real detector, we confirmed significant improvements of suppression power for the narrow-band noise. We also found improvement of the noise floor.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/innovative-demodulation-scheme-for-coherent-detectors-in-cmb-experiments-replacement-2/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>
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		<item>
		<title>The Nature of the Compton-thick X-ray Reprocessor in NGC 4945 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/the-nature-of-the-compton-thick-x-ray-reprocessor-in-ngc-4945-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/the-nature-of-the-compton-thick-x-ray-reprocessor-in-ngc-4945-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:32:43 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[agns]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[Chandra]]></category>
		<category><![CDATA[cm 2]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[compton]]></category>
		<category><![CDATA[continuum]]></category>
		<category><![CDATA[eddington luminosity]]></category>
		<category><![CDATA[Fermi]]></category>
		<category><![CDATA[galaxy ngc]]></category>
		<category><![CDATA[line emission]]></category>
		<category><![CDATA[methodology]]></category>
		<category><![CDATA[orders of magnitude]]></category>
		<category><![CDATA[reflection model]]></category>
		<category><![CDATA[restriction]]></category>
		<category><![CDATA[shape]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectrum]]></category>
		<category><![CDATA[variability]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/the-nature-of-the-compton-thick-x-ray-reprocessor-in-ngc-4945-replacement/</guid>
		<description><![CDATA[We present an exhaustive methodology for fitting Compton-thick X-ray reprocessor models to obscured AGNs and for interpreting the results. We focus on the MYTORUS model but also utilize other models. We apply the techniques to Suzaku, BeppoSAX, and Swift BAT spectra of the Sy 2 galaxy NGC 4945, but the methods are applicable to other [...]]]></description>
			<content:encoded><![CDATA[<p>We present an exhaustive methodology for fitting Compton-thick X-ray reprocessor models to obscured AGNs and for interpreting the results. We focus on the MYTORUS model but also utilize other models. We apply the techniques to Suzaku, BeppoSAX, and Swift BAT spectra of the Sy 2 galaxy NGC 4945, but the methods are applicable to other AGNs including Compton-thin sources. The models overcome a major restriction of disk-reflection models, namely the assumption of an infinite column density. Finite column-density models produce a richer variety of spectral shapes and characteristics, even for Compton-thin AGNs. Although NGC 4945 is one of the brightest AGNs above 10 keV, the models span nearly a factor of 3 in column density (~2 to 6 x 10^{24} cm^{-2}) and 2 orders of magnitude in the intrinsic 2-195 keV luminosity. Models in which the continuum above 10 keV is dominated by the direct (unscattered) continuum or Compton-scattered continuum give the highest and lowest intrinsic luminosities respectively. Variability properties favor solutions in which the unscattered continuum dominates above 10 keV. The data require that the Compton-scattered continuum and Fe Kalpha line emission come predominantly from the illuminated surfaces of the X-ray reprocessor, implying a clumpy medium with a global covering factor that is small enough that the Compton-scattered continuum does not dominate the spectrum above 10 keV. This can be identified with the ~30 pc region spatially resolved by Chandra. The implied intrinsic bolometric luminosity is close to, or greater than, the Eddington luminosity. However, a strongly beamed AGN embedded in a shell of Compton-thick (but clumpy) matter requires less fine-tuning of the covering factor. Beaming is consistent with recent radio and Fermi results. Such beamed Compton-thick AGNs would be preferentially selected in surveys over unbeamed Compton-thick AGNs.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/the-nature-of-the-compton-thick-x-ray-reprocessor-in-ngc-4945-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Revisit of the Interaction between Holographic Dark Energy and Dark Matter [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/revisit-of-the-interaction-between-holographic-dark-energy-and-dark-matter-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/revisit-of-the-interaction-between-holographic-dark-energy-and-dark-matter-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:32:33 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cmb data]]></category>
		<category><![CDATA[confidence level]]></category>
		<category><![CDATA[cosmic expansion]]></category>
		<category><![CDATA[cosmological constraints]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[de sitter]]></category>
		<category><![CDATA[decrement]]></category>
		<category><![CDATA[energy flow]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[existence]]></category>
		<category><![CDATA[general model]]></category>
		<category><![CDATA[gravitational interaction]]></category>
		<category><![CDATA[hde]]></category>
		<category><![CDATA[increment]]></category>
		<category><![CDATA[interaction terms]]></category>
		<category><![CDATA[simple models]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/revisit-of-the-interaction-between-holographic-dark-energy-and-dark-matter-replacement/</guid>
		<description><![CDATA[In this paper we investigate the possible direct, non-gravitational interaction between holographic dark energy (HDE) and dark matter. Firstly, we start with two simple models with the interaction terms $Q \propto \rho_{dm}$ and $Q \propto \rho_{de}$, and then we move on to the general form $Q \propto \rho_m^\alpha\rho_{de}^\beta$. The cosmological constraints of the models are [...]]]></description>
			<content:encoded><![CDATA[<p>In this paper we investigate the possible direct, non-gravitational interaction between holographic dark energy (HDE) and dark matter. Firstly, we start with two simple models with the interaction terms $Q \propto \rho_{dm}$ and $Q \propto \rho_{de}$, and then we move on to the general form $Q \propto \rho_m^\alpha\rho_{de}^\beta$. The cosmological constraints of the models are obtained from the joint analysis of the present Union2.1+BAO+CMB+$H_0$ data. We find that the data slightly favor an energy flow from dark matter to dark energy, although the original HDE model still lies in the 95.4% confidence level (CL) region. For all models we find $c&lt;1$ at the 95.4% CL. We show that compared with the cosmic expansion, the effect of interaction on the evolution of $\rho_{dm}$ and $\rho_{de}$ is smaller, and the relative increment (decrement) amount of the energy in the dark matter component is constrained to be less than 9% (15%) at the 95.4% CL. By introducing the interaction, we find that even when $c&lt;1$ the big rip still can be avoided due to the existence of a de Sitter solution at $z\rightarrow-1$. We show that this solution can not be accomplished in the two simple models, while for the general model such a solution can be achieved with a large $\beta$, and the big rip may be avoided at the 95.4% CL.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/revisit-of-the-interaction-between-holographic-dark-energy-and-dark-matter-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Warm Gas in the Virgo Cluster: I. Distribution of Lya Absorbers [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/warm-gas-in-the-virgo-cluster-i-distribution-of-lya-absorbers-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/warm-gas-in-the-virgo-cluster-i-distribution-of-lya-absorbers-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:32:17 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorption]]></category>
		<category><![CDATA[cluster impact]]></category>
		<category><![CDATA[cm 2]]></category>
		<category><![CDATA[cosmological simulations]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[galaxy cluster]]></category>
		<category><![CDATA[ghrs]]></category>
		<category><![CDATA[impact parameter]]></category>
		<category><![CDATA[outskirt]]></category>
		<category><![CDATA[parameter range]]></category>
		<category><![CDATA[probes]]></category>
		<category><![CDATA[qso]]></category>
		<category><![CDATA[stis]]></category>
		<category><![CDATA[strength increase]]></category>
		<category><![CDATA[substructure]]></category>
		<category><![CDATA[systematic study]]></category>
		<category><![CDATA[velocity range]]></category>
		<category><![CDATA[vir]]></category>
		<category><![CDATA[virgo cluster]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/warm-gas-in-the-virgo-cluster-i-distribution-of-lya-absorbers-replacement/</guid>
		<description><![CDATA[The first systematic study of the warm gas (T=10^4-5 K) distribution across a galaxy cluster is presented using multiple background QSOs to the Virgo Cluster. We detect 25 Lya absorbers (N_HI = 10^13.1-15.4 cm^-2) in the Virgo velocity range toward 9 of 12 QSO sightlines observed with COS, with a cluster impact parameter range of [...]]]></description>
			<content:encoded><![CDATA[<p>The first systematic study of the warm gas (T=10^4-5 K) distribution across a galaxy cluster is presented using multiple background QSOs to the Virgo Cluster. We detect 25 Lya absorbers (N_HI = 10^13.1-15.4 cm^-2) in the Virgo velocity range toward 9 of 12 QSO sightlines observed with COS, with a cluster impact parameter range of 0.25-1.15 Mpc (0.23-1.05R_vir). Including 18 Lya absorbers previously detected by STIS or GHRS toward 7 of 11 background QSOs in and around the Virgo Cluster, we establish a sample of 43 absorbers towards a total of 23 background probes for studying the incidence of Lya absorbers in and around the Virgo Cluster. With these absorbers, we find: 1) Warm gas is predominantly in the outskirts of the cluster and avoids the X-ray detected hot ICM. Also, Lya absorption strength increases with a cluster impact parameter. 2) Lya absorbing warm gas traces cold HI emitting gas in the substructures of the Virgo Cluster. 3) Including the absorbers associated with the surrounding substructures, the warm gas covering fraction (100% for N_HI &gt; 10^13.1 cm^-2) is in agreement with cosmological simulations. We speculate that the observed warm gas is part of large-scale gas flows feeding the cluster both the ICM and galaxies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/warm-gas-in-the-virgo-cluster-i-distribution-of-lya-absorbers-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>High energy gamma-ray emission from compact galactic sources in the context of observations with the next generation Cherenkov Telescope Arrays [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/high-energy-gamma-ray-emission-from-compact-galactic-sources-in-the-context-of-observations-with-the-next-generation-cherenkov-telescope-arrays-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/high-energy-gamma-ray-emission-from-compact-galactic-sources-in-the-context-of-observations-with-the-next-generation-cherenkov-telescope-arrays-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:32:03 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[compact object]]></category>
		<category><![CDATA[cta]]></category>
		<category><![CDATA[energetic particle]]></category>
		<category><![CDATA[energy range]]></category>
		<category><![CDATA[galactic sources]]></category>
		<category><![CDATA[gamma ray emission]]></category>
		<category><![CDATA[gev energy]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[hypothesis]]></category>
		<category><![CDATA[observational result]]></category>
		<category><![CDATA[order of magnitude]]></category>
		<category><![CDATA[physical processes]]></category>
		<category><![CDATA[ray astronomy]]></category>
		<category><![CDATA[ray sources]]></category>
		<category><![CDATA[telescope array]]></category>
		<category><![CDATA[telescopes]]></category>
		<category><![CDATA[tev energies]]></category>
		<category><![CDATA[theoretical implications]]></category>
		<category><![CDATA[time resolution]]></category>
		<category><![CDATA[unexpected feature]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/high-energy-gamma-ray-emission-from-compact-galactic-sources-in-the-context-of-observations-with-the-next-generation-cherenkov-telescope-arrays-replacement/</guid>
		<description><![CDATA[The observational progress in the $\gamma$-ray astronomy in the last few years has led to the discovery of more than a thousand sources at GeV energies and more than a hundred sources at TeV energies. A few different classes of compact objects in the Galaxy have been established. They show many unexpected features at high [...]]]></description>
			<content:encoded><![CDATA[<p>The observational progress in the $\gamma$-ray astronomy in the last few years has led to the discovery of more than a thousand sources at GeV energies and more than a hundred sources at TeV energies. A few different classes of compact objects in the Galaxy have been established. They show many unexpected features at high energies the physics of which remains mainly unknown. At present it is clear that detailed investigation of these new phenomena can be performed only with the technical equipment which offer an order of magnitude better sensitivity, and a few times better energy, angular and time resolution in the broad energy range staring from a few tens of GeV up to a few hundreds TeV. Such facilities can be realized by the next generation of instruments such as the planned Cherenkov Telescope Array (CTA).   The aim of this report is to summarize up to date observational results on the compact galactic sources in the GeV-TeV $\gamma$-ray energy range, discuss their theoretical implications, and indicate which hypothesis considered at present might be verified with the next generation of telescopes. We point out which of the observational features of the $\gamma$-ray sources are important to investigate with special care with the planned CTA in order to put a new light on physical processes involved. Their knowledge should finally allow us to answer the question on the origin of energetic particles in our Galaxy.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/high-energy-gamma-ray-emission-from-compact-galactic-sources-in-the-context-of-observations-with-the-next-generation-cherenkov-telescope-arrays-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Planck Intermediate Results. IV. The XMM-Newton validation programme for new Planck clusters [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/planck-intermediate-results-iv-the-xmm-newton-validation-programme-for-new-planck-clusters-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/planck-intermediate-results-iv-the-xmm-newton-validation-programme-for-new-planck-clusters-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:31:48 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[ancillary data]]></category>
		<category><![CDATA[bright source]]></category>
		<category><![CDATA[cluster]]></category>
		<category><![CDATA[cluster candidates]]></category>
		<category><![CDATA[faint source]]></category>
		<category><![CDATA[intermediate results]]></category>
		<category><![CDATA[msun]]></category>
		<category><![CDATA[planck]]></category>
		<category><![CDATA[ras]]></category>
		<category><![CDATA[redshift systems]]></category>
		<category><![CDATA[rosat]]></category>
		<category><![CDATA[signal to noise]]></category>
		<category><![CDATA[signal to noise ratio]]></category>
		<category><![CDATA[sky map]]></category>
		<category><![CDATA[sky survey]]></category>
		<category><![CDATA[source catalogue]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[validation]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xmm newton]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/planck-intermediate-results-iv-the-xmm-newton-validation-programme-for-new-planck-clusters-replacement/</guid>
		<description><![CDATA[We present the final results from the XMM-Newton validation follow-up of new Planck cluster candidates. We observed 15 new candidates, detected with signal-to-noise ratios between 4.0 and 6.1 in the 15.5-month nominal Planck survey. The candidates were selected using ancillary data flags derived from the ROSAT All Sky Survey (RASS) and Digitized Sky Survey all-sky [...]]]></description>
			<content:encoded><![CDATA[<p>We present the final results from the XMM-Newton validation follow-up of new Planck cluster candidates. We observed 15 new candidates, detected with signal-to-noise ratios between 4.0 and 6.1 in the 15.5-month nominal Planck survey. The candidates were selected using ancillary data flags derived from the ROSAT All Sky Survey (RASS) and Digitized Sky Survey all-sky maps, with the aim of pushing into the low SZ flux, high- z regime and testing RASS flags as indicators of candidate reliability. 14 new clusters were detected by XMM-Newton, 10 single clusters and 2 double systems. Redshifts from X-ray spectroscopy lie in the range 0.2 to 0.9, with six clusters at z&gt;0.5. Estimated M500 ranges from 2.5 X 10^14 to 8 X 10^14 Msun. We discuss our results in the context of the full XMM validation programme, in which 51 new clusters have been detected. This includes 4 double and 2 triple systems, some of which are chance projections on the sky of clusters at different redshifts. Association with a source from the RASS-Bright Source Catalogue is a robust indicator of candidate reliability, whereas association with a source from the RASS-Faint Source Catalogue does not guarantee that the SZ candidate is a bona fide cluster. Most Planck clusters appear in RASS maps, with a significance greater than 2 sigma being a good indication of a real cluster. The full sample indicates a Planck sensitivity threshold of Y500 ~ 4 X 10^-4 arcmin^2, with indication for Malmquist bias in the YX-Y500 relation below this level. The corresponding mass threshold depends on redshift. Systems with M500 &gt; 5 X 10^14 Msun at z&gt;0.5 are easily detectable with Planck. The newly-detected clusters follow the YX-Y500 relation derived from X-ray selected samples, with no indication of evolution. Compared to X-ray selected clusters, the new SZ clusters are underluminous on average for their mass, at all redshifts.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/planck-intermediate-results-iv-the-xmm-newton-validation-programme-for-new-planck-clusters-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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		<item>
		<title>Galaxy mass, cluster-centric distance and secular evolution: their role in the evolution of galaxies in clusters in the last 10 Gyr [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/galaxy-mass-cluster-centric-distance-and-secular-evolution-their-role-in-the-evolution-of-galaxies-in-clusters-in-the-last-10-gyr-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/galaxy-mass-cluster-centric-distance-and-secular-evolution-their-role-in-the-evolution-of-galaxies-in-clusters-in-the-last-10-gyr-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:31:22 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cessation]]></category>
		<category><![CDATA[cluster]]></category>
		<category><![CDATA[dependence]]></category>
		<category><![CDATA[diagnosis]]></category>
		<category><![CDATA[differential]]></category>
		<category><![CDATA[differential evolution]]></category>
		<category><![CDATA[epochs]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[galaxy evolution]]></category>
		<category><![CDATA[gyr]]></category>
		<category><![CDATA[key role]]></category>
		<category><![CDATA[photometry]]></category>
		<category><![CDATA[r200]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[sfh]]></category>
		<category><![CDATA[slope]]></category>
		<category><![CDATA[star formation history]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/galaxy-mass-cluster-centric-distance-and-secular-evolution-their-role-in-the-evolution-of-galaxies-in-clusters-in-the-last-10-gyr-replacement/</guid>
		<description><![CDATA[Galaxy mass and environment are known to play a key role in galaxy evolution: looking at galaxy colors at different redshifts, fixed galaxy mass and environment, offers a powerful diagnosis to disentangle the role of each. In this work, we study the simulateneous dependence of the fraction of blue galaxies fblue on secular evolution, environment [...]]]></description>
			<content:encoded><![CDATA[<p>Galaxy mass and environment are known to play a key role in galaxy evolution: looking at galaxy colors at different redshifts, fixed galaxy mass and environment, offers a powerful diagnosis to disentangle the role of each. In this work, we study the simulateneous dependence of the fraction of blue galaxies fblue on secular evolution, environment and galaxy mass with a well-controlled cluster sample. We are thus able to study the evolution and respective role of the cessation of star formation history (SFH) in clusters due to galaxy mass (&#8220;mass quenching&#8221;) or to environment (&#8220;environmental quenching&#8221;). We define an homogenous X-ray selected cluster sample (25 clusters with 0 &lt; z &lt; 1 and one cluster at z \sim 2.2), having similar masses and well-defined sizes. Using multicolor photometry and a large spectroscopic sample to calibrate photometric redshifts, we carefully estimate fblue for each cluster at different galaxy mass and cluster-centric distance bins. We then fit with a simple model the dependence of fblue on redshift (z), environment (r/r200) and galaxy mass (M). fblue increases with cluster-centric distance with a slope $1.2^{+0.4}_{-0.3}$, decreases with galaxy mass with a slope $-3.8^{+0.6}_{-0.5}$, and increases with redshift with a slope $3.2^{+0.7}_{-0.5}$. The data also require for the first time a differential evolution with galaxy mass of fblue with redshift, with lower mass galaxies evolving slower by a factor $-4.1^{+1.1}_{-0.9}$. Our study shows that the processes responsible for the cessation of star formation in clusters are effective at all epochs (z&lt;2.2), and more effective in denser environments and for more massive galaxies. We found that the mass and environmental quenchings are separable, that environmental quenching does not change with epoch, and that mass quenching is a dynamical process, i.e. its evolutionary rate is mass-dependent. [Abridged]</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/galaxy-mass-cluster-centric-distance-and-secular-evolution-their-role-in-the-evolution-of-galaxies-in-clusters-in-the-last-10-gyr-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Observing Black Holes: Quasi-Periodic Oscillations [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/21/observing-black-holes-quasi-periodic-oscillations-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/21/observing-black-holes-quasi-periodic-oscillations-cross-listing/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:31:05 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[angular momentum]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[circular orbit]]></category>
		<category><![CDATA[existence]]></category>
		<category><![CDATA[frequency qpos]]></category>
		<category><![CDATA[fundamental frequency]]></category>
		<category><![CDATA[general relativity]]></category>
		<category><![CDATA[gravity]]></category>
		<category><![CDATA[high frequency]]></category>
		<category><![CDATA[kerr]]></category>
		<category><![CDATA[maxima]]></category>
		<category><![CDATA[numerical analysis]]></category>
		<category><![CDATA[observable effects]]></category>
		<category><![CDATA[orbital frequency]]></category>
		<category><![CDATA[periodic oscillation]]></category>
		<category><![CDATA[qualitative agreement]]></category>
		<category><![CDATA[spacetime geometry]]></category>
		<category><![CDATA[stable orbit]]></category>
		<category><![CDATA[twin peak]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/observing-black-holes-quasi-periodic-oscillations-cross-listing/</guid>
		<description><![CDATA[The twin peaks high-frequency quasiperiodic oscillations (QPOs), which are observed in a number of black hole binaries, can be related to the epicyclic frequencies of the geodesic motion, thereby providing a testing ground for the spacetime geometry near the black holes. In this paper, we explore some observable effects of the geodesic motion in the [...]]]></description>
			<content:encoded><![CDATA[<p>The twin peaks high-frequency quasiperiodic oscillations (QPOs), which are observed in a number of black hole binaries, can be related to the epicyclic frequencies of the geodesic motion, thereby providing a testing ground for the spacetime geometry near the black holes. In this paper, we explore some observable effects of the geodesic motion in the spacetime of rotating black holes in general relativity and braneworld gravity. We focus on the description of the motion in terms of three fundamental frequencies: the orbital frequency, the radial and vertical epicyclic frequencies. For a Kerr black hole, we perform a detailed numerical analysis of these frequencies at the innermost stable circular orbits and beyond them as well as at the characteristic stable orbits, for which the radial epicyclic frequency attains its highest value. We find that the values of the radial and vertical epicyclic frequencies at particular orbits are in good qualitative agreement with the observed frequencies of the twin peaks QPOs in some black hole binaries. It is interesting that at the characteristic stable circular orbits, where the radial epicyclic frequency has maxima, the vertical and radial epicyclic frequencies exhibit an approximate 2 : 1 ratio even in the case of near-extreme rotation of the black hole. We also perform a similar analysis of the fundamental frequencies for a rotating braneworld black hole and argue that the existence of such a black hole with a negative tidal charge, whose angular momentum exceeds the Kerr bound in general relativity, does not confront with the observations of high frequency QPOs.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/observing-black-holes-quasi-periodic-oscillations-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<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>Galaxy mass, cluster-centric distance and secular evolution: their role in the evolution of galaxies in clusters in the last 10 Gyr</title>
		<link>http://voxcharta.org/2012/05/20/galaxy-mass-cluster-centric-distance-and-secular-evolution-their-role-in-the-evolution-of-galaxies-in-clusters-in-the-last-10-gyr/</link>
		<comments>http://voxcharta.org/2012/05/20/galaxy-mass-cluster-centric-distance-and-secular-evolution-their-role-in-the-evolution-of-galaxies-in-clusters-in-the-last-10-gyr/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:45:48 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cessation]]></category>
		<category><![CDATA[cluster]]></category>
		<category><![CDATA[dependence]]></category>
		<category><![CDATA[diagnosis]]></category>
		<category><![CDATA[differential]]></category>
		<category><![CDATA[differential evolution]]></category>
		<category><![CDATA[epochs]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[galaxy evolution]]></category>
		<category><![CDATA[gyr]]></category>
		<category><![CDATA[key role]]></category>
		<category><![CDATA[photometry]]></category>
		<category><![CDATA[r200]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[sfh]]></category>
		<category><![CDATA[slope]]></category>
		<category><![CDATA[star formation history]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/galaxy-mass-cluster-centric-distance-and-secular-evolution-their-role-in-the-evolution-of-galaxies-in-clusters-in-the-last-10-gyr/</guid>
		<description><![CDATA[Galaxy mass and environment are known to play a key role in galaxy evolution: looking at galaxy colors at different redshifts, fixed galaxy mass and environment, offers a powerful diagnosis to disentangle the role of each. In this work, we study the simulateneous dependence of the fraction of blue galaxies fblue on secular evolution, environment [...]]]></description>
			<content:encoded><![CDATA[<p>Galaxy mass and environment are known to play a key role in galaxy evolution: looking at galaxy colors at different redshifts, fixed galaxy mass and environment, offers a powerful diagnosis to disentangle the role of each. In this work, we study the simulateneous dependence of the fraction of blue galaxies fblue on secular evolution, environment and galaxy mass with a well-controlled cluster sample. We are thus able to study the evolution and respective role of the cessation of star formation history (SFH) in clusters due to galaxy mass (&#8220;mass quenching&#8221;) or to environment (&#8220;environmental quenching&#8221;). We define an homogenous X-ray selected cluster sample (25 clusters with 0 &lt; z &lt; 1 and one cluster at z \sim 2.2), having similar masses and well-defined sizes. Using multicolor photometry and a large spectroscopic sample to calibrate photometric redshifts, we carefully estimate fblue for each cluster at different galaxy mass and cluster-centric distance bins. We then fit with a simple model the dependence of fblue on redshift (z), environment (r/r200) and galaxy mass (M). fblue increases with cluster-centric distance with a slope $1.2^{+0.4}_{-0.3}$, decreases with galaxy mass with a slope $-3.8^{+0.6}_{-0.5}$, and increases with redshift with a slope $3.2^{+0.7}_{-0.5}$. The data also require for the first time a differential evolution with galaxy mass of fblue with redshift, with lower mass galaxies evolving slower by a factor $-4.1^{+1.1}_{-0.9}$. Our study shows that the processes responsible for the cessation of star formation in clusters are effective at all epochs (z&lt;2.2), and more effective in denser environments and for more massive galaxies. We found that the mass and environmental quenchings are separable, that environmental quenching does not change with epoch, and that mass quenching is a dynamical process, i.e. its evolutionary rate is mass-dependent. [Abridged]</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/galaxy-mass-cluster-centric-distance-and-secular-evolution-their-role-in-the-evolution-of-galaxies-in-clusters-in-the-last-10-gyr/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<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>
		</item>
		<item>
		<title>Asteroseismology of the open clusters NGC 6791, NGC 6811, and NGC 6819 from nineteen months of Kepler photometry</title>
		<link>http://voxcharta.org/2012/05/20/asteroseismology-of-the-open-clusters-ngc-6791-ngc-6811-and-ngc-6819-from-nineteen-months-of-kepler-photometry/</link>
		<comments>http://voxcharta.org/2012/05/20/asteroseismology-of-the-open-clusters-ngc-6791-ngc-6811-and-ngc-6819-from-nineteen-months-of-kepler-photometry/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:45:06 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[19 months]]></category>
		<category><![CDATA[binaries]]></category>
		<category><![CDATA[blue straggler]]></category>
		<category><![CDATA[clump stars]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[dnu]]></category>
		<category><![CDATA[eff]]></category>
		<category><![CDATA[epsilon]]></category>
		<category><![CDATA[giant branch stars]]></category>
		<category><![CDATA[kepler]]></category>
		<category><![CDATA[linewidth]]></category>
		<category><![CDATA[nasa]]></category>
		<category><![CDATA[open cluster]]></category>
		<category><![CDATA[photometric data]]></category>
		<category><![CDATA[photometry]]></category>
		<category><![CDATA[red giant]]></category>
		<category><![CDATA[separations]]></category>
		<category><![CDATA[space telescope]]></category>
		<category><![CDATA[stellar classification]]></category>
		<category><![CDATA[stellar population]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/asteroseismology-of-the-open-clusters-ngc-6791-ngc-6811-and-ngc-6819-from-nineteen-months-of-kepler-photometry/</guid>
		<description><![CDATA[We studied 115 red giants in the three open clusters NGC 6791, NGC 6811, and NGC 6819, based on photometric data covering more than 19 months with NASA&#8217;s Kepler space telescope. We present the asteroseismic diagrams of the asymptotic parameters \Delta\nu, \delta\nu_01, \delta\nu_02 and \epsilon. When the stellar populations from the clusters are compared, we [...]]]></description>
			<content:encoded><![CDATA[<p>We studied 115 red giants in the three open clusters NGC 6791, NGC 6811, and NGC 6819, based on photometric data covering more than 19 months with NASA&#8217;s Kepler space telescope. We present the asteroseismic diagrams of the asymptotic parameters \Delta\nu, \delta\nu_01, \delta\nu_02 and \epsilon. When the stellar populations from the clusters are compared, we see evidence for a difference in mass of the red giant branch stars, and possibly a difference in structure of the red clump stars, from the small separations \delta\nu_01 and \delta\nu_02. Ensemble \&#8217;echelle diagrams and lower limits to the linewidth of l = 0 modes as a function of Dnu of the clusters NGC 6791 and NGC 6819 are also shown, together with a correlation between the l = 0 ridge width and T_eff. Lastly, we distinguish between red giant branch and red clump stars through the measurement of the period spacing of mixed modes in 53 stars among all the three clusters to verify the stellar classification from the color-magnitude diagram. These seismic results also allow us to identify a number of potentially interesting stars including evolved blue stragglers and binaries, as well as stars in late He-core burning phases.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/asteroseismology-of-the-open-clusters-ngc-6791-ngc-6811-and-ngc-6819-from-nineteen-months-of-kepler-photometry/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Probing ionizing radiation of L&lt;~0.1L* star-forming galaxies at z&gt;~3 with strong lensing</title>
		<link>http://voxcharta.org/2012/05/20/probing-ionizing-radiation-of-l0-1l-star-forming-galaxies-at-z3-with-strong-lensing/</link>
		<comments>http://voxcharta.org/2012/05/20/probing-ionizing-radiation-of-l0-1l-star-forming-galaxies-at-z3-with-strong-lensing/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:44:46 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[advent]]></category>
		<category><![CDATA[characterisation]]></category>
		<category><![CDATA[continuum emission]]></category>
		<category><![CDATA[cross section]]></category>
		<category><![CDATA[fesc]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[galaxy cluster]]></category>
		<category><![CDATA[ionizing radiation]]></category>
		<category><![CDATA[lyman]]></category>
		<category><![CDATA[magnification]]></category>
		<category><![CDATA[monte carlo simulation]]></category>
		<category><![CDATA[observational capabilities]]></category>
		<category><![CDATA[redshift 3]]></category>
		<category><![CDATA[sigma]]></category>
		<category><![CDATA[telescopes]]></category>
		<category><![CDATA[u band]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/probing-ionizing-radiation-of-l0-1l-star-forming-galaxies-at-z3-with-strong-lensing/</guid>
		<description><![CDATA[We show the effectiveness of strong lensing in the characterisation of Lyman continuum emission from faint L~ 3. Past observations of L&#62;~L* galaxies at redshift &#62;~3 have provided upper limits of the average escape fraction of ionising radiation of fesc~5%. Galaxies with relatively high fesc (&#62;10%) seem to be particularly rare at these luminosities, there [...]]]></description>
			<content:encoded><![CDATA[<p>We show the effectiveness of strong lensing in the characterisation of Lyman continuum emission from faint L~ 3. Past observations of L&gt;~L* galaxies at redshift &gt;~3 have provided upper limits of the average escape fraction of ionising radiation of fesc~5%. Galaxies with relatively high fesc (&gt;10%) seem to be particularly rare at these luminosities, there is therefore the need to explore fainter limits. Before the advent of giant ground based telescopes, one viable way to probe fesc down to 0.05-0.15L* is to exploit strong lensing magnification. This is investigated with Monte Carlo simulations that take into account the current observational capabilities. Adopting a lensing cross-section of 10 arcmin^2 within which the magnification is higher than 1 (achievable with about 4-5 galaxy clusters), with a U-band survey depth of 30(30.5) (AB, 1-sigma), it is possible to constrain fesc for z~3 star-forming galaxies down to 15(10)% at 3-sigma for L&lt;0.15L* luminosities. This is particularly interesting if fesc increases at fainter luminosities, as predicted from various HI reionization scenarios and radiation transfer modelling. Ongoing observational programs on galaxy clusters are discussed and offer positive prospects for the future, even though from space the HST/WFC3 instrument represents the only option we have to investigate details of the spatial distribution of the Lyman continuum emission arising from z~2-4 galaxies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/probing-ionizing-radiation-of-l0-1l-star-forming-galaxies-at-z3-with-strong-lensing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Search for cold gas in strong MgII absorbers at 0.5&lt;z&lt;1.5: nature and evolution of 21-cm absorbers</title>
		<link>http://voxcharta.org/2012/05/20/search-for-cold-gas-in-strong-mgii-absorbers-at-0-5z1-5-nature-and-evolution-of-21-cm-absorbers/</link>
		<comments>http://voxcharta.org/2012/05/20/search-for-cold-gas-in-strong-mgii-absorbers-at-0-5z1-5-nature-and-evolution-of-21-cm-absorbers/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:44:34 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cold gas]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/search-for-cold-gas-in-strong-mgii-absorbers-at-0-5z1-5-nature-and-evolution-of-21-cm-absorbers/</guid>
		<description><![CDATA[We report 4 new detections of 21-cm absorption from a systematic search of 21-cm absorption in a sample of 17 strong (Wr(MgII 2796)&#62;1A) intervening MgII absorbers at 0.5&#60;z&#60;1.5. We also present 20-cm milliarcsecond scale maps of 40 quasars having 42 intervening strong MgII absorbers for which we have searched for 21-cm absorption. Combining 21-cm absorption [...]]]></description>
			<content:encoded><![CDATA[<p>We report 4 new detections of 21-cm absorption from a systematic search of 21-cm absorption in a sample of 17 strong (Wr(MgII 2796)&gt;1A) intervening MgII absorbers at 0.5&lt;z&lt;1.5. We also present 20-cm milliarcsecond scale maps of 40 quasars having 42 intervening strong MgII absorbers for which we have searched for 21-cm absorption. Combining 21-cm absorption measurements for 50 strong MgII systems from our surveys with the measurements from literature, we obtain a sample of 85 strong MgII absorbers at 0.5&lt;z&lt;1 and 1.1&lt;z&lt;1.5. We present detailed analysis of this sample, taking into account the effect of the varying 21-cm optical depth sensitivity and covering factor associated with the different quasar sight lines. We find that the 21-cm detection rate is higher towards the quasars with flat or inverted spectral index at cm wavelengths. About 70% of 21-cm detections are towards the quasars with linear size, LS100 km/s are mainly seen towards the quasars with extended radio morphology at arcsecond scales. However, we do not find any correlation between the integrated 21-cm optical depth or DeltaV with the LS measured from the milliarcsecond scale images. All this can be understood if the absorbing gas is patchy with a typical correlation length of ~30-100 pc. We show that within the measurement uncertainty, the 21-cm detection rate in strong MgII systems is constant over 0.5&lt;z&lt;1.5, i.e., over ~30% of the total age of universe. We show that the detection rate can be underestimated by up to a factor 2 if 21-cm optical depths are not corrected for the partial coverage estimated using milliarcsecond scale maps. Since stellar feedback processes are expected to diminish the filling factor of cold neutral medium over 0.5&lt;z&lt;1, this lack of evolution in the 21-cm detection rate in strong MgII absorbers is intriguing. [abridged]</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/search-for-cold-gas-in-strong-mgii-absorbers-at-0-5z1-5-nature-and-evolution-of-21-cm-absorbers/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A New Population of High Redshift, Dusty Lyman-Alpha Emitters and Blobs Discovered by WISE</title>
		<link>http://voxcharta.org/2012/05/20/a-new-population-of-high-redshift-dusty-lyman-alpha-emitters-and-blobs-discovered-by-wise/</link>
		<comments>http://voxcharta.org/2012/05/20/a-new-population-of-high-redshift-dusty-lyman-alpha-emitters-and-blobs-discovered-by-wise/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:44:13 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[alpha emitter]]></category>
		<category><![CDATA[blob]]></category>
		<category><![CDATA[lyman alpha]]></category>
		<category><![CDATA[population]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/a-new-population-of-high-redshift-dusty-lyman-alpha-emitters-and-blobs-discovered-by-wise/</guid>
		<description><![CDATA[We report a new technique to select 1.6&#60;z10^{13-14}L_sun) and warm colors, typically larger than submillimeter-selected galaxies (SMGs) and dust-obscured galaxies (DOGs). These traits are commonly associated with the dust being energized by intense AGN activity. We hypothesize that the combination of spatially extended Lyman-alpha, large amounts of warm IR-luminous dust, and rarity (implying a short-lived [...]]]></description>
			<content:encoded><![CDATA[<p>We report a new technique to select 1.6&lt;z10^{13-14}L_sun) and warm colors, typically larger than submillimeter-selected galaxies (SMGs) and dust-obscured galaxies (DOGs). These traits are commonly associated with the dust being energized by intense AGN activity. We hypothesize that the combination of spatially extended Lyman-alpha, large amounts of warm IR-luminous dust, and rarity (implying a short-lived phase) can be explained if the galaxies are undergoing strong `feedback&#8217; transforming them from an extreme dusty starburst to a QSO.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/a-new-population-of-high-redshift-dusty-lyman-alpha-emitters-and-blobs-discovered-by-wise/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<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>
		</item>
		<item>
		<title>Vortex and spiral instabilities at gap edges in three-dimensional self-gravitating disc-satellite simulations</title>
		<link>http://voxcharta.org/2012/05/20/vortex-and-spiral-instabilities-at-gap-edges-in-three-dimensional-self-gravitating-disc-satellite-simulations/</link>
		<comments>http://voxcharta.org/2012/05/20/vortex-and-spiral-instabilities-at-gap-edges-in-three-dimensional-self-gravitating-disc-satellite-simulations/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:43:41 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[density enhancement]]></category>
		<category><![CDATA[dependence]]></category>
		<category><![CDATA[gap]]></category>
		<category><![CDATA[gravity]]></category>
		<category><![CDATA[instabilities]]></category>
		<category><![CDATA[mach number]]></category>
		<category><![CDATA[maxima]]></category>
		<category><![CDATA[numerical simulation]]></category>
		<category><![CDATA[orbital radius]]></category>
		<category><![CDATA[perturbation]]></category>
		<category><![CDATA[previous results]]></category>
		<category><![CDATA[relative density]]></category>
		<category><![CDATA[satellite simulations]]></category>
		<category><![CDATA[several times]]></category>
		<category><![CDATA[spiral arm]]></category>
		<category><![CDATA[timescale]]></category>
		<category><![CDATA[vertical motion]]></category>
		<category><![CDATA[vertical structure]]></category>
		<category><![CDATA[vortex]]></category>
		<category><![CDATA[vortices]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/vortex-and-spiral-instabilities-at-gap-edges-in-three-dimensional-self-gravitating-disc-satellite-simulations/</guid>
		<description><![CDATA[Numerical simulations of global three-dimensional (3D), self-gravitating discs with a gap opened by an embedded planet are presented. The simulations are customised to examine planetary gap stability. Previous results, obtained by Lin &#38; Papaoizou from two-dimensional (2D) disc models, are reproduced in 3D. These include (i) the development of vortices associated with local vortensity minima [...]]]></description>
			<content:encoded><![CDATA[<p>Numerical simulations of global three-dimensional (3D), self-gravitating discs with a gap opened by an embedded planet are presented. The simulations are customised to examine planetary gap stability. Previous results, obtained by Lin &amp; Papaoizou from two-dimensional (2D) disc models, are reproduced in 3D. These include (i) the development of vortices associated with local vortensity minima at gap edges and their merging on dynamical timescales in weakly self-gravitating discs, (ii) the increased number of vortices as the strength of self-gravity is increased and their resisted merging, and (iii) suppression of the vortex instability and development of global spiral arms associated with local vortensity maxima in massive discs. The vertical structure of these disturbances are examined. In terms of the relative density perturbation, the vortex disturbance has weak vertical dependence when self-gravity is neglected. Vortices become more vertically stratified with increasing self-gravity. This effect is seen even when the unperturbed region around the planet&#8217;s orbital radius has a Toomre stability parameter ~10. The spiral modes display significant vertical structure at the gap edge, with the midplane density enhancement being several times larger than that near the upper disc boundary. However, for both instabilities the vertical Mach number is typically a few per cent,and on average vertical motions near the gap edge do not dominate horizontal motions.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/vortex-and-spiral-instabilities-at-gap-edges-in-three-dimensional-self-gravitating-disc-satellite-simulations/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Resolved [CII] emission in a lensed quasar at z=4.4</title>
		<link>http://voxcharta.org/2012/05/20/resolved-cii-emission-in-a-lensed-quasar-at-z4-4/</link>
		<comments>http://voxcharta.org/2012/05/20/resolved-cii-emission-in-a-lensed-quasar-at-z4-4/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:43:27 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[cii]]></category>
		<category><![CDATA[compact region]]></category>
		<category><![CDATA[companion disk]]></category>
		<category><![CDATA[disk galaxy]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[host galaxy]]></category>
		<category><![CDATA[iram]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[lensed quasar]]></category>
		<category><![CDATA[map]]></category>
		<category><![CDATA[quasar images]]></category>
		<category><![CDATA[quasar nucleus]]></category>
		<category><![CDATA[receivers]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[rotation field]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[stellar medium]]></category>
		<category><![CDATA[surface density]]></category>
		<category><![CDATA[vicinity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/resolved-cii-emission-in-a-lensed-quasar-at-z4-4/</guid>
		<description><![CDATA[We present one of the first resolved maps of the [CII] 158 micron line, a powerful tracer of the star forming inter-stellar medium, at high redshift. We use the new IRAM PdBI receivers at 350 GHz to map this line in BRI 0952-0115, the host galaxy of a lensed quasar at z=4.4 previously found to [...]]]></description>
			<content:encoded><![CDATA[<p>We present one of the first resolved maps of the [CII] 158 micron line, a powerful tracer of the star forming inter-stellar medium, at high redshift. We use the new IRAM PdBI receivers at 350 GHz to map this line in BRI 0952-0115, the host galaxy of a lensed quasar at z=4.4 previously found to be very bright in [CII] emission. The [CII] emission is clearly resolved and our data allow us to resolve two [CII] lensed images associated with the optical quasar images. We find that the star formation, as traced by [CII], is distributed over a region of ~ 1 kpc in size near the quasar nucleus, and we infer a star formation surface density &gt;150 Msun/yr/kpc^2, similar to that observed in local ULIRGs. We also reveal another [CII] component, extended over ~ 12 kpc, and located at ~ 10 kpc from the quasar. We suggest that this component is a companion disk galaxy, in the process of merging with the quasar host, whose rotation field is distorted by the interaction with the quasar host, and where star formation, although intense, is more diffuse. These observations suggest that galaxy merging at high-z can enhance star formation at the same time in the form of more compact regions, in the vicinity of the accreting black hole, and in more extended star forming galaxies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/resolved-cii-emission-in-a-lensed-quasar-at-z4-4/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The optically unbiased GRB host (TOUGH) survey. V. VLT/X-shooter emission-line redshifts for Swift GRBs at z~2</title>
		<link>http://voxcharta.org/2012/05/20/the-optically-unbiased-grb-host-tough-survey-v-vltx-shooter-emission-line-redshifts-for-swift-grbs-at-z2/</link>
		<comments>http://voxcharta.org/2012/05/20/the-optically-unbiased-grb-host-tough-survey-v-vltx-shooter-emission-line-redshifts-for-swift-grbs-at-z2/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:43:14 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[aim]]></category>
		<category><![CDATA[bia]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[completeness]]></category>
		<category><![CDATA[darkness]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[faint star]]></category>
		<category><![CDATA[grbs]]></category>
		<category><![CDATA[host galaxy]]></category>
		<category><![CDATA[hosts]]></category>
		<category><![CDATA[nir spectroscopy]]></category>
		<category><![CDATA[optical afterglow]]></category>
		<category><![CDATA[prototype]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[redshift galaxies]]></category>
		<category><![CDATA[shooter]]></category>
		<category><![CDATA[swift]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/the-optically-unbiased-grb-host-tough-survey-v-vltx-shooter-emission-line-redshifts-for-swift-grbs-at-z2/</guid>
		<description><![CDATA[We present simultaneous optical and near-infrared (NIR) spectroscopy of 19 Swift GRB host galaxies with VLT/X-shooter with the aim of measuring their redshifts. Galaxies were selected from The Optically Unbiased GRB Host (TOUGH) survey (15 of the 19 galaxies) or because they hosted GRBs without a bright optical afterglow. Here, we provide emission-line redshifts for [...]]]></description>
			<content:encoded><![CDATA[<p>We present simultaneous optical and near-infrared (NIR) spectroscopy of 19 Swift GRB host galaxies with VLT/X-shooter with the aim of measuring their redshifts. Galaxies were selected from The Optically Unbiased GRB Host (TOUGH) survey (15 of the 19 galaxies) or because they hosted GRBs without a bright optical afterglow. Here, we provide emission-line redshifts for 13 of the observed galaxies with brightnesses between F606W &gt; 27 mag and R=22.9 mag (median R=24.6 mag). The median redshift is z=2.1 for all, and z=2.3 for the TOUGH hosts. Our new data significantly improve the redshift completeness of the TOUGH survey, which now stands at 77% (53 out of 69 GRBs). They furthermore provide accurate redshifts for eight prototype-dark GRBs (e.g., GRBs 071021 at z=2.452 and 080207 at z=2.086), which are exemplary of GRBs where redshifts are challenging to obtain via afterglow spectroscopy. This establishes X-shooter spectroscopy as an efficient tool for redshift determination of faint, star-forming, high-redshift galaxies such as GRB hosts. It is hence a further step towards removing the bias in GRB samples that is caused by optically-dark events, and provides the basis for a better understanding of the conditions in which GRBs form. The distribution of column densities as measured from X-ray data (N_{H,X}), for example, is closely related to the darkness of the afterglow and skewed towards low N_{H, X} values in samples that are dominated by bursts with bright optical afterglows.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/the-optically-unbiased-grb-host-tough-survey-v-vltx-shooter-emission-line-redshifts-for-swift-grbs-at-z2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Empirical Constraints of Super-Galactic Winds at z &gt;= 0.5</title>
		<link>http://voxcharta.org/2012/05/20/empirical-constraints-of-super-galactic-winds-at-z-0-5/</link>
		<comments>http://voxcharta.org/2012/05/20/empirical-constraints-of-super-galactic-winds-at-z-0-5/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:42:06 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorption feature]]></category>
		<category><![CDATA[angle theta]]></category>
		<category><![CDATA[clump]]></category>
		<category><![CDATA[disk galaxy]]></category>
		<category><![CDATA[doublet]]></category>
		<category><![CDATA[energy input]]></category>
		<category><![CDATA[galactic wind]]></category>
		<category><![CDATA[hst image]]></category>
		<category><![CDATA[impact parameter]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[minor axis]]></category>
		<category><![CDATA[orientation angles]]></category>
		<category><![CDATA[parameter space]]></category>
		<category><![CDATA[public archive]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[relative motion]]></category>
		<category><![CDATA[super star clusters]]></category>
		<category><![CDATA[supernova explosion]]></category>
		<category><![CDATA[thermal energy]]></category>
		<category><![CDATA[velocity field]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/empirical-constraints-of-super-galactic-winds-at-z-0-5/</guid>
		<description><![CDATA[(Abridged) Under the hypothesis that MgII absorbers found near the minor axis of a galaxy originate in the cool phase of winds, we carry out a study to constrain the properties of large-scale outflows at redshift z &#62;= 0.5 based on the observed relative motions of individual absorbing clouds with respect to the positions and [...]]]></description>
			<content:encoded><![CDATA[<p>(Abridged) Under the hypothesis that MgII absorbers found near the minor axis of a galaxy originate in the cool phase of winds, we carry out a study to constrain the properties of large-scale outflows at redshift z &gt;= 0.5 based on the observed relative motions of individual absorbing clouds with respect to the positions and orientations of the galaxies. We identify in the literature four highly inclined disk galaxies located within 50 kpc and with the minor axis oriented within 45 degrees of a background QSO sightline. Deep HST images of the galaxies are available for accurate morphologies of the galaxies. Echelle spectra of the QSO members are also available in public archives for resolving the velocity field of individual absorption clumps. Three galaxies in our sample are located at rho=8-34 kpc and exhibit strong associated MgII absorption feature with Wr(2796) &gt;= 0.8 {\AA}. One galaxy, located at an impact parameters rho=48 kpc, does not show an associated MgII absorber to a 3-sigma limit of Wr(2796)=0.01{\AA}. Combining known inclination and orientation angles of the star-forming disks, and resolved absorption profiles of the associated absorbers at rho &lt; 35 kpc, we explore the parameter space for the opening angle theta_0 and the velocity field of large-scale galactic outflows as a function of z-height, v(z). We find that the absorption profiles of the MgII doublets and FeII series are compatible with the gas being either accelerated or decelerated, depending on theta_0, though accelerated outflows are valid only for a narrow range of theta_0. Under an acceleration scenario, we compare the derived $v(z)$ with predictions from Murray et al. (2011) and find that if the gas is being accelerateted by the radiation and ram pressure forces from super star clusters, then the efficiency of thermal energy input from a supernova explosion is epsilon &lt;= 0.01.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/empirical-constraints-of-super-galactic-winds-at-z-0-5/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<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>
		</item>
		<item>
		<title>A Spitzer IRAC Measure of the Zodiacal Light</title>
		<link>http://voxcharta.org/2012/05/20/a-spitzer-irac-measure-of-the-zodiacal-light/</link>
		<comments>http://voxcharta.org/2012/05/20/a-spitzer-irac-measure-of-the-zodiacal-light/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:41:11 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accurate knowledge]]></category>
		<category><![CDATA[background source]]></category>
		<category><![CDATA[brightness level]]></category>
		<category><![CDATA[cosmic background explorer]]></category>
		<category><![CDATA[cosmic infrared background]]></category>
		<category><![CDATA[dust cloud]]></category>
		<category><![CDATA[dust disk]]></category>
		<category><![CDATA[galactic astronomy]]></category>
		<category><![CDATA[infrared array camera]]></category>
		<category><![CDATA[infrared background experiment]]></category>
		<category><![CDATA[instrument calibration]]></category>
		<category><![CDATA[instrumental background]]></category>
		<category><![CDATA[interplanetary dust]]></category>
		<category><![CDATA[kelsall]]></category>
		<category><![CDATA[light model]]></category>
		<category><![CDATA[north ecliptic pole]]></category>
		<category><![CDATA[percent discrepancy]]></category>
		<category><![CDATA[sinusoidal variation]]></category>
		<category><![CDATA[zodiacal light]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/a-spitzer-irac-measure-of-the-zodiacal-light/</guid>
		<description><![CDATA[The dominant non-instrumental background source for space-based infrared observatories is the zo- diacal light. We present Spitzer Infrared Array Camera (IRAC) measurements of the zodiacal light at 3.6, 4.5, 5.8, and 8.0 {\mu}m, taken as part of the instrument calibrations. We measure the changing surface brightness levels in approximately weekly IRAC observations near the north [...]]]></description>
			<content:encoded><![CDATA[<p>The dominant non-instrumental background source for space-based infrared observatories is the zo- diacal light. We present Spitzer Infrared Array Camera (IRAC) measurements of the zodiacal light at 3.6, 4.5, 5.8, and 8.0 {\mu}m, taken as part of the instrument calibrations. We measure the changing surface brightness levels in approximately weekly IRAC observations near the north ecliptic pole (NEP) over the period of roughly 8.5 years. This long time baseline is crucial for measuring the annual sinusoidal variation in the signal levels due to the tilt of the dust disk with respect to the ecliptic, which is the true signal of the zodiacal light. This is compared to both Cosmic Background Explorer Diffuse Infrared Background Experiment (COBE DIRBE) data and a zodiacal light model based thereon. Our data show a few percent discrepancy from the Kelsall et al. (1998) model including a potential warping of the interplanetary dust disk and a previously detected overdensity in the dust cloud directly behind the Earth in its orbit. Accurate knowledge of the zodiacal light is important for both extragalactic and Galactic astronomy including measurements of the cosmic infrared background, absolute measures of extended sources, and comparison to extrasolar interplanetary dust models. IRAC data can be used to further inform and test future zodiacal light models.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/a-spitzer-irac-measure-of-the-zodiacal-light/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>An Interface for the Virtual Observatory of the University of Guanajuato</title>
		<link>http://voxcharta.org/2012/05/20/an-interface-for-the-virtual-observatory-of-the-university-of-guanajuato/</link>
		<comments>http://voxcharta.org/2012/05/20/an-interface-for-the-virtual-observatory-of-the-university-of-guanajuato/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:40:57 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[attempts]]></category>
		<category><![CDATA[data tables]]></category>
		<category><![CDATA[database managers]]></category>
		<category><![CDATA[interface]]></category>
		<category><![CDATA[php scripts]]></category>
		<category><![CDATA[phpmyadmin]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[sql database]]></category>
		<category><![CDATA[starlight]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[synthesis]]></category>
		<category><![CDATA[technical parameters]]></category>
		<category><![CDATA[ufsc]]></category>
		<category><![CDATA[university of guanajuato]]></category>
		<category><![CDATA[virtual observatory]]></category>
		<category><![CDATA[web front]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/an-interface-for-the-virtual-observatory-of-the-university-of-guanajuato/</guid>
		<description><![CDATA[We present the first attempts to build a user-friendly interface for the Virtual Observatory of the University of Guanajuato. The data tables will be accessible to the public through PHP scripts and SQL database managers, such as MySQL and PostgreSQL, all administrated through phpMyAdmin and pgMyAdmin. Although it is not made public yet, this interface [...]]]></description>
			<content:encoded><![CDATA[<p>We present the first attempts to build a user-friendly interface for the Virtual Observatory of the University of Guanajuato. The data tables will be accessible to the public through PHP scripts and SQL database managers, such as MySQL and PostgreSQL, all administrated through phpMyAdmin and pgMyAdmin. Although it is not made public yet, this interface will be the basis upon which the final front end for our VO will be built. Furthermore, we present a preliminary version of a web front end to the publicly available stellar population synthesis code STARLIGHT (starlight.ufsc.br) which will be made available with our VO. This front end aims to provide an easy and flexible access to the code itself, letting users fit their own observed spectra with their preferred combination of physical and technical parameters, rather than making available only the results of fitting a specific sample of spectra with predefined parameters.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/an-interface-for-the-virtual-observatory-of-the-university-of-guanajuato/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Cosmological solution of Machian gravity [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/20/cosmological-solution-of-machian-gravity-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/20/cosmological-solution-of-machian-gravity-cross-listing/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:40:43 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[alternate model]]></category>
		<category><![CDATA[correct solution]]></category>
		<category><![CDATA[cosmological model]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[dark matter and dark energy]]></category>
		<category><![CDATA[dimensional model]]></category>
		<category><![CDATA[dimensional space]]></category>
		<category><![CDATA[energy component]]></category>
		<category><![CDATA[field equation]]></category>
		<category><![CDATA[forms of matter]]></category>
		<category><![CDATA[general theory of relativity]]></category>
		<category><![CDATA[geometry]]></category>
		<category><![CDATA[gravity model]]></category>
		<category><![CDATA[mathematical terms]]></category>
		<category><![CDATA[matter and energy]]></category>
		<category><![CDATA[observational evidence]]></category>
		<category><![CDATA[real matter]]></category>
		<category><![CDATA[space time]]></category>
		<category><![CDATA[standard model]]></category>
		<category><![CDATA[theory of relativity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/cosmological-solution-of-machian-gravity-cross-listing/</guid>
		<description><![CDATA[The standard model of cosmology predicts that more than 95% matter in the universe consists of dark components namely dark matter and dark energy. In spite of several attempts to measure these components, there is not a single direct observational evidence for these components till date. Hence, different alternate models of cosmology have been put [...]]]></description>
			<content:encoded><![CDATA[<p>The standard model of cosmology predicts that more than 95% matter in the universe consists of dark components namely dark matter and dark energy. In spite of several attempts to measure these components, there is not a single direct observational evidence for these components till date. Hence, different alternate models of cosmology have been put forward by different authors. However, most of these models have their own problems. Therefore, in this paper, a new cosmological model has been proposed. This model is based on the Machian gravity model, which will be discussed in detail in a later paper. The model can provide an exactly similar cosmology as that of the standard cosmological model without demanding any ad-hoc dark matter or dark energy components. The paper shows that when the field equations from Machian gravity (a 5 dimensional model) are projected to the 4-dimensional space-time, some new mathematical terms arise in the equations that behave exactly like dark matter and dark energy. These mathematical terms come completely from the geometry of the universe and therefore these do not have any connection with the real matter. As the General theory of Relativity does not follow Mach&#8217;s principle, the FLRW model that is based on GR, cannot provide the correct solution to the cosmological model and demands extra forms of matter and energy to give any predictions consistent with the observations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/cosmological-solution-of-machian-gravity-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The sizes, masses and specific star-formation rates of massive galaxies at 1.3&lt;z&lt;1.5: strong evidence in favour of evolution via minor mergers</title>
		<link>http://voxcharta.org/2012/05/20/the-sizes-masses-and-specific-star-formation-rates-of-massive-galaxies-at-1-3z1-5-strong-evidence-in-favour-of-evolution-via-minor-mergers/</link>
		<comments>http://voxcharta.org/2012/05/20/the-sizes-masses-and-specific-star-formation-rates-of-massive-galaxies-at-1-3z1-5-strong-evidence-in-favour-of-evolution-via-minor-mergers/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:40:32 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[massive galaxy]]></category>
		<category><![CDATA[star formation rate]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/the-sizes-masses-and-specific-star-formation-rates-of-massive-galaxies-at-1-3z1-5-strong-evidence-in-favour-of-evolution-via-minor-mergers/</guid>
		<description><![CDATA[We report the results of a comprehensive study of the relationship between galaxy size, stellar mass and specific star-formation rate (sSFR) at redshifts 1.3&#60;z= 6&#215;10^10 Msun), spectroscopic sample from the UKIDSS Ultra-deep Survey (UDS), with accurate stellar-mass measurements derived from spectro photometric fitting, we find that at z~1.4 the location of massive galaxies on the [...]]]></description>
			<content:encoded><![CDATA[<p>We report the results of a comprehensive study of the relationship between galaxy size, stellar mass and specific star-formation rate (sSFR) at redshifts 1.3&lt;z= 6&#215;10^10 Msun), spectroscopic sample from the UKIDSS Ultra-deep Survey (UDS), with accurate stellar-mass measurements derived from spectro photometric fitting, we find that at z~1.4 the location of massive galaxies on the size-mass plane is determined primarily by their sSFR. At this epoch we find that massive galaxies which are passive (sSFR &lt;= 0.1 Gyr^-1) follow a tight size-mass relation, with half-light radii a factor f=2.4+/-0.2 smaller than their local counterparts. Moreover, amongst the passive sub-sample we find no evidence that the off-set from the local size-mass relation is a function of stellar population age. Based on a sub-sample with dynamical mass estimates we also derive an independent estimate of f=2.3+/-0.3 for the typical growth in half-light radius between z~1.4 and the present day. Focusing on the passive sub-sample, we conclude that to produce the necessary evolution predominantly via major mergers would require an unfeasible number of merger events and over populate the high-mass end of the local stellar mass function. In contrast, we find that a scenario in which mass accretion is dominated by minor mergers can produce the necessary evolution, whereby an increase in stellar mass by a factor of ~2, accompanied by an increase in size by a factor of ~3.5, is sufficient to reconcile the size-mass relation at z~1.4 with that observed locally. Finally, we note that a significant fraction (44+/-12%) of the passive galaxies in our sample have a disk-like morphology, providing additional evidence that separate physical processes are responsible for the quenching of star-formation and the morphological transformation of massive galaxies (abridged).</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/the-sizes-masses-and-specific-star-formation-rates-of-massive-galaxies-at-1-3z1-5-strong-evidence-in-favour-of-evolution-via-minor-mergers/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Does the Sun work as a nuclear fusion amplifier of planetary tidal forcing? A proposal for a physical mechanism based on the mass-luminosity relation</title>
		<link>http://voxcharta.org/2012/05/20/does-the-sun-work-as-a-nuclear-fusion-amplifier-of-planetary-tidal-forcing-a-proposal-for-a-physical-mechanism-based-on-the-mass-luminosity-relation/</link>
		<comments>http://voxcharta.org/2012/05/20/does-the-sun-work-as-a-nuclear-fusion-amplifier-of-planetary-tidal-forcing-a-proposal-for-a-physical-mechanism-based-on-the-mass-luminosity-relation/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:40:16 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[amplification factor]]></category>
		<category><![CDATA[classical physics]]></category>
		<category><![CDATA[conversion factor]]></category>
		<category><![CDATA[dynamo processes]]></category>
		<category><![CDATA[fusion rate]]></category>
		<category><![CDATA[gravitational potential energy]]></category>
		<category><![CDATA[magnification factor]]></category>
		<category><![CDATA[mercury and venus]]></category>
		<category><![CDATA[nuclear fusion]]></category>
		<category><![CDATA[orbital period]]></category>
		<category><![CDATA[physical mechanism]]></category>
		<category><![CDATA[solar activity]]></category>
		<category><![CDATA[solar core]]></category>
		<category><![CDATA[solar cycle]]></category>
		<category><![CDATA[solar dynamo]]></category>
		<category><![CDATA[solar luminosity]]></category>
		<category><![CDATA[sun work]]></category>
		<category><![CDATA[sunspot number]]></category>
		<category><![CDATA[tidal energy]]></category>
		<category><![CDATA[venus earth]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/does-the-sun-work-as-a-nuclear-fusion-amplifier-of-planetary-tidal-forcing-a-proposal-for-a-physical-mechanism-based-on-the-mass-luminosity-relation/</guid>
		<description><![CDATA[Empirical evidences show that planetary tides may influence solar activity: 1) the 11-yr Schwabe sunspot number cycle is constrained between the spring tidal period of Jupiter and Saturn, 9.93 yr, and the tidal orbital period of Jupiter, 11.86 yr, and a model based on these cycles reconstructs solar dynamics at multiple time ; 2) a [...]]]></description>
			<content:encoded><![CDATA[<p>Empirical evidences show that planetary tides may influence solar activity: 1) the 11-yr Schwabe sunspot number cycle is constrained between the spring tidal period of Jupiter and Saturn, 9.93 yr, and the tidal orbital period of Jupiter, 11.86 yr, and a model based on these cycles reconstructs solar dynamics at multiple time ; 2) a measure of the alignment of Venus, Earth and Jupiter reveals quasi 11.07-yr cycles well correlated to the 11-year Schwabe solar cycles; 3) there exists a 11.08 yr cyclical recurrence in the solar jerk-shock vector, which is induced mostly by Mercury and Venus. However, Newtonian classical physics fails to explain the phenomenon. Only by means of a significant nuclear fusion amplification of the tidal gravitational potential energy released in the Sun, may planetary tides produce irradiance output oscillations with a sufficient magnitude to influence solar dynamo processes. Here we use an adaptation of the well-known mass-luminosity relation to calculate a conversion factor between the solar luminosity and the potential gravitational power associated to the mass lost by nuclear fusion: the average estimated amplification factor is A=4,250,000. We use this magnification factor to evaluate the theoretical luminosity oscillations that planetary tides may potentially stimulate inside the solar core by making its nuclear fusion rate oscillate. By converting the power related to this energy into solar irradiance units at 1 AU we find that the tidal oscillations may be able to theoretically induce an oscillating luminosity increase from 0.05-0.65 $W/m^{2}$ to 0.25-1.63 $W/m^{2}$, which is a range compatible with the ACRIM satellite observed total solar irradiance fluctuations. In conclusion, the Sun, by means of its nuclear active core, may be working as a great amplifier of the small planetary tidal energy dissipated in it.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/does-the-sun-work-as-a-nuclear-fusion-amplifier-of-planetary-tidal-forcing-a-proposal-for-a-physical-mechanism-based-on-the-mass-luminosity-relation/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Medium modification of the charged current neutrino opacity and its implications</title>
		<link>http://voxcharta.org/2012/05/20/medium-modification-of-the-charged-current-neutrino-opacity-and-its-implications/</link>
		<comments>http://voxcharta.org/2012/05/20/medium-modification-of-the-charged-current-neutrino-opacity-and-its-implications/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:39:50 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[antineutrino]]></category>
		<category><![CDATA[boltzmann equation]]></category>
		<category><![CDATA[closer to one]]></category>
		<category><![CDATA[collisional]]></category>
		<category><![CDATA[cross section]]></category>
		<category><![CDATA[driven wind]]></category>
		<category><![CDATA[electron neutrino]]></category>
		<category><![CDATA[interaction rate]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[neutrino interaction]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[nucleon]]></category>
		<category><![CDATA[nucleosynthesis]]></category>
		<category><![CDATA[opacity]]></category>
		<category><![CDATA[particle energy]]></category>
		<category><![CDATA[period of time]]></category>
		<category><![CDATA[proto]]></category>
		<category><![CDATA[proton]]></category>
		<category><![CDATA[symmetry]]></category>
		<category><![CDATA[vector]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/medium-modification-of-the-charged-current-neutrino-opacity-and-its-implications/</guid>
		<description><![CDATA[Previous work on neutrino emission from proto-neutron stars which employed full solutions of the Boltzmann equation showed that the average energies of emitted electron neutrinos and antineutrinos are closer to one another than predicted by older, more approximate work. This in turn implied that the neutrino driven wind is proton rich during its entire life, [...]]]></description>
			<content:encoded><![CDATA[<p>Previous work on neutrino emission from proto-neutron stars which employed full solutions of the Boltzmann equation showed that the average energies of emitted electron neutrinos and antineutrinos are closer to one another than predicted by older, more approximate work. This in turn implied that the neutrino driven wind is proton rich during its entire life, precluding $r$-process nucleosynthesis and the synthesis of Sr, Y, and Zr. This work relied on charged current neutrino interaction rates that are appropriate for a free nucleon gas. Here, it is shown in detail that the inclusion of the nucleon potential energies and collisional broadening of the response significantly alters this conclusion. Iso-vector interactions, which give rise to the nuclear symmetry energy, produce a difference between neutron and proton single-particle energies $\Delta U=U_n-U_p$ and alter the kinematics of the charged current reaction. In neutron-rich matter, and for a given neutrino/antineutrino energy, the rate for $\nu_e+n\rightarrow e^-+p$ is enhanced while $ \bar{\nu}_e+p\rightarrow n+e^+$ is suppressed because the $Q$ value for these reactions is altered by $\pm\Delta U$, respectively. Collisional broadening acts to enhance both $\nu_e$ and $\bar{\nu}_e$ cross-sections, but mean field shifts have a larger effect. Therefore, electron neutrinos decouple at lower temperature than when the nucleons are assumed to be free and have lower average energies. The change is large enough to allow for a reasonable period of time when the neutrino driven wind is predicted to be neutron rich. It is also shown that the electron fraction in the wind is influenced by the nuclear symmetry energy.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/medium-modification-of-the-charged-current-neutrino-opacity-and-its-implications/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Age and helium content of the open cluster NGC 6791 from multiple eclipsing binary members. II. age dependencies and new insights</title>
		<link>http://voxcharta.org/2012/05/20/age-and-helium-content-of-the-open-cluster-ngc-6791-from-multiple-eclipsing-binary-members-ii-age-dependencies-and-new-insights/</link>
		<comments>http://voxcharta.org/2012/05/20/age-and-helium-content-of-the-open-cluster-ngc-6791-from-multiple-eclipsing-binary-members-ii-age-dependencies-and-new-insights/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:39:36 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accuracy and precision]]></category>
		<category><![CDATA[binary star]]></category>
		<category><![CDATA[cluster ngc]]></category>
		<category><![CDATA[cluster stars]]></category>
		<category><![CDATA[consistency check]]></category>
		<category><![CDATA[eclipsing binary]]></category>
		<category><![CDATA[gyr]]></category>
		<category><![CDATA[helium content]]></category>
		<category><![CDATA[helium mass]]></category>
		<category><![CDATA[mass fraction]]></category>
		<category><![CDATA[mass loss]]></category>
		<category><![CDATA[model comparison]]></category>
		<category><![CDATA[new insights]]></category>
		<category><![CDATA[observational constraints]]></category>
		<category><![CDATA[open cluster]]></category>
		<category><![CDATA[stellar model]]></category>
		<category><![CDATA[stellar structure]]></category>
		<category><![CDATA[stellar system]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/age-and-helium-content-of-the-open-cluster-ngc-6791-from-multiple-eclipsing-binary-members-ii-age-dependencies-and-new-insights/</guid>
		<description><![CDATA[Models of stellar structure and evolution can be constrained by measuring accurate parameters of detached eclipsing binaries in open clusters. Multiple binary stars provide the means to determine helium abundances in these old stellar systems, and in turn, to improve estimates of their age. In the first paper of this series, we demonstrated how measurements [...]]]></description>
			<content:encoded><![CDATA[<p>Models of stellar structure and evolution can be constrained by measuring accurate parameters of detached eclipsing binaries in open clusters. Multiple binary stars provide the means to determine helium abundances in these old stellar systems, and in turn, to improve estimates of their age. In the first paper of this series, we demonstrated how measurements of multiple eclipsing binaries in the old open cluster NGC6791 sets tighter constraints on the properties of stellar models than has previously been possible, thereby potentially improving both the accuracy and precision of the cluster age. Here we add additional constraints and perform an extensive model comparison to determine the best estimates of the cluster age and helium content, employing as many observational constraints as possible. We improve our photometry and correct empirically for differential reddening effects. We then perform an extensive comparison of the CMDs and eclipsing binary measurements to Victoria and DSEP isochrones to estimate cluster parameters. We also reanalyse a spectrum of the star 2-17 to improve [Fe/H] constraints. We find a best estimate of the age of ~8.3 Gyr while demonstrating that remaining age uncertainty is dominated by uncertainties in the CNO abundances. The helium mass fraction is well constrained at Y = 0.30 \pm 0.01 resulting in dY/dZ ~ 1.4 assuming that such a relation exists. During the analysis we firmly identify blue straggler stars, including the star 2-17, and find indications for the presence of their evolved counterparts. Our analysis supports the RGB mass-loss found from asteroseismology and we determine precisely the absolute mass of stars on the lower RGB, 1.15\pm0.02Msun. This will be an important consistency check for the detailed asteroseismology of cluster stars.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/age-and-helium-content-of-the-open-cluster-ngc-6791-from-multiple-eclipsing-binary-members-ii-age-dependencies-and-new-insights/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>GRB980923. A burst with a short duration high energy component</title>
		<link>http://voxcharta.org/2012/05/20/grb980923-a-burst-with-a-short-duration-high-energy-component/</link>
		<comments>http://voxcharta.org/2012/05/20/grb980923-a-burst-with-a-short-duration-high-energy-component/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:39:24 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[burst]]></category>
		<category><![CDATA[clear evidence]]></category>
		<category><![CDATA[duration]]></category>
		<category><![CDATA[egret]]></category>
		<category><![CDATA[energy component]]></category>
		<category><![CDATA[gamma ray burst]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[keV]]></category>
		<category><![CDATA[lad]]></category>
		<category><![CDATA[light curve]]></category>
		<category><![CDATA[observation]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[sim 2]]></category>
		<category><![CDATA[spectral components]]></category>
		<category><![CDATA[spectral index]]></category>
		<category><![CDATA[spectrum]]></category>
		<category><![CDATA[tasc]]></category>
		<category><![CDATA[variability]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/grb980923-a-burst-with-a-short-duration-high-energy-component/</guid>
		<description><![CDATA[The prompt emission of Gamma Ray Bursts (GRBs) is usually well described by the Band function: two power-laws joined smoothly at a given break energy. In addition to the Band component, a few bursts (GRB941017, GRB090510, GRB090902B and GRB090926A) show clear evidence for a distinct high-energy spectral component, which in some cases evolves independently from [...]]]></description>
			<content:encoded><![CDATA[<p>The prompt emission of Gamma Ray Bursts (GRBs) is usually well described by the Band function: two power-laws joined smoothly at a given break energy. In addition to the Band component, a few bursts (GRB941017, GRB090510, GRB090902B and GRB090926A) show clear evidence for a distinct high-energy spectral component, which in some cases evolves independently from the prompt keV component and is well described by a power-law (PL), sometimes with a cut-off energy; this component is found to have long duration, even longer than the burst itself for all the four bursts. Here we report the observation of an anomalous short duration high energy component in GRB980923. GRB980923 is one of the brightest Gamma-Ray Bursts (GRBs) observed by BATSE. Its light curve is characterized by a rapid variability phase lasting \sim 40 s, followed by a smooth emission tail lasting \sim 400 s. A detailed joint analysis of BATSE (LAD and SD) and EGRET TASC data of GRB980923 reveles the presence of an anomalous keV to MeV component in the spectrum that evolves independently from the prompt keV one. This component is well described by a PL with a spectral index of 1.44 and lasts only \sim 2 s; it represents one of the three clearly separated spectral components identified in GRB980923, the other two being the keV prompt emission, well described by the Band function and the tail, well fit by a Smoothly Broken Power Law (SBPL).</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/grb980923-a-burst-with-a-short-duration-high-energy-component/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<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>
		</item>
		<item>
		<title>Protostellar Accretion Flows Destabilized by Magnetic Flux Redistribution</title>
		<link>http://voxcharta.org/2012/05/20/protostellar-accretion-flows-destabilized-by-magnetic-flux-redistribution/</link>
		<comments>http://voxcharta.org/2012/05/20/protostellar-accretion-flows-destabilized-by-magnetic-flux-redistribution/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:38:57 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[advection]]></category>
		<category><![CDATA[central star]]></category>
		<category><![CDATA[collapse]]></category>
		<category><![CDATA[dense core]]></category>
		<category><![CDATA[density region]]></category>
		<category><![CDATA[field strength]]></category>
		<category><![CDATA[heart of the problem]]></category>
		<category><![CDATA[inflow]]></category>
		<category><![CDATA[interchange instability]]></category>
		<category><![CDATA[latter phase]]></category>
		<category><![CDATA[low density]]></category>
		<category><![CDATA[magnetic flux]]></category>
		<category><![CDATA[molecular cloud]]></category>
		<category><![CDATA[orders of magnitude]]></category>
		<category><![CDATA[radii]]></category>
		<category><![CDATA[realistic level]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[stellar field]]></category>
		<category><![CDATA[three dimensions]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/protostellar-accretion-flows-destabilized-by-magnetic-flux-redistribution/</guid>
		<description><![CDATA[Magnetic flux redistribution lies at the heart of the problem of star formation in dense cores of molecular clouds that are magnetized to a realistic level. If all of the magnetic flux of a typical core were to be dragged into the central star, the stellar field strength would be orders of magnitude higher than [...]]]></description>
			<content:encoded><![CDATA[<p>Magnetic flux redistribution lies at the heart of the problem of star formation in dense cores of molecular clouds that are magnetized to a realistic level. If all of the magnetic flux of a typical core were to be dragged into the central star, the stellar field strength would be orders of magnitude higher than the observed values. This well-known &#8220;magnetic flux problem&#8221; can in principle be resolved through non-ideal MHD effects. Two dimensional (axisymmetric) calculations have shown that ambipolar diffusion, in particular, can transport magnetic flux outward relative to matter, allowing material to enter the central object without dragging the field lines along. We show through simulations that such axisymmetric protostellar accretion flows are unstable in three dimensions to magnetic interchange instability in the azimuthal direction. The instability is driven by the magnetic flux redistributed from the matter that enters the central object. It typically starts to develop during the transition from the prestellar phase of star formation to the protostellar mass accretion phase. In the latter phase, the magnetic flux is transported outward mainly through advection, by strongly magnetized low-density regions that expand against the collapsing inflow. The tussle between the gravity-driven infall and magnetically driven expansion leads to a filamentary inner accretion flow, more disordered than previously pictured. The efficient outward transport of magnetic flux by advection lowers the field strength at small radii, making the magnetic braking less efficient and the formation of rotationally supported disks easier in principle. However, we find no evidence for such disks in any of our rotating collapse simulations. We conclude that the inner protostellar accretion flow is shaped to a large extent by this magnetic interchange instability. How disks form in such an environment is unclear.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/protostellar-accretion-flows-destabilized-by-magnetic-flux-redistribution/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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		<title>Three-Dimensional Explosion Geometry of Stripped-Envelope Core-Collapse Supernovae. I. Spectropolarimetric Observations</title>
		<link>http://voxcharta.org/2012/05/20/three-dimensional-explosion-geometry-of-stripped-envelope-core-collapse-supernovae-i-spectropolarimetric-observations/</link>
		<comments>http://voxcharta.org/2012/05/20/three-dimensional-explosion-geometry-of-stripped-envelope-core-collapse-supernovae-i-spectropolarimetric-observations/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:38:33 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[core collapse supernovae]]></category>
		<category><![CDATA[dispersion]]></category>
		<category><![CDATA[distributions]]></category>
		<category><![CDATA[ejecta]]></category>
		<category><![CDATA[explosion]]></category>
		<category><![CDATA[polarization]]></category>
		<category><![CDATA[SNe]]></category>
		<category><![CDATA[three dimensional geometry]]></category>
		<category><![CDATA[type ic]]></category>
		<category><![CDATA[wavelength]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/three-dimensional-explosion-geometry-of-stripped-envelope-core-collapse-supernovae-i-spectropolarimetric-observations/</guid>
		<description><![CDATA[We study the multi-dimensional geometry of supernova (SN) explosions by means of spectropolarimetric observations of stripped-envelope SNe, i.e., SNe without a H-rich layer. We perform spectropolarimetric observations of 2 stripped-envelope SNe, the Type Ib SN 2009jf and the Type Ic SN 2009mi. Both objects show non-zero polarization at the wavelength of the strong lines. They [...]]]></description>
			<content:encoded><![CDATA[<p>We study the multi-dimensional geometry of supernova (SN) explosions by means of spectropolarimetric observations of stripped-envelope SNe, i.e., SNe without a H-rich layer. We perform spectropolarimetric observations of 2 stripped-envelope SNe, the Type Ib SN 2009jf and the Type Ic SN 2009mi. Both objects show non-zero polarization at the wavelength of the strong lines. They also show a loop in the Stokes Q-U diagram, which indicates a non-axisymmetric, three-dimensional ion distribution in the ejecta. We show that five out of six stripped-envelope SNe which have been observed spectropolarimetrically so far show such a loop. This implies that a three-dimensional geometry is common in stripped-envelope SNe. We find that stronger lines tend to show higher polarization. This effect is not related to the geometry, and must be corrected to compare the polarization of different lines or different objects. Even after the correction, however, there remains a dispersion of polarization degree among different objects. Such a dispersion might be caused by three-dimensional clumpy ion distributions viewed from different directions.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/three-dimensional-explosion-geometry-of-stripped-envelope-core-collapse-supernovae-i-spectropolarimetric-observations/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<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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		<item>
		<title>130 GeV Gamma-Ray Line from Dark Matter Decay [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/20/130-gev-gamma-ray-line-from-dark-matter-decay-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/20/130-gev-gamma-ray-line-from-dark-matter-decay-cross-listing/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:38:09 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abundance]]></category>
		<category><![CDATA[annihilation]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[decay]]></category>
		<category><![CDATA[dimension 6]]></category>
		<category><![CDATA[expectation value]]></category>
		<category><![CDATA[Fermi]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[grand unification]]></category>
		<category><![CDATA[mssm]]></category>
		<category><![CDATA[tev scale]]></category>
		<category><![CDATA[vacuum]]></category>
		<category><![CDATA[viable model]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/130-gev-gamma-ray-line-from-dark-matter-decay-cross-listing/</guid>
		<description><![CDATA[The 130 GeV gamma-ray line based on tentative analyses on the Fermi-LAT data is hard to be understood with dark matter annihilation in the conventional framework of the MSSM. We point out that it can be nicely explained with two body decay of a scalar dark matter ($\tilde{\phi}_{\rm DM}\rightarrow\gamma\gamma$) by the dimension 6 operator suppressed [...]]]></description>
			<content:encoded><![CDATA[<p>The 130 GeV gamma-ray line based on tentative analyses on the Fermi-LAT data is hard to be understood with dark matter annihilation in the conventional framework of the MSSM. We point out that it can be nicely explained with two body decay of a scalar dark matter ($\tilde{\phi}_{\rm DM}\rightarrow\gamma\gamma$) by the dimension 6 operator suppressed with the mass of the grand unification scale ($\sim 10^{16}$ GeV), ${\cal L}\supset|\tilde{\phi}_{\rm DM}|^2F_{\mu\nu}F^{\mu\nu}/M_{\rm GUT}^2$, in which the scalar dark matter $\tilde{\phi}_{\rm DM}$ develops a TeV scale vacuum expectation value. We propose a viable model, which can explain the 130 GeV gamma-ray line and also the abundance of $\tilde{\phi}_{\rm DM}$.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/130-gev-gamma-ray-line-from-dark-matter-decay-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>On the HU Aquarii planetary system hypothesis</title>
		<link>http://voxcharta.org/2012/05/20/on-the-hu-aquarii-planetary-system-hypothesis/</link>
		<comments>http://voxcharta.org/2012/05/20/on-the-hu-aquarii-planetary-system-hypothesis/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:37:50 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[body solution]]></category>
		<category><![CDATA[compact system]]></category>
		<category><![CDATA[companion]]></category>
		<category><![CDATA[eccentricity]]></category>
		<category><![CDATA[ephemeris]]></category>
		<category><![CDATA[jupiter masses]]></category>
		<category><![CDATA[kepler]]></category>
		<category><![CDATA[kinematic model]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[light travel time]]></category>
		<category><![CDATA[photometric observations]]></category>
		<category><![CDATA[planetary system]]></category>
		<category><![CDATA[precision light]]></category>
		<category><![CDATA[resolution photo]]></category>
		<category><![CDATA[spectral window]]></category>
		<category><![CDATA[systematics]]></category>
		<category><![CDATA[unique solution]]></category>
		<category><![CDATA[vir]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/on-the-hu-aquarii-planetary-system-hypothesis/</guid>
		<description><![CDATA[In this work, we investigate the eclipse timing of the polar binary HU Aquarii that has been observed for almost two decades. Recently, Qian et al. attributed large (O-C) deviations between the eclipse ephemeris and observations to a compact system of two massive jovian companions. We improve the Keplerian, kinematic model of the Light Travel [...]]]></description>
			<content:encoded><![CDATA[<p>In this work, we investigate the eclipse timing of the polar binary HU Aquarii that has been observed for almost two decades. Recently, Qian et al. attributed large (O-C) deviations between the eclipse ephemeris and observations to a compact system of two massive jovian companions. We improve the Keplerian, kinematic model of the Light Travel Time (LTT) effect and re-analyse the whole currently available data set. We add almost 60 new, yet unpublished, mostly precision light curves obtained using the time high-resolution photo-polarimeter OPTIMA, as well as photometric observations performed at the MONET/N, PIRATE and TCS telescopes. We determine new mid&#8211;egress times with a mean uncertainty at the level of 1 second or better. We claim that because the observations that currently exist in the literature are non-homogeneous with respect to spectral windows (ultraviolet, X-ray, visual, polarimetric mode) and the reported mid&#8211;egress measurements errors, they may introduce systematics that affect orbital fits. Indeed, we find that the published data, when taken literally, cannot be explained by any unique solution. Many qualitatively different and best-fit 2-planet configurations, including self-consistent, Newtonian N-body solutions may be able to explain the data. However, using high resolution, precision OPTIMA light curves, we find that the (O-C) deviations are best explained by the presence of a single circumbinary companion orbiting at a distance of ~4.5 AU with a small eccentricity and having ~7 Jupiter-masses. This object could be the next circumbinary planet detected from the ground, similar to the announced companions around close binaries HW Vir, NN Ser, UZ For, DP Leo or SZ Her, and planets of this type around Kepler-16, Kepler-34 and Kepler-35.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/on-the-hu-aquarii-planetary-system-hypothesis/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A divergence-cleaning scheme for cosmological SPMHD simulations</title>
		<link>http://voxcharta.org/2012/05/20/a-divergence-cleaning-scheme-for-cosmological-spmhd-simulations/</link>
		<comments>http://voxcharta.org/2012/05/20/a-divergence-cleaning-scheme-for-cosmological-spmhd-simulations/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:37:35 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[artifact]]></category>
		<category><![CDATA[cluster formation]]></category>
		<category><![CDATA[cosmological simulations]]></category>
		<category><![CDATA[divergence]]></category>
		<category><![CDATA[faraday rotation]]></category>
		<category><![CDATA[galaxy cluster]]></category>
		<category><![CDATA[gas dynamics]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[implementation]]></category>
		<category><![CDATA[induction equation]]></category>
		<category><![CDATA[instabilities]]></category>
		<category><![CDATA[lorentz force]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetic field line]]></category>
		<category><![CDATA[magnetohydrodynamics mhd]]></category>
		<category><![CDATA[map]]></category>
		<category><![CDATA[numerical error]]></category>
		<category><![CDATA[parabolic]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[structure function]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/a-divergence-cleaning-scheme-for-cosmological-spmhd-simulations/</guid>
		<description><![CDATA[In magnetohydrodynamics (MHD), the magnetic field is evolved by the induction equation and coupled to the gas dynamics by the Lorentz force. We perform numerical smoothed particle magnetohydrodynamics (Spmhd) simulations and study the influence of a numerical magnetic divergence. For instabilities arising from divergence B related errors, we find the hyperbolic/parabolic cleaning scheme suggested by [...]]]></description>
			<content:encoded><![CDATA[<p>In magnetohydrodynamics (MHD), the magnetic field is evolved by the induction equation and coupled to the gas dynamics by the Lorentz force. We perform numerical smoothed particle magnetohydrodynamics (Spmhd) simulations and study the influence of a numerical magnetic divergence. For instabilities arising from divergence B related errors, we find the hyperbolic/parabolic cleaning scheme suggested by Dedner et al. 2002 to give good results and prevent numerical artifacts from growing. Additionally, we demonstrate that certain current Spmhd implementations of magnetic field regularizations give rise to unphysical instabilities in long-time simulations. We also find this effect when employing Euler potentials (divergenceless by definition), which are not able to follow the winding-up process of magnetic field lines properly. Furthermore, we present cosmological simulations of galaxy cluster formation at extremely high resolution including the evolution of magnetic fields. We show synthetic Faraday rotation maps and derive structure functions to compare them with observations. Comparing all the simulations with and without divergence cleaning, we are able to confirm the results of previous simulations performed with the standard implementation of MHD in Spmhd at normal resolution. However, at extremely high resolution, a cleaning scheme is needed to prevent the growth of numerical errors at small scales.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/a-divergence-cleaning-scheme-for-cosmological-spmhd-simulations/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>The bright-end of the luminosity function at z~9</title>
		<link>http://voxcharta.org/2012/05/20/the-bright-end-of-the-luminosity-function-at-z9/</link>
		<comments>http://voxcharta.org/2012/05/20/the-bright-end-of-the-luminosity-function-at-z9/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:37:24 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[10x10]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[galaxy luminosity function]]></category>
		<category><![CDATA[hawk]]></category>
		<category><![CDATA[interloper]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[mpc]]></category>
		<category><![CDATA[phi]]></category>
		<category><![CDATA[sfr]]></category>
		<category><![CDATA[shooter]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[star formation history]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[vlt]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/the-bright-end-of-the-luminosity-function-at-z9/</guid>
		<description><![CDATA[We report new constraints on the galaxy luminosity function at z~9 based on observations carried out with ESO/VLT FORS2, HAWK-I and X-Shooter around the lensing cluster A2667, as part of our project aimed at selecting z~7-10 candidates accessible to spectroscopy. Only one J-dropout source was selected in this field fulfilling the color and magnitude criteria. [...]]]></description>
			<content:encoded><![CDATA[<p>We report new constraints on the galaxy luminosity function at z~9 based on observations carried out with ESO/VLT FORS2, HAWK-I and X-Shooter around the lensing cluster A2667, as part of our project aimed at selecting z~7-10 candidates accessible to spectroscopy. Only one J-dropout source was selected in this field fulfilling the color and magnitude criteria. This source was recently confirmed as a mid-z interloper based on X-Shooter spectroscopy. The depth and the area covered by our survey are well suited to set strong constraints on the bright-end of the galaxy luminosity function and hence on the star formation history at very high redshift. The non-detection of reliable J-dropout sources over the ~36arcmin2 field of view towards A2667 was used to carefully determine the lens-corrected effective volume and the corresponding upper-limit on the density of sources. The strongest limit is obtained for Phi(M_{1500}=-21.4+/-0.50)-19.7 with fixed alpha=-1.74 and Phi*=1.10&#215;10^{-3}Mpc^{-3}. The corresponding star formation rate density should be rho_{SFR}&lt;5.97&#215;10^{-3}M_{solar}/yr/Mpc^{3} at z~9. These results are in good agreement with the most recent estimates already published in this range of redshift and for this luminosity domain. This new result confirms the decrease in the density of luminous galaxies at very high-redshift, hence providing strong constraints for the design of future surveys aiming to explore the very high-redshift Universe.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/the-bright-end-of-the-luminosity-function-at-z9/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>A Suzaku Study of Ejecta Structure and Origin of Hard X-ray Emission in the Supernova Remnant G156.2+5.7</title>
		<link>http://voxcharta.org/2012/05/20/a-suzaku-study-of-ejecta-structure-and-origin-of-hard-x-ray-emission-in-the-supernova-remnant-g156-25-7/</link>
		<comments>http://voxcharta.org/2012/05/20/a-suzaku-study-of-ejecta-structure-and-origin-of-hard-x-ray-emission-in-the-supernova-remnant-g156-25-7/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:37:10 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cluster of galaxies]]></category>
		<category><![CDATA[diameter]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[element]]></category>
		<category><![CDATA[equilibrium]]></category>
		<category><![CDATA[extent]]></category>
		<category><![CDATA[ism]]></category>
		<category><![CDATA[radial structure]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[robust evidence]]></category>
		<category><![CDATA[shock]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[supernova remnant]]></category>
		<category><![CDATA[thermal emission]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/a-suzaku-study-of-ejecta-structure-and-origin-of-hard-x-ray-emission-in-the-supernova-remnant-g156-25-7/</guid>
		<description><![CDATA[We report an X-ray study of the evolved Galactic supernova remnant (SNR) G156.2+5.7 based on six pointing observations with Suzaku. The remnant&#8217;s large extent (100$\arcmin$ in diameter) allows us to investigate its radial structure in the northwestern and eastern directions from the apparent center. The X-ray spectra were well fit with a two-component non-equilibrium ionization [...]]]></description>
			<content:encoded><![CDATA[<p>We report an X-ray study of the evolved Galactic supernova remnant (SNR) G156.2+5.7 based on six pointing observations with Suzaku. The remnant&#8217;s large extent (100$\arcmin$ in diameter) allows us to investigate its radial structure in the northwestern and eastern directions from the apparent center. The X-ray spectra were well fit with a two-component non-equilibrium ionization model representing the swept-up interstellar medium (ISM) and the metal-rich ejecta. We found prominent central concentrations of Si, S and Fe from the ejecta component; the lighter elements of O, Ne and Mg were distributed more uniformly. The temperature of the ISM component suggests a slow shock (610-960 km s$^{-1}$), hence the remnant&#8217;s age is estimated to be 7,000-15,000 yr, assuming its distance to be $\sim$1.1 kpc. G156.2+5.7 has also been thought to emit hard, non-thermal X-rays, despite being considerably older than any other such remnant. In response to a recent discovery of a background cluster of galaxies (2XMM J045637.2+522411), we carefully excluded its contribution, and reexamined the origin of the hard X-ray emission. We found that the residual hard X-ray emission is consistent with the expected level of the cosmic X-ray background. Thus, no robust evidence for the non-thermal emission was obtained from G156.2+5.7. These results are consistent with the picture of an evolved SNR.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/a-suzaku-study-of-ejecta-structure-and-origin-of-hard-x-ray-emission-in-the-supernova-remnant-g156-25-7/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Measuring Space-Time Geometry over the Ages [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/20/measuring-space-time-geometry-over-the-ages-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/20/measuring-space-time-geometry-over-the-ages-cross-listing/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:36:48 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[baseline]]></category>
		<category><![CDATA[centuries]]></category>
		<category><![CDATA[coordinates]]></category>
		<category><![CDATA[curvature]]></category>
		<category><![CDATA[decade]]></category>
		<category><![CDATA[drift]]></category>
		<category><![CDATA[einstein]]></category>
		<category><![CDATA[formalism]]></category>
		<category><![CDATA[free matter]]></category>
		<category><![CDATA[initial condition]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[observational program]]></category>
		<category><![CDATA[parametrization]]></category>
		<category><![CDATA[proper motion]]></category>
		<category><![CDATA[space time]]></category>
		<category><![CDATA[theorists]]></category>
		<category><![CDATA[time geometry]]></category>
		<category><![CDATA[visual observations]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/measuring-space-time-geometry-over-the-ages-cross-listing/</guid>
		<description><![CDATA[Theorists are often told to express things in the &#8220;observational plane&#8221;. One can do this for space-time geometry, considering &#8220;visual&#8221; observations of matter in our universe by a single observer over time, with no assumptions about isometries, initial conditions, nor any particular relation between matter and geometry, such as Einstein&#8217;s equations. Using observables as coordinates [...]]]></description>
			<content:encoded><![CDATA[<p>Theorists are often told to express things in the &#8220;observational plane&#8221;. One can do this for space-time geometry, considering &#8220;visual&#8221; observations of matter in our universe by a single observer over time, with no assumptions about isometries, initial conditions, nor any particular relation between matter and geometry, such as Einstein&#8217;s equations. Using observables as coordinates naturally leads to a parametrization of space-time geometry in terms of other observables, which in turn prescribes an observational program to measure the geometry. Under the assumption of vorticity-free matter flow we describe this observational program, which includes measurements of gravitational lensing, proper motion, and redshift drift. Only 15% of the curvature information can be extracted without long time baseline observations, and this increases to 35% with observations that will take decades. The rest would likely require centuries of observations. The formalism developed is exact, non-perturbative, and more general than the usual cosmological analysis.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/measuring-space-time-geometry-over-the-ages-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Regulation of Black Hole Winds and Jets Across the Mass Scale</title>
		<link>http://voxcharta.org/2012/05/20/regulation-of-black-hole-winds-and-jets-across-the-mass-scale/</link>
		<comments>http://voxcharta.org/2012/05/20/regulation-of-black-hole-winds-and-jets-across-the-mass-scale/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:36:36 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[eddington]]></category>
		<category><![CDATA[energetics]]></category>
		<category><![CDATA[grating]]></category>
		<category><![CDATA[hole accretion]]></category>
		<category><![CDATA[hole mass]]></category>
		<category><![CDATA[ionization]]></category>
		<category><![CDATA[jet power]]></category>
		<category><![CDATA[jet production]]></category>
		<category><![CDATA[mass scale]]></category>
		<category><![CDATA[mechanical power]]></category>
		<category><![CDATA[outflow velocity]]></category>
		<category><![CDATA[possible connection]]></category>
		<category><![CDATA[snr]]></category>
		<category><![CDATA[uniform analysis]]></category>
		<category><![CDATA[wind power]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/regulation-of-black-hole-winds-and-jets-across-the-mass-scale/</guid>
		<description><![CDATA[We present a study of the mechanical power generated by both winds and jets across the black hole mass scale. We begin with the study of ionized X-ray winds and present a uniform analysis using Chandra grating spectra. The high quality grating spectra facilitate the characterization of the outflow velocity, ionization and column density of [...]]]></description>
			<content:encoded><![CDATA[<p>We present a study of the mechanical power generated by both winds and jets across the black hole mass scale. We begin with the study of ionized X-ray winds and present a uniform analysis using Chandra grating spectra. The high quality grating spectra facilitate the characterization of the outflow velocity, ionization and column density of the absorbing gas. We find that the kinetic power of the winds scales with increasing bolometric luminosity as log(L_wind) \propto (1.57 \pm 0.07) log(L_Bol). This means that SMBH may be more efficient than stellar-mass black holes in launching winds. In addition, the simplicity of the scaling may suggest common driving mechanisms across the mass scale. For comparison, we next examine jet production, estimating jet power based on the energy required to inflate local bubbles. The jet relation is log(L_Jet)\propto (1.18\pm0.24) log(L_Bol). The energetics of the bubble associated with Cygnus X-1 are particularly difficult to determine, and the bubble could be a background SNR. If we exclude Cygnus X-1, then the jets follow a consistent relation to the winds within errors but with a higher normalization, log(L_Jet) \propto (1.34 \pm 0.50) log(L_Bol). The formal consistency in the wind and jet scaling relations suggests that a common launching mechanism may drive both flows; magnetic processes are viable possibilities. We also examine winds with especially high velocities, v &gt; 0.01c. These ultra-fast outflows tend to resemble the jets more than the winds, indicating we may be observing a regime in which winds become jets. This study allows for the total power from black hole accretion, both mechanical and radiative, to be characterized in a simple manner and suggests a possible connection between winds and jets. Finally, we find at low Eddington fractions, the jet power is dominant, and at high Eddington fractions the wind power is dominant.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/regulation-of-black-hole-winds-and-jets-across-the-mass-scale/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<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>
		</item>
		<item>
		<title>Classification of the FRW universe with a cosmological constant and a perfect fluid of the equation of state $p = w\rho$ [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/classification-of-the-frw-universe-with-a-cosmological-constant-and-a-perfect-fluid-of-the-equation-of-state-p-wrho-replacement/</link>
		<comments>http://voxcharta.org/2012/05/20/classification-of-the-frw-universe-with-a-cosmological-constant-and-a-perfect-fluid-of-the-equation-of-state-p-wrho-replacement/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:36:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration]]></category>
		<category><![CDATA[big bang]]></category>
		<category><![CDATA[cosmological constant]]></category>
		<category><![CDATA[crunch]]></category>
		<category><![CDATA[curvature]]></category>
		<category><![CDATA[deceleration]]></category>
		<category><![CDATA[dimensional space]]></category>
		<category><![CDATA[energy density]]></category>
		<category><![CDATA[equation of state]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[existence]]></category>
		<category><![CDATA[friedmann]]></category>
		<category><![CDATA[frw]]></category>
		<category><![CDATA[period]]></category>
		<category><![CDATA[singularity]]></category>
		<category><![CDATA[textbook]]></category>
		<category><![CDATA[universe]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/classification-of-the-frw-universe-with-a-cosmological-constant-and-a-perfect-fluid-of-the-equation-of-state-p-wrho-replacement/</guid>
		<description><![CDATA[We systematically study the evolution of the Friedmann-Robertson-Walker (FRW) universe coupled with a cosmological constant $\Lambda$ and a perfect fluid that has the equation of state $p=w\rho$, where $p$ and $\rho$ denote, respectively, the pressure and energy density of the fluid, and $w$ is an arbitrary real constant. Depending on the specific values of $w,\; [...]]]></description>
			<content:encoded><![CDATA[<p>We systematically study the evolution of the Friedmann-Robertson-Walker (FRW) universe coupled with a cosmological constant $\Lambda$ and a perfect fluid that has the equation of state $p=w\rho$, where $p$ and $\rho$ denote, respectively, the pressure and energy density of the fluid, and $w$ is an arbitrary real constant. Depending on the specific values of $w,\; \Lambda$, and the curvature $k$ of 3-dimensional space, we separate all of the solutions into various cases. In each case the main properties of the evolution are given in detail, including the periods of deceleration and/or acceleration, and the existence of big bang, big crunch, and big rip singularities. In some cases, errors in classification and interpretation appearing in standard textbooks have been corrected.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/classification-of-the-frw-universe-with-a-cosmological-constant-and-a-perfect-fluid-of-the-equation-of-state-p-wrho-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<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>Wheels of Fire IV. Star Formation and the Neutral Interstellar Medium in the Ring Galaxy AM0644-741 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/wheels-of-fire-iv-star-formation-and-the-neutral-interstellar-medium-in-the-ring-galaxy-am0644-741-replacement/</link>
		<comments>http://voxcharta.org/2012/05/20/wheels-of-fire-iv-star-formation-and-the-neutral-interstellar-medium-in-the-ring-galaxy-am0644-741-replacement/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:35:04 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[atnf]]></category>
		<category><![CDATA[atomic gas]]></category>
		<category><![CDATA[diameter]]></category>
		<category><![CDATA[instabilities]]></category>
		<category><![CDATA[interstellar medium]]></category>
		<category><![CDATA[ism]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[low density]]></category>
		<category><![CDATA[massive star formation]]></category>
		<category><![CDATA[molecular fraction]]></category>
		<category><![CDATA[precursor]]></category>
		<category><![CDATA[ring galaxy]]></category>
		<category><![CDATA[sest]]></category>
		<category><![CDATA[wheels of fire]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/wheels-of-fire-iv-star-formation-and-the-neutral-interstellar-medium-in-the-ring-galaxy-am0644-741-replacement/</guid>
		<description><![CDATA[We combine data from the ATNF and the SEST to investigate the neutral ISM in AM0644-741, a large and robustly star-forming ring galaxy. The galaxy&#8217;s ISM is concentrated in the 42-kpc diameter starburst ring, but appears dominated by atomic gas, with a global molecular fraction (f_mol) of only 7.9%. Apart from the starburst peak, the [...]]]></description>
			<content:encoded><![CDATA[<p>We combine data from the ATNF and the SEST to investigate the neutral ISM in AM0644-741, a large and robustly star-forming ring galaxy. The galaxy&#8217;s ISM is concentrated in the 42-kpc diameter starburst ring, but appears dominated by atomic gas, with a global molecular fraction (f_mol) of only 7.9%. Apart from the starburst peak, the gas ring is stable against the growth of gravitational instabilities (Q_gas=2-7). Including stars lowers Q overall, but not enough to make Q100 Myr confinement time in the starburst ring, which enhances the destructive effects of embedded massive stars and supernovae. As a result, the ring&#8217;s molecular ISM becomes dominated by small clouds where star formation is most intense, causing H2 to be underestimated by 12CO line fluxes: in effect X(CO) &gt;&gt; X(Gal) despite the ring&#8217;s solar metallicity. The observed large HI component is primarily a low density photodissociation product, i.e., a tracer rather than a precursor of massive star formation. Such an &#8220;over-cooked&#8221; ISM may be a general characteristic of evolved starburst ring galaxies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/wheels-of-fire-iv-star-formation-and-the-neutral-interstellar-medium-in-the-ring-galaxy-am0644-741-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The role of OH in the chemical evolution of protoplanetary disks. I. The comet-forming region [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/the-role-of-oh-in-the-chemical-evolution-of-protoplanetary-disks-i-the-comet-forming-region-replacement/</link>
		<comments>http://voxcharta.org/2012/05/20/the-role-of-oh-in-the-chemical-evolution-of-protoplanetary-disks-i-the-comet-forming-region-replacement/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:34:42 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accurate treatment]]></category>
		<category><![CDATA[chemical composition]]></category>
		<category><![CDATA[chemical evolution]]></category>
		<category><![CDATA[chemical model]]></category>
		<category><![CDATA[chemical species]]></category>
		<category><![CDATA[cm 3]]></category>
		<category><![CDATA[comet formation]]></category>
		<category><![CDATA[complex organic molecules]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[desorption]]></category>
		<category><![CDATA[ects]]></category>
		<category><![CDATA[grain size distribution]]></category>
		<category><![CDATA[model yields]]></category>
		<category><![CDATA[photo processes]]></category>
		<category><![CDATA[photon flux]]></category>
		<category><![CDATA[protoplanetary disk]]></category>
		<category><![CDATA[rate equations]]></category>
		<category><![CDATA[timescale]]></category>
		<category><![CDATA[water ice]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/the-role-of-oh-in-the-chemical-evolution-of-protoplanetary-disks-i-the-comet-forming-region-replacement/</guid>
		<description><![CDATA[Context. Time dependent gas-grain chemistry can help us understand the layered structure of species deposited onto the surface of grains during the lifetime of a protoplanetary disk. The history of trapping important quantities of carbon- and oxygen-bearing molecules onto the grains is of special significance for the formation of more complex (organic) molecules on the [...]]]></description>
			<content:encoded><![CDATA[<p>Context. Time dependent gas-grain chemistry can help us understand the layered structure of species deposited onto the surface of grains during the lifetime of a protoplanetary disk. The history of trapping important quantities of carbon- and oxygen-bearing molecules onto the grains is of special significance for the formation of more complex (organic) molecules on the surface of grains. Aims. Among other processes, cosmic ray-induced UV photo-processes can lead to the efficient formation of OH. Using a more accurate treatment of cosmic ray-gas interactions for disks, we obtain an increased cosmic ray-induced UV photon flux of 3.8&#215;10^5 photons cm^-2s^-1 for a cosmic-ray ionization rate of H2 value of 5&#215;10^-17 s^-1 (compared to previous estimates of 10^4 photons cm^-2s^-1 based on ISM dust properties). We explore the role of the enhanced OH abundance on the gas-grain chemistry in the midplane of the disk at 10 AU, which is a plausible location for comet formation. We focus on studying the formation/destruction pathways and timescales of the dominant chemical species. Methods. We solve the chemical rate equations based on a gas-grain chemical network and correcting for the enhanced cosmic rayinduced UV field. This field is estimated from an appropriate treatment of dust properties in a protoplanetary disk, as opposed to previous estimates that assume an ISM-like grain size distribution. We also explore the chemical eff?ects of photo-desorption of water ice into OH+H. Results. Near the end of the disk&#8217;s lifetime our chemical model yields H2O, CO, CO2 and CH4 ice abundances at 10 AU (consistent with a midplane density of 10^10 cm^-3 and a temperature of 20 K) that are compatible with measurements of the chemical composition of cometary bodies for a [C/O] ratio of 0.16. Such comparison provides constraints on the physical conditions in which comets were formed.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/the-role-of-oh-in-the-chemical-evolution-of-protoplanetary-disks-i-the-comet-forming-region-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>FRW Cosmology in Ghost Free Massive Gravity [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/frw-cosmology-in-ghost-free-massive-gravity-replacement/</link>
		<comments>http://voxcharta.org/2012/05/20/frw-cosmology-in-ghost-free-massive-gravity-replacement/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:34:30 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[attractor]]></category>
		<category><![CDATA[control parameter]]></category>
		<category><![CDATA[cosmological constant]]></category>
		<category><![CDATA[cosmological evolution]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[deformation]]></category>
		<category><![CDATA[frw]]></category>
		<category><![CDATA[ghost]]></category>
		<category><![CDATA[graviton]]></category>
		<category><![CDATA[massive gravity]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[previous works]]></category>
		<category><![CDATA[universe]]></category>
		<category><![CDATA[xi region]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/frw-cosmology-in-ghost-free-massive-gravity-replacement/</guid>
		<description><![CDATA[We study FRW homogeneous cosmological solutions in the recently found ghost free massive gravity. In previous works it was shown that when the additional extra metric, needed to generate the mass term, is taken as non-dynamical and flat, no homogeneous FRW cosmology exists. We show that, when the additional metric is a dynamical field, a [...]]]></description>
			<content:encoded><![CDATA[<p>We study FRW homogeneous cosmological solutions in the recently found ghost free massive gravity. In previous works it was shown that when the additional extra metric, needed to generate the mass term, is taken as non-dynamical and flat, no homogeneous FRW cosmology exists. We show that, when the additional metric is a dynamical field, a perfectly safe FRW universe exists. FRW solutions fall in two branches. In the first branch the massive deformation is equivalent to an effectively generated cosmological constant whose scale is determined by the graviton mass. The second branch is quite rich: we have FRW cosmology in the presence of a &#8220;gravitational&#8221; fluid. The control parameter xi is the ratio of the two conformal factors. When xi is large, generically the cosmological evolution greatly differs from GR at the early time. In the small xi region, the evolution is similar to GR and the universe flows at late time toward an attractor represented by a dS phase.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/frw-cosmology-in-ghost-free-massive-gravity-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Was The Sun Born In A Massive Cluster? [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/was-the-sun-born-in-a-massive-cluster-replacement/</link>
		<comments>http://voxcharta.org/2012/05/20/was-the-sun-born-in-a-massive-cluster-replacement/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:34:18 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cluster]]></category>
		<category><![CDATA[cluster mass]]></category>
		<category><![CDATA[cluster properties]]></category>
		<category><![CDATA[contamination]]></category>
		<category><![CDATA[contrary]]></category>
		<category><![CDATA[cross section]]></category>
		<category><![CDATA[disruption]]></category>
		<category><![CDATA[eccentric orbit]]></category>
		<category><![CDATA[lifetime]]></category>
		<category><![CDATA[massive cluster]]></category>
		<category><![CDATA[myr]]></category>
		<category><![CDATA[nearby supernova]]></category>
		<category><![CDATA[outer planet]]></category>
		<category><![CDATA[outer solar system]]></category>
		<category><![CDATA[probability]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[star cluster]]></category>
		<category><![CDATA[stellar encounters]]></category>
		<category><![CDATA[surface density]]></category>
		<category><![CDATA[velocity distribution]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/was-the-sun-born-in-a-massive-cluster-replacement/</guid>
		<description><![CDATA[A number of authors have argued that the Sun must have been born in a cluster of no more than about 1000 stars, on the basis that, in a larger cluster, close encounters between the Sun and other stars would have truncated the outer Solar System or excited the outer planets into eccentric orbits. However, [...]]]></description>
			<content:encoded><![CDATA[<p>A number of authors have argued that the Sun must have been born in a cluster of no more than about 1000 stars, on the basis that, in a larger cluster, close encounters between the Sun and other stars would have truncated the outer Solar System or excited the outer planets into eccentric orbits. However, this dynamical limit is in tension with meteoritic evidence that the Solar System was exposed to a nearby supernova during or shortly after its formation; a 1000-star cluster is much too small for supernova contamination to be likely. In this paper we revisit the dynamical limit in the light of improved observations of the properties of young clusters. We use a series of scattering simulations to measure the velocity-dependent cross-section for disruption of the outer Solar System by stellar encounters, and use this cross-section to compute the probability of a disruptive encounter as a function of birth cluster properties. We find that, contrary to prior work, the probability of disruption is small regardless of the cluster mass, and that it actually decreases rather than increases with cluster mass. Our results differ from prior work for three main reasons: (1) unlike in most previous work, we compute a velocity-dependent cross section and properly integrate over the cluster mass-dependent velocity distribution of incoming stars; (2) we adopt realistically-short cluster lifetimes of a few crossing times, rather than assuming lifetimes of 10 to 100 Myr; and (3) following recent observations, we adopt a mass-independent surface density for embedded clusters, rather than a mass-independent radius as assumed many earlier papers. Our results remove the tension between the dynamical limit and the meteoritic evidence, and suggest that the Sun was born in a massive cluster.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/was-the-sun-born-in-a-massive-cluster-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The density profiles of Dark Matter halos in Spiral Galaxies [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/the-density-profiles-of-dark-matter-halos-in-spiral-galaxies-replacement/</link>
		<comments>http://voxcharta.org/2012/05/20/the-density-profiles-of-dark-matter-halos-in-spiral-galaxies-replacement/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:34:04 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cold dark matter]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[dark halo]]></category>
		<category><![CDATA[dark matter halo]]></category>
		<category><![CDATA[density profile]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gaseous disk]]></category>
		<category><![CDATA[inconsistency]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[paradigm]]></category>
		<category><![CDATA[phenomenology]]></category>
		<category><![CDATA[radii]]></category>
		<category><![CDATA[rotation curve]]></category>
		<category><![CDATA[rotation curves]]></category>
		<category><![CDATA[spiral]]></category>
		<category><![CDATA[spiral galaxy]]></category>
		<category><![CDATA[universal rotation]]></category>
		<category><![CDATA[velocities]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/the-density-profiles-of-dark-matter-halos-in-spiral-galaxies-replacement/</guid>
		<description><![CDATA[In spiral galaxies, we explain their non-Keplerian rotation curves (RCs) by means of a non-luminous component embedding their stellar-gaseous disks. Understanding the detailed properties of this component (labelled Dark Matter, DM) is one of the most pressing issues of Cosmology. We investigate the recent relationship (claimed by Walker et al. 2010, hereafter W+10) between $r$, [...]]]></description>
			<content:encoded><![CDATA[<p>In spiral galaxies, we explain their non-Keplerian rotation curves (RCs) by means of a non-luminous component embedding their stellar-gaseous disks. Understanding the detailed properties of this component (labelled Dark Matter, DM) is one of the most pressing issues of Cosmology. We investigate the recent relationship (claimed by Walker et al. 2010, hereafter W+10) between $r$, the galaxy radial coordinate, and $V_h(r)$, the dark halo contribution to the circular velocity at $r$, {\it a}) in the framework of the Universal Rotation Curve (URC) paradigm and directly {\it b}) by means of the kinematics of a large sample of DM dominated spirals. We find a general agreement between the W+10 claim, the distribution of DM emerging from the URC and that inferred in the (low luminosity) objects of our sample. We show that such a phenomenology, linking the spiral&#8217;s luminosity, radii and circular velocities, implies an evident inconsistency with (naive) predictions in the $\Lambda$ Cold Dark Matter ($\Lambda$CDM) scenario.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/the-density-profiles-of-dark-matter-halos-in-spiral-galaxies-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>High-resolution X-ray spectroscopy reveals the special nature of Wolf-Rayet star winds [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/high-resolution-x-ray-spectroscopy-reveals-the-special-nature-of-wolf-rayet-star-winds-replacement/</link>
		<comments>http://voxcharta.org/2012/05/20/high-resolution-x-ray-spectroscopy-reveals-the-special-nature-of-wolf-rayet-star-winds-replacement/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:33:52 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration]]></category>
		<category><![CDATA[clump]]></category>
		<category><![CDATA[fe line]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[hot x]]></category>
		<category><![CDATA[newton telescope]]></category>
		<category><![CDATA[o star]]></category>
		<category><![CDATA[photosphere]]></category>
		<category><![CDATA[porous structure]]></category>
		<category><![CDATA[rams]]></category>
		<category><![CDATA[shock]]></category>
		<category><![CDATA[spectral analysis]]></category>
		<category><![CDATA[spectral signature]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[star winds]]></category>
		<category><![CDATA[stellar radii]]></category>
		<category><![CDATA[stellar wind]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xmm newton]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/high-resolution-x-ray-spectroscopy-reveals-the-special-nature-of-wolf-rayet-star-winds-replacement/</guid>
		<description><![CDATA[We present the first high-resolution X-ray spectrum of a putatively single Wolf-Rayet star. 400 ks observations of WR 6 by the XMM-Newton-telescope resulted in a superb quality high-resolution X-ray spectrum. Spectral analysis reveals that the X-rays originate far out in the stellar wind, more than 30 stellar radii from the photosphere, and thus outside the [...]]]></description>
			<content:encoded><![CDATA[<p>We present the first high-resolution X-ray spectrum of a putatively single Wolf-Rayet star. 400 ks observations of WR 6 by the XMM-Newton-telescope resulted in a superb quality high-resolution X-ray spectrum. Spectral analysis reveals that the X-rays originate far out in the stellar wind, more than 30 stellar radii from the photosphere, and thus outside the wind acceleration zone where the line-driving instability could create shocks. The X-ray emitting plasma reaches temperatures up to 50\,MK, and is embedded within the un-shocked, &#8220;cool&#8221; stellar wind as revealed by characteristic spectral signatures. We detect a fluorescent Fe line at approx 6.4 keV. The presence of fluorescence is consistent with a two-component medium, where the cool wind is permeated with the hot X-ray emitting plasma. The wind must have a very porous structure to allow the observed amount of X-rays to escape. We find that neither the line-driving instability nor any alternative binary scenario can explain the data. We suggest a scenario where X-rays are produced when the fast wind rams into slow &#8220;sticky clumps&#8221; that resist acceleration. Our new data show that the X-rays in single WR-star are generated by some special mechanism different from the one operating in the O-star winds.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/high-resolution-x-ray-spectroscopy-reveals-the-special-nature-of-wolf-rayet-star-winds-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Strong Multifield Slowroll Condition and Spiral Inflation [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/the-strong-multifield-slowroll-condition-and-spiral-inflation-replacement-4/</link>
		<comments>http://voxcharta.org/2012/05/20/the-strong-multifield-slowroll-condition-and-spiral-inflation-replacement-4/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:33:39 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[analyze this]]></category>
		<category><![CDATA[blueprint]]></category>
		<category><![CDATA[confusion]]></category>
		<category><![CDATA[de sitter]]></category>
		<category><![CDATA[gradient flow]]></category>
		<category><![CDATA[Hubble]]></category>
		<category><![CDATA[inflation]]></category>
		<category><![CDATA[liddle]]></category>
		<category><![CDATA[locus]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[spiral]]></category>
		<category><![CDATA[string theory]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/the-strong-multifield-slowroll-condition-and-spiral-inflation-replacement-4/</guid>
		<description><![CDATA[We point out the existing confusions about the slowroll parameters and conditions for multifield inflation. If one requires the fields to roll down the gradient flow, we find that only articles adopting the Hubble slowroll expansion are on the right track, and a correct condition can be found in a recent book by Liddle and [...]]]></description>
			<content:encoded><![CDATA[<p>We point out the existing confusions about the slowroll parameters and conditions for multifield inflation. If one requires the fields to roll down the gradient flow, we find that only articles adopting the Hubble slowroll expansion are on the right track, and a correct condition can be found in a recent book by Liddle and Lyth. We further analyze this condition and show that the gradient flow requirement is stronger than just asking for a slowly changing, quasi-de Sitter solution. Therefore it is possible to have a multifield slowroll model that does not follow the gradient flow. Consequently, it no longer requires the gradient to be small. It even bypasses the first slowroll condition and some related no-go theorems from string theory. We provide the &#8220;spiral inflation&#8221; as a generic blueprint of such inflation model and show that it relies on a monodromy locus&#8212;a common structure in string theory effective potentials.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/the-strong-multifield-slowroll-condition-and-spiral-inflation-replacement-4/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Particle-in-cell simulations of particle energization from low Mach number fast mode shocks [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/particle-in-cell-simulations-of-particle-energization-from-low-mach-number-fast-mode-shocks-replacement-2/</link>
		<comments>http://voxcharta.org/2012/05/20/particle-in-cell-simulations-of-particle-energization-from-low-mach-number-fast-mode-shocks-replacement-2/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:33:26 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[boundary method]]></category>
		<category><![CDATA[cell pic]]></category>
		<category><![CDATA[cell simulation]]></category>
		<category><![CDATA[dimensional particle]]></category>
		<category><![CDATA[electron distribution]]></category>
		<category><![CDATA[electron mass]]></category>
		<category><![CDATA[initial generation]]></category>
		<category><![CDATA[mach number]]></category>
		<category><![CDATA[magnetic pressure]]></category>
		<category><![CDATA[microphysics]]></category>
		<category><![CDATA[moving wall]]></category>
		<category><![CDATA[pic simulations]]></category>
		<category><![CDATA[plasma turbulence]]></category>
		<category><![CDATA[shock formation]]></category>
		<category><![CDATA[shock speed]]></category>
		<category><![CDATA[shock transition]]></category>
		<category><![CDATA[simulation result]]></category>
		<category><![CDATA[simulation time]]></category>
		<category><![CDATA[solar flare]]></category>
		<category><![CDATA[transition region]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/particle-in-cell-simulations-of-particle-energization-from-low-mach-number-fast-mode-shocks-replacement-2/</guid>
		<description><![CDATA[Astrophysical shocks are often studied in the high Mach number limit but weakly compressive fast shocks can occur in magnetic reconnection outflows and are considered to be a site of particle energization in solar flares. Here we study the microphysics of such perpendicular, low Mach number collisionless shocks using two-dimensional particle-in-cell (PIC) simulations with a [...]]]></description>
			<content:encoded><![CDATA[<p>Astrophysical shocks are often studied in the high Mach number limit but weakly compressive fast shocks can occur in magnetic reconnection outflows and are considered to be a site of particle energization in solar flares. Here we study the microphysics of such perpendicular, low Mach number collisionless shocks using two-dimensional particle-in-cell (PIC) simulations with a reduced ion/electron mass ratio and employ a moving wall boundary method for initial generation of the shock. This moving wall method allows for more control of the shock speed, smaller simulation box sizes, and longer simulation times than the commonly used fixed wall, reflection method of shock formation. Our results, which are independent of the shock formation method, reveal the prevalence shock drift acceleration (SDA) of both electron and ions in a purely perpendicular shock with Alfv\&#8217;en Mach number $M_A=6.8$ and ratio of thermal to magnetic pressure $\beta=8$. We determine the respective minimum energies required for electrons and ions to incur SDA. We derive a theoretical electron distribution via SDA that compares to the simulation results. We also show that a modified two-stream instability due to the incoming and reflecting ions in the shock transition region acts as the mechanism to generate collisionless plasma turbulence that sustains the shock.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/particle-in-cell-simulations-of-particle-energization-from-low-mach-number-fast-mode-shocks-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Highly Ionized Collimated Outflow from HE 0238 &#8211; 1904 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/highly-ionized-collimated-outflow-from-he-0238-1904-replacement/</link>
		<comments>http://voxcharta.org/2012/05/20/highly-ionized-collimated-outflow-from-he-0238-1904-replacement/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:33:14 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorption line]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[hydrogen density]]></category>
		<category><![CDATA[interaction]]></category>
		<category><![CDATA[ionization]]></category>
		<category><![CDATA[line profile]]></category>
		<category><![CDATA[outflow]]></category>
		<category><![CDATA[photoionization model]]></category>
		<category><![CDATA[qso]]></category>
		<category><![CDATA[radio jet]]></category>
		<category><![CDATA[term stability]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/highly-ionized-collimated-outflow-from-he-0238-1904-replacement/</guid>
		<description><![CDATA[We present a detailed analysis of a highly ionized, multiphased and collimated outflowing gas detected through O V, O VI, Ne VIII and Mg X absorption associated with the QSO HE 0238 &#8211; 1904 (z_em ~ 0.629). Based on the similarities in the absorption line profiles and estimated covering fractions, we find that the O [...]]]></description>
			<content:encoded><![CDATA[<p>We present a detailed analysis of a highly ionized, multiphased and collimated outflowing gas detected through O V, O VI, Ne VIII and Mg X absorption associated with the QSO HE 0238 &#8211; 1904 (z_em ~ 0.629). Based on the similarities in the absorption line profiles and estimated covering fractions, we find that the O VI and Ne VIII absorption trace the same phase of the absorbing gas. Simple photoionization models can reproduce the observed N(Ne VIII), N(O VI) and N(Mg X) from a single phase whereas the low ionization species (e.g. N III, N IV, O IV) originate from a different phase. The measured N(Ne VIII)/N(O VI) ratio is found to be remarkably similar (within a factor of ~ 2) in several individual absorption components kinematically spread over ~ 1800 km/s. Under photoionization this requires a fine tuning between hydrogen density (nH) and the distance of the absorbing gas from the QSO. Alternatively this can also be explained by collisional ionization in hot gas with T &gt; 10^{5.7} K. Long-term stability favors the absorbing gas being located outside the broad line region (BLR). We speculate that the collimated flow of such a hot gas could possibly be triggered by the radio jet interaction.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/highly-ionized-collimated-outflow-from-he-0238-1904-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Supernova 1998S at 14 years Postmortem: Continuing CSM Interaction and Dust Formation [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/supernova-1998s-at-14-years-postmortem-continuing-csm-interaction-and-dust-formation-replacement/</link>
		<comments>http://voxcharta.org/2012/05/20/supernova-1998s-at-14-years-postmortem-continuing-csm-interaction-and-dust-formation-replacement/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:32:58 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[centroid]]></category>
		<category><![CDATA[circumstellar material]]></category>
		<category><![CDATA[clump]]></category>
		<category><![CDATA[dust extinction]]></category>
		<category><![CDATA[dust formation]]></category>
		<category><![CDATA[emission features]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[large binocular telescope]]></category>
		<category><![CDATA[last decade]]></category>
		<category><![CDATA[optical spectrum]]></category>
		<category><![CDATA[oxygen profiles]]></category>
		<category><![CDATA[radial distribution]]></category>
		<category><![CDATA[red supergiant]]></category>
		<category><![CDATA[red wing]]></category>
		<category><![CDATA[SNe]]></category>
		<category><![CDATA[strong wind]]></category>
		<category><![CDATA[type iin]]></category>
		<category><![CDATA[wavelength dependence]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/supernova-1998s-at-14-years-postmortem-continuing-csm-interaction-and-dust-formation-replacement/</guid>
		<description><![CDATA[We report late-time spectroscopic observations of the Type IIn SN 1998S, taken 14 years after explosion using the Large Binocular Telescope. The optical spectrum exhibits broad emission features of [O I], [O II], [O III], H-alpha, H-beta, and [Fe II]. The last decade of evolution has exhibited a strengthening of the oxygen transitions, evidence that [...]]]></description>
			<content:encoded><![CDATA[<p>We report late-time spectroscopic observations of the Type IIn SN 1998S, taken 14 years after explosion using the Large Binocular Telescope. The optical spectrum exhibits broad emission features of [O I], [O II], [O III], H-alpha, H-beta, and [Fe II]. The last decade of evolution has exhibited a strengthening of the oxygen transitions, evidence that the late-time emission is powered by increasingly metal-rich SN ejecta crossing the reverse shock. The H-alpha luminosity requires that SN 1998S is still interacting with dense circumstellar material (CSM), probably produced by the strong wind of a red supergiant progenitor at least ~1000 years before explosion. The emission lines exhibit asymmetric blueshifted profiles, which implies that the receding hemisphere of the SN is obscured by dust. The [O III] line, in particular, exhibits a complete suppression of its red wing. This could be the result of the expected wavelength dependence for dust extinction or a smaller radial distribution for [O III]. In the latter case, the red wing of [O III] could be absorbed by core dust, while both the blue and red wings are absorbed by dust within the cool dense shell between the forward and reverse shocks; this interpretation could explain why late-time [O III] emission from SNe is often weaker than models predict. The [O I] line exhibits double-peaked structure on top of the broader underlying profile, possibly due to emission from individual clumps of ejecta or ring-like structures of metal-rich debris. The centroids of the peaks are blueshifted and lack a red counterpart. However, an archival spectrum obtained on day 1093 exhibits a third, redshifted peak, which we suspect has become extinguished by dust that formed over the last decade. This implies that the &#8220;missing&#8221; red components of multi-peaked oxygen profiles observed in other SNe might be obscured by varying degrees of dust extinction.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/supernova-1998s-at-14-years-postmortem-continuing-csm-interaction-and-dust-formation-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>The VMC Survey. V. First results for Classical Cepheids [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/the-vmc-survey-v-first-results-for-classical-cepheids-replacement/</link>
		<comments>http://voxcharta.org/2012/05/20/the-vmc-survey-v-first-results-for-classical-cepheids-replacement/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:32:45 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[3d geometry]]></category>
		<category><![CDATA[cepheid]]></category>
		<category><![CDATA[classical cepheids]]></category>
		<category><![CDATA[dataset]]></category>
		<category><![CDATA[determinations]]></category>
		<category><![CDATA[epochs]]></category>
		<category><![CDATA[large magellanic cloud]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[literature data]]></category>
		<category><![CDATA[magellanic cloud]]></category>
		<category><![CDATA[magellanic system]]></category>
		<category><![CDATA[modulus]]></category>
		<category><![CDATA[overtone]]></category>
		<category><![CDATA[parallax]]></category>
		<category><![CDATA[period range]]></category>
		<category><![CDATA[photometry]]></category>
		<category><![CDATA[time series]]></category>
		<category><![CDATA[variable star]]></category>
		<category><![CDATA[zero point]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/the-vmc-survey-v-first-results-for-classical-cepheids-replacement/</guid>
		<description><![CDATA[The VISTA Magellanic Cloud (VMC, PI M.R. Cioni) survey is collecting deep Ks-band time-series photometry of the pulsating variable stars hosted by the system formed by the two Magellanic Clouds (MCs) and the &#8220;bridge&#8221; connecting them. In this paper we present the first results for Classical Cepheids, from the VMC observations of two fields in [...]]]></description>
			<content:encoded><![CDATA[<p>The VISTA Magellanic Cloud (VMC, PI M.R. Cioni) survey is collecting deep Ks-band time-series photometry of the pulsating variable stars hosted by the system formed by the two Magellanic Clouds (MCs) and the &#8220;bridge&#8221; connecting them. In this paper we present the first results for Classical Cepheids, from the VMC observations of two fields in the Large Magellanic Cloud (LMC). The VMC Ks-band light curves of the Cepheids are well sampled (12-epochs) and of excellent precision. We were able to measure for the first time the Ks magnitude of the faintest Classical Cepheids in the LMC (Ks\sim17.5 mag), which are mostly pulsating in the First Overtone (FO) mode, and to obtain FO Period-Luminosity (PL), Period-Wesenheit (PW), and Period-Luminosity-Color (PLC) relations, spanning the full period range from 0.25 to 6 day. Since the longest period Cepheid in our dataset has a variability period of 23 day, we have complemented our sample with literature data for brighter F Cepheids. On this basis we have built a PL relation in the Ks band that, for the first time, includes short period pulsators, and spans the whole range from 1.6 to 100 days in period. We also provide the first ever empirical PW and PLC relations using the (V-Ks) color and time-series Ks photometry. The very small dispersion (\sim0.07 mag) of these relations makes them very well suited to study the three-dimensional (3D) geometry of the Magellanic system. The use of &#8220;direct&#8221; (parallax- and Baade-Wesselink- based) distance measurements to both Galactic and LMC Cepheids, allowed us to calibrate the zero points of the PL, PW, and PLC relations obtained in this paper, and in turn to estimate an absolute distance modulus of (m-M)0=18.46\pm0.03 for the LMC. This result is in agreement with most of the latest literature determinations based on Classical Cepheids.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/the-vmc-survey-v-first-results-for-classical-cepheids-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>The parsec-scale jet of PKS 1749+096 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/the-parsec-scale-jet-of-pks-1749096-replacement/</link>
		<comments>http://voxcharta.org/2012/05/20/the-parsec-scale-jet-of-pks-1749096-replacement/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:32:22 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bimodal distribution]]></category>
		<category><![CDATA[bl lac objects]]></category>
		<category><![CDATA[coincidence]]></category>
		<category><![CDATA[distinct component]]></category>
		<category><![CDATA[doppler]]></category>
		<category><![CDATA[epochs]]></category>
		<category><![CDATA[flare]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[inverse compton]]></category>
		<category><![CDATA[jet parameters]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[lorentz factor]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[morphology]]></category>
		<category><![CDATA[motion]]></category>
		<category><![CDATA[new jet]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectral property]]></category>
		<category><![CDATA[target]]></category>
		<category><![CDATA[variability]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/the-parsec-scale-jet-of-pks-1749096-replacement/</guid>
		<description><![CDATA[PKS 1749+096 is a BL Lac object showing weak extended jet emission to the northeast of the compact VLBI core on parsec scales. We aim at better understanding the jet kinematics and variability of this source and finding clues that may applicable to other BL Lac objects. The jet was studied with multi-epoch multi-frequency high-resolution [...]]]></description>
			<content:encoded><![CDATA[<p>PKS 1749+096 is a BL Lac object showing weak extended jet emission to the northeast of the compact VLBI core on parsec scales. We aim at better understanding the jet kinematics and variability of this source and finding clues that may applicable to other BL Lac objects. The jet was studied with multi-epoch multi-frequency high-resolution VLBI observations. The jet is characterized by a one-sided curved morphology at all epochs and all frequencies. The VLBI core, located at the southern end of the jet, was identified based on its spectral properties. The equipartition magnetic field of the core was investigated, through which we derived a Doppler factor of 5, largely consistent with that derived from kinematics (component C5). The study of the detailed jet kinematics at 22 and 15 GHz, spanning a period of more than 10 years, indicates the possible existence of a bimodal distribution of the jet apparent speed. Ballistic and non-ballistic components are found to coexist in the jet. Superluminal motions in the range of 5-21 c were measured in 11 distinct components. We estimated the physical jet parameters with the minimum Lorentz factor of 10.2 and Doppler factors in the range of 10.2-20.4 (component C5). The coincidence in time of the component&#8217;s ejection and flares supports the idea that, at least in PKS 1749+096, ejection of new jet components is connected with major outbursts in flux density. For the best-traced component (C5) we found that the flux density decays rapidly as it travels downstream the jet, accompanied by a steepening of its spectra, which argues in favor of a contribution of inverse Compton cooling. These properties make PKS 1749+096 a suitable target for an intensive monitoring to decipher the variability phenomenon of BL Lac objects.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/the-parsec-scale-jet-of-pks-1749096-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Warm Dark Matter in Low Scale Left-Right Theory [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/warm-dark-matter-in-low-scale-left-right-theory-replacement/</link>
		<comments>http://voxcharta.org/2012/05/20/warm-dark-matter-in-low-scale-left-right-theory-replacement/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:31:52 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[boltzmann equation]]></category>
		<category><![CDATA[decay]]></category>
		<category><![CDATA[dilution]]></category>
		<category><![CDATA[disagreement]]></category>
		<category><![CDATA[early universe]]></category>
		<category><![CDATA[energy constraints]]></category>
		<category><![CDATA[entropy]]></category>
		<category><![CDATA[gauge boson]]></category>
		<category><![CDATA[keV]]></category>
		<category><![CDATA[lhc]]></category>
		<category><![CDATA[low energy]]></category>
		<category><![CDATA[numerical study]]></category>
		<category><![CDATA[overproduction]]></category>
		<category><![CDATA[qcd phase transition]]></category>
		<category><![CDATA[relic density]]></category>
		<category><![CDATA[symmetric theory]]></category>
		<category><![CDATA[tev scale]]></category>
		<category><![CDATA[viability]]></category>
		<category><![CDATA[viable candidate]]></category>
		<category><![CDATA[warm dark matter]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/warm-dark-matter-in-low-scale-left-right-theory-replacement/</guid>
		<description><![CDATA[We investigate the viability of having dark matter in the minimal left-right symmetric theory. We find the lightest right-handed neutrino with a mass around keV as the only viable candidate consistent with a TeV scale of left-right symmetry. In order to account for the correct relic density with such low scales, the thermal overproduction of [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate the viability of having dark matter in the minimal left-right symmetric theory. We find the lightest right-handed neutrino with a mass around keV as the only viable candidate consistent with a TeV scale of left-right symmetry. In order to account for the correct relic density with such low scales, the thermal overproduction of the dark matter in the early universe is compensated by a sufficient late entropy production due to late decay of heavier right-handed neutrinos. We point out that the presence of the right-handed charge-current interactions, operative around the QCD phase transition, has a crucial impact on the amount of dilution, as does the nature of the phase transition itself. A careful numerical study, employing the Boltzmann equations, reveals the existence of a narrow window for the right-handed gauge boson mass, possibly within the reach of LHC (in disagreement with a previous study). We also elaborate on a variety of astrophysical, cosmological and low energy constraints on this scenario.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/warm-dark-matter-in-low-scale-left-right-theory-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>[CII] line emission in massive star-forming galaxies at z=4.7 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/cii-line-emission-in-massive-star-forming-galaxies-at-z4-7-replacement/</link>
		<comments>http://voxcharta.org/2012/05/20/cii-line-emission-in-massive-star-forming-galaxies-at-z4-7-replacement/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:31:32 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acs]]></category>
		<category><![CDATA[alpha emitter]]></category>
		<category><![CDATA[big bang]]></category>
		<category><![CDATA[cii]]></category>
		<category><![CDATA[counterpart]]></category>
		<category><![CDATA[dust continuum emission]]></category>
		<category><![CDATA[fir luminosity]]></category>
		<category><![CDATA[gyr]]></category>
		<category><![CDATA[host galaxy]]></category>
		<category><![CDATA[line emission]]></category>
		<category><![CDATA[luminous object]]></category>
		<category><![CDATA[luminous quasar]]></category>
		<category><![CDATA[luminous star]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[millimeter]]></category>
		<category><![CDATA[mjy]]></category>
		<category><![CDATA[quasar]]></category>
		<category><![CDATA[smg]]></category>
		<category><![CDATA[starburst galaxy]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/cii-line-emission-in-massive-star-forming-galaxies-at-z4-7-replacement/</guid>
		<description><![CDATA[We present Atacama Large Millimeter/submillimeter Array (ALMA) observations of the [CII] 157.7micron fine structure line and thermal dust continuum emission from a pair of gas-rich galaxies at z=4.7, BR1202-0725. This system consists of a luminous quasar host galaxy and a bright submm galaxy (SMG), while a fainter star-forming galaxy is also spatially coincident within a [...]]]></description>
			<content:encoded><![CDATA[<p>We present Atacama Large Millimeter/submillimeter Array (ALMA) observations of the [CII] 157.7micron fine structure line and thermal dust continuum emission from a pair of gas-rich galaxies at z=4.7, BR1202-0725. This system consists of a luminous quasar host galaxy and a bright submm galaxy (SMG), while a fainter star-forming galaxy is also spatially coincident within a 4&#8243; (25 kpc) region. All three galaxies are detected in the submm continuum, indicating FIR luminosities in excess of 10^13 Lsun for the two most luminous objects. The SMG and the quasar host galaxy are both detected in [CII] line emission with luminosities, L([CII]) = (10.0 +/- 1.5)x10^9 Lsun and L([CII]) = (6.5+/-1.0)x10^9 Lsun, respectively. We estimate a luminosity ratio, L([CII])/L(FIR) = (8.3+/-1.2)x10^-4 for the starburst SMG to the North, and L([CII])/L(FIR) = (2.5+/-0.4)x10^-4 for the quasar host galaxy, in agreement with previous high-redshift studies that suggest lower [CII]-to-FIR luminosity ratios in quasars than in starburst galaxies. The third fainter object with a flux density, S(340GHz) = 1.9+/-0.3 mJy, is coincident with a Ly-Alpha emitter and is detected in HST ACS F775W and F814W images but has no clear counterpart in the H-band. Even if this third companion does not lie at a similar redshift to BR1202-0725, the quasar and the SMG represent an overdensity of massive, infrared luminous star-forming galaxies within 1.3 Gyr of the Big Bang.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/cii-line-emission-in-massive-star-forming-galaxies-at-z4-7-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Optimization by Smoothed Bandpass Calibration in Radio Spectroscopy [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/optimization-by-smoothed-bandpass-calibration-in-radio-spectroscopy-replacement/</link>
		<comments>http://voxcharta.org/2012/05/20/optimization-by-smoothed-bandpass-calibration-in-radio-spectroscopy-replacement/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:31:20 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[allan variance]]></category>
		<category><![CDATA[archival data]]></category>
		<category><![CDATA[blank sky]]></category>
		<category><![CDATA[conventional method]]></category>
		<category><![CDATA[dual beam]]></category>
		<category><![CDATA[integration time]]></category>
		<category><![CDATA[iriki]]></category>
		<category><![CDATA[otf]]></category>
		<category><![CDATA[radio spectroscopy]]></category>
		<category><![CDATA[receiving system]]></category>
		<category><![CDATA[scan pattern]]></category>
		<category><![CDATA[signal to noise ratio]]></category>
		<category><![CDATA[single beam]]></category>
		<category><![CDATA[spectral resolution]]></category>
		<category><![CDATA[system noise]]></category>
		<category><![CDATA[target source]]></category>
		<category><![CDATA[telescope time]]></category>
		<category><![CDATA[time efficiency]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/optimization-by-smoothed-bandpass-calibration-in-radio-spectroscopy-replacement/</guid>
		<description><![CDATA[We have developed the Smoothed Bandpass Calibration (SBC) method and the best suitable scan pattern to optimize radio spectroscopic observations. Adequate spectral smoothing is applied to the spectrum toward OFF-source blank sky adjacent to a target source direction for the purpose of bandpass correction. Because the smoothing process reduces noise, the integration time for OFF-source [...]]]></description>
			<content:encoded><![CDATA[<p>We have developed the Smoothed Bandpass Calibration (SBC) method and the best suitable scan pattern to optimize radio spectroscopic observations. Adequate spectral smoothing is applied to the spectrum toward OFF-source blank sky adjacent to a target source direction for the purpose of bandpass correction. Because the smoothing process reduces noise, the integration time for OFF-source scans can be reduced keeping the signal-to-noise ratio. Since the smoothing is not applied to ON-source scans, the spectral resolution for line features is kept. An optimal smoothing window is determined by bandpass flatness evaluated by Spectral Allan Variance (SAV). An efficient scan pattern is designed to the OFF-source scans within the bandpass stability timescale estimated by Time-based Allan Variance (TAV). We have tested the SBC using the digital spectrometer, VESPA, on the VERA Iriki station. For the targeted noise level of 5e-4 as a ratio to the system noise, the optimal smoothing window was 32 &#8211; 60 ch in the whole bandwidth of 1024 ch, and the optimal scan pattern was designed as a sequence of 70-s ON + 10-s OFF scan pairs. The noise level with the SBC was reduced by a factor of 1.74 compared with the conventional method. The total telescope time to achieve the goal with the SBC was 400 s, which was 1/3 of 1200 s required by the conventional way. Improvement in telescope time efficiency with the SBC was calculated as 3x, 2x and 1.3x for single-beam, dual-beam, and on-the-fly (OTF) scans, respectively. The SBC works to optimize scan patterns for observations from now, and also works to improve signal-to-noise ratios of archival data if ON- and OFF-source spectra are individually recorded, though the efficiency depends on the spectral stability of the receiving system.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/optimization-by-smoothed-bandpass-calibration-in-radio-spectroscopy-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<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>Deuterium at high-redshift: Primordial abundance in the zabs = 2.621 damped Ly-alpha system towards CTQ247</title>
		<link>http://voxcharta.org/2012/05/17/deuterium-at-high-redshift-primordial-abundance-in-the-zabs-2-621-damped-ly-alpha-system-towards-ctq247/</link>
		<comments>http://voxcharta.org/2012/05/17/deuterium-at-high-redshift-primordial-abundance-in-the-zabs-2-621-damped-ly-alpha-system-towards-ctq247/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:58:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[alpha system]]></category>
		<category><![CDATA[deuterium]]></category>
		<category><![CDATA[echelle spectrograph]]></category>
		<category><![CDATA[hi 5]]></category>
		<category><![CDATA[lyman alpha]]></category>
		<category><![CDATA[Measurement]]></category>
		<category><![CDATA[metallicity]]></category>
		<category><![CDATA[oxygen abundance]]></category>
		<category><![CDATA[signal to noise]]></category>
		<category><![CDATA[spectral resolution]]></category>
		<category><![CDATA[spectrum]]></category>
		<category><![CDATA[Telescope]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/deuterium-at-high-redshift-primordial-abundance-in-the-zabs-2-621-damped-ly-alpha-system-towards-ctq247/</guid>
		<description><![CDATA[The detection of neutral deuterium in the low-metallicity damped Lyman-{\alpha} system at zabs = 2.621 towards the quasar CTQ247 is reported. Using a high signal-to-noise and high spectral resolution (R = 60000) spectrum from the Very Large Telescope Ultraviolet and Visual Echelle Spectrograph, we precisely measure the deuterium-to-oxygen ratio log N(DI)/N(OI) = 0.74+/-0.04, as well [...]]]></description>
			<content:encoded><![CDATA[<p>The detection of neutral deuterium in the low-metallicity damped Lyman-{\alpha} system at zabs = 2.621 towards the quasar CTQ247 is reported. Using a high signal-to-noise and high spectral resolution (R = 60000) spectrum from the Very Large Telescope Ultraviolet and Visual Echelle Spectrograph, we precisely measure the deuterium-to-oxygen ratio log N(DI)/N(OI) = 0.74+/-0.04, as well as the overall oxygen abundance, log N(OI)/N(HI)=-5.29+/-0.10 (or equivalently [O/H]=-1.99+/-0.10 with respect to the solar value). Assuming uniform metallicity throughout the system, our measurement translates to (D/H) = (2.8+0.8 -0.6)x10^-5. This ratio is consistent within errors (&lt;0.4sigma) with the primordial ratio, (D/H)p = (2.59+/-0.15)x10^-5, predicted by standard Big-Bang Nucleosynthesis using the WMAP7 value of the cosmological density of baryons (100 Omega_b h^2 = 2.249+/-0.056). The DI absorption lines are observed to be broader than the OI absorption lines. From a consistent fit of the profiles we derive the turbulent broadening to be 5.2 km/s and the temperature of the gas to be T = 8800+/-1500 K, corresponding to a warm neutral medium.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/deuterium-at-high-redshift-primordial-abundance-in-the-zabs-2-621-damped-ly-alpha-system-towards-ctq247/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>
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		<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>
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		<item>
		<title>Cosmic Rays and Stochastic Magnetic Reconnection in the Heliotail</title>
		<link>http://voxcharta.org/2012/05/17/cosmic-rays-and-stochastic-magnetic-reconnection-in-the-heliotail/</link>
		<comments>http://voxcharta.org/2012/05/17/cosmic-rays-and-stochastic-magnetic-reconnection-in-the-heliotail/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:56:13 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration processes]]></category>
		<category><![CDATA[anisotropy]]></category>
		<category><![CDATA[arrival direction]]></category>
		<category><![CDATA[convective processes]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[diffusion model]]></category>
		<category><![CDATA[energetic particle]]></category>
		<category><![CDATA[energy dependence]]></category>
		<category><![CDATA[energy spectrum]]></category>
		<category><![CDATA[experimental evidence]]></category>
		<category><![CDATA[galactic cosmic rays]]></category>
		<category><![CDATA[heliosphere]]></category>
		<category><![CDATA[interstellar medium]]></category>
		<category><![CDATA[magnetic reconnection]]></category>
		<category><![CDATA[parsec]]></category>
		<category><![CDATA[shock acceleration]]></category>
		<category><![CDATA[smearing]]></category>
		<category><![CDATA[supernova remnant]]></category>
		<category><![CDATA[tev energies]]></category>
		<category><![CDATA[wind gradient]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/cosmic-rays-and-stochastic-magnetic-reconnection-in-the-heliotail/</guid>
		<description><![CDATA[Galactic cosmic rays are believed to be generated by diffusive shock acceleration processes in Supernova Remnants, and the arrival direction is likely determined by the distribution of their sources throughout the Galaxy, in particular by the nearest and youngest ones. Transport to Earth through the interstellar medium is expected to affect the cosmic ray properties [...]]]></description>
			<content:encoded><![CDATA[<p>Galactic cosmic rays are believed to be generated by diffusive shock acceleration processes in Supernova Remnants, and the arrival direction is likely determined by the distribution of their sources throughout the Galaxy, in particular by the nearest and youngest ones. Transport to Earth through the interstellar medium is expected to affect the cosmic ray properties as well. However, the observed anisotropy of TeV cosmic rays and its energy dependence cannot be explained with diffusion models of particle propagation in the Galaxy. Within a distance of a few parsec, diffusion regime is not valid and particles with energy below about 100 TeV must be influenced by the heliosphere and its elongated tail. The observation of a highly significant localized excess region of cosmic rays from the apparent direction of the downstream interstellar flow at 1-10 TeV energies might provide the first experimental evidence that the heliotail can affect the transport of energetic particles. In particular, TeV cosmic rays propagating through the heliotail interact with the 100-300 AU wide magnetic field polarity domains generated by the 11 year cycles. Since the strength of non-linear convective processes is expected to be larger than viscous damping, the plasma in the heliotail is turbulent. Where magnetic field domains converge on each other due to solar wind gradient, stochastic magnetic reconnection likely occurs. Such processes may be efficient enough to re-accelerate a fraction of TeV particles as long as scattering processes are not strong. Therefore the fractional excess of TeV cosmic rays from the narrow region toward the heliotail direction traces sightlines with the lowest smearing scattering effects, that can also explain the observation of a harder than average energy spectrum.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/cosmic-rays-and-stochastic-magnetic-reconnection-in-the-heliotail/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Constraining the Circumbinary Envelope of Z CMa via imaging polarimetry</title>
		<link>http://voxcharta.org/2012/05/17/constraining-the-circumbinary-envelope-of-z-cma-via-imaging-polarimetry/</link>
		<comments>http://voxcharta.org/2012/05/17/constraining-the-circumbinary-envelope-of-z-cma-via-imaging-polarimetry/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:55:53 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[beam of light]]></category>
		<category><![CDATA[binary system]]></category>
		<category><![CDATA[cma]]></category>
		<category><![CDATA[cocoon]]></category>
		<category><![CDATA[dual beam]]></category>
		<category><![CDATA[herbig]]></category>
		<category><![CDATA[jets]]></category>
		<category><![CDATA[low density]]></category>
		<category><![CDATA[micro jet]]></category>
		<category><![CDATA[optical wavelength]]></category>
		<category><![CDATA[ori]]></category>
		<category><![CDATA[outburst]]></category>
		<category><![CDATA[pencil]]></category>
		<category><![CDATA[polarimeter]]></category>
		<category><![CDATA[polarimetry]]></category>
		<category><![CDATA[polarization angle]]></category>
		<category><![CDATA[preferred orientation]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[variability]]></category>
		<category><![CDATA[variable geometry]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/constraining-the-circumbinary-envelope-of-z-cma-via-imaging-polarimetry/</guid>
		<description><![CDATA[Z CMa is a complex binary system, composed of a Herbig Be and an FU Ori star. The Herbig star is surrounded by a dust cocoon of variable geometry, and the whole system is surrounded by an infalling envelope. Previous spectropolarimetric observations have reported a preferred orientation of the polarization angle, perpendicular to the direction [...]]]></description>
			<content:encoded><![CDATA[<p>Z CMa is a complex binary system, composed of a Herbig Be and an FU Ori star. The Herbig star is surrounded by a dust cocoon of variable geometry, and the whole system is surrounded by an infalling envelope. Previous spectropolarimetric observations have reported a preferred orientation of the polarization angle, perpendicular to the direction of a large, parsec-sized jet associated with the Herbig star. The variability in the amount of polarized light has been associated to changes in the geometry of the dust cocoon that surrounds the Herbig star. We aim to constrain the properties of Z CMa by means of imaging polarimetry at optical wavelengths. Using ExPo, a dual-beam imaging polarimeter which operates at optical wavelengths, we have obtained imaging (linear) polarimetric data of Z CMa. Our observations were secured during the return to quiescence after the 2008 outburst. We detect three polarized features over Z CMa. Two of these features are related to the two jets reported in this system: the large jet associated to the Herbig star, and the micro-jet associated to the FU Ori star. Our results suggest that the micro-jet extends to a distance ten times larger than reported in previous studies. The third feature suggests the presence of a hole in the dust cocoon that surrounds the Herbig star of this system. According to our simulations, this hole can produce a pencil beam of light that we see scattered off the low-density envelope surrounding the system.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/constraining-the-circumbinary-envelope-of-z-cma-via-imaging-polarimetry/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>A new, precise measurement of the primordial abundance of Deuterium</title>
		<link>http://voxcharta.org/2012/05/17/a-new-precise-measurement-of-the-primordial-abundance-of-deuterium/</link>
		<comments>http://voxcharta.org/2012/05/17/a-new-precise-measurement-of-the-primordial-abundance-of-deuterium/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:55:39 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abundance]]></category>
		<category><![CDATA[accurate determination]]></category>
		<category><![CDATA[angular power spectrum]]></category>
		<category><![CDATA[bbn]]></category>
		<category><![CDATA[biases]]></category>
		<category><![CDATA[big bang nucleosynthesis]]></category>
		<category><![CDATA[CMB]]></category>
		<category><![CDATA[consistent manner]]></category>
		<category><![CDATA[cosmic microwave background]]></category>
		<category><![CDATA[deuterium]]></category>
		<category><![CDATA[dla]]></category>
		<category><![CDATA[endeavour]]></category>
		<category><![CDATA[high quality]]></category>
		<category><![CDATA[literature]]></category>
		<category><![CDATA[lyman alpha]]></category>
		<category><![CDATA[nuclear reaction]]></category>
		<category><![CDATA[omega]]></category>
		<category><![CDATA[physics]]></category>
		<category><![CDATA[precise measurement]]></category>
		<category><![CDATA[systematic error]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/a-new-precise-measurement-of-the-primordial-abundance-of-deuterium/</guid>
		<description><![CDATA[The metal-poor damped Lyman alpha (DLA) system at z = 3.04984 in the QSO SDSSJ1419+0829 has near-ideal properties for an accurate determination of the primordial abundance of deuterium, (D/H)_p. We have analysed a high-quality spectrum of this object with software specifically designed to deduce the best fitting value of D/H and to assess comprehensively the [...]]]></description>
			<content:encoded><![CDATA[<p>The metal-poor damped Lyman alpha (DLA) system at z = 3.04984 in the QSO SDSSJ1419+0829 has near-ideal properties for an accurate determination of the primordial abundance of deuterium, (D/H)_p. We have analysed a high-quality spectrum of this object with software specifically designed to deduce the best fitting value of D/H and to assess comprehensively the random and systematic errors affecting this determination. We find (D/H)_DLA = (2.535 +/-0.05) x 10^(-5), which in turn implies Omega_b h^2 = 0.0223 +/- 0.0009, in very good agreement with Omega_b h^2 (CMB) = 0.0222 +/- 0.0004 deduced from the angular power spectrum of the cosmic microwave background. If the value in this DLA is indeed the true (D/H)_p produced by Big-Bang nucleosynthesis (BBN), there may be no need to invoke non-standard physics nor early astration of D to bring together Omega_b h^2 (BBN) and Omega_b h^2 (CMB). The scatter between most of the reported values of (D/H)_p in the literature may be due largely to unaccounted systematic errors and biases. Further progress in this area will require a homogeneous set of data comparable to those reported here and analysed in a self-consistent manner. Such an endeavour, while observationally demanding, has the potential of improving our understanding of BBN physics, including the relevant nuclear reactions, and the subsequent processing of 4He and 7Li through stars.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/a-new-precise-measurement-of-the-primordial-abundance-of-deuterium/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>IDCS J1426+3508: Discovery of a Massive, IR-Selected Galaxy Cluster at z = 1.75</title>
		<link>http://voxcharta.org/2012/05/17/idcs-j14263508-discovery-of-a-massive-ir-selected-galaxy-cluster-at-z-1-75/</link>
		<comments>http://voxcharta.org/2012/05/17/idcs-j14263508-discovery-of-a-massive-ir-selected-galaxy-cluster-at-z-1-75/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:55:25 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[chandra data]]></category>
		<category><![CDATA[cluster survey]]></category>
		<category><![CDATA[diameter]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[distant cluster]]></category>
		<category><![CDATA[ergs]]></category>
		<category><![CDATA[galaxy cluster]]></category>
		<category><![CDATA[hubble space telescope]]></category>
		<category><![CDATA[keck observatory]]></category>
		<category><![CDATA[massive cluster]]></category>
		<category><![CDATA[massive galaxy]]></category>
		<category><![CDATA[point source]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/idcs-j14263508-discovery-of-a-massive-ir-selected-galaxy-cluster-at-z-1-75/</guid>
		<description><![CDATA[We report the discovery of an IR-selected massive galaxy cluster in the IRAC Distant Cluster Survey (IDCS). We present new data from the Hubble Space Telescope and the W. M. Keck Observatory that spectroscopically confirm IDCS J1426+3508 at z=1.75. Moreover, the cluster is detected in archival Chandra data as an extended X-ray source, comprising 54 [...]]]></description>
			<content:encoded><![CDATA[<p>We report the discovery of an IR-selected massive galaxy cluster in the IRAC Distant Cluster Survey (IDCS). We present new data from the Hubble Space Telescope and the W. M. Keck Observatory that spectroscopically confirm IDCS J1426+3508 at z=1.75. Moreover, the cluster is detected in archival Chandra data as an extended X-ray source, comprising 54 counts after the removal of point sources. We calculate an X-ray luminosity of L{0.5-2 keV} = (5.5 +/- 1.2) X 1e44 ergs/s within r = 60 arcsec (~1 Mpc diameter), which implies M_{200,L_x} = (5.6 +/- 1.6) X 1e14 Msun. IDCS J1426+3508 appears to be an exceptionally massive cluster for its redshift.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/idcs-j14263508-discovery-of-a-massive-ir-selected-galaxy-cluster-at-z-1-75/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>IDCS J1426.5+3508: Sunyaev-Zel&#8217;dovich Measurement of a Massive IR-selected Cluster at z=1.75</title>
		<link>http://voxcharta.org/2012/05/17/idcs-j1426-53508-sunyaev-zeldovich-measurement-of-a-massive-ir-selected-cluster-at-z1-75/</link>
		<comments>http://voxcharta.org/2012/05/17/idcs-j1426-53508-sunyaev-zeldovich-measurement-of-a-massive-ir-selected-cluster-at-z1-75/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:55:07 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[carma]]></category>
		<category><![CDATA[cluster survey]]></category>
		<category><![CDATA[decrement]]></category>
		<category><![CDATA[distant cluster]]></category>
		<category><![CDATA[galaxy cluster]]></category>
		<category><![CDATA[infrared techniques]]></category>
		<category><![CDATA[massive galaxy]]></category>
		<category><![CDATA[Measurement]]></category>
		<category><![CDATA[msun]]></category>
		<category><![CDATA[precursor]]></category>
		<category><![CDATA[probability]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[statistical study]]></category>
		<category><![CDATA[survey]]></category>
		<category><![CDATA[universe]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[Zel]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/idcs-j1426-53508-sunyaev-zeldovich-measurement-of-a-massive-ir-selected-cluster-at-z1-75/</guid>
		<description><![CDATA[We report 31 GHz CARMA observations of IDCS J1426.5+3508, an infrared-selected galaxy cluster at z = 1.75. A Sunyaev-Zel&#8217;dovich decrement is detected towards this cluster, indicating a total mass of M200 = (4.3 +/- 1.1) x 10^{14} Msun in agreement with the approximate X-ray mass of ~5 x 10^{14} Msun. IDCS J1426.5+3508 is by far [...]]]></description>
			<content:encoded><![CDATA[<p>We report 31 GHz CARMA observations of IDCS J1426.5+3508, an infrared-selected galaxy cluster at z = 1.75. A Sunyaev-Zel&#8217;dovich decrement is detected towards this cluster, indicating a total mass of M200 = (4.3 +/- 1.1) x 10^{14} Msun in agreement with the approximate X-ray mass of ~5 x 10^{14} Msun. IDCS J1426.5+3508 is by far the most distant cluster yet detected via the Sunyaev-Zel&#8217;dovich effect, and the most massive z &gt;= 1.4 galaxy cluster found to date. Despite the mere ~1% probability of finding it in the 8.82 deg^2 IRAC Distant Cluster Survey, IDCS J1426.5+3508 is not completely unexpected in LCDM once the area of large, existing surveys is considered. IDCS J1426.5+3508 is, however, among the rarest, most extreme clusters ever discovered, and indeed is an evolutionary precursor to the most massive known clusters at all redshifts. We discuss how imminent, highly sensitive Sunyaev-Zel&#8217;dovich experiments will complement infrared techniques for statistical studies of the formation of the most massive galaxy clusters in the z &gt; 1.5 Universe, including potential precursors to IDCS J1426.5+3508.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/idcs-j1426-53508-sunyaev-zeldovich-measurement-of-a-massive-ir-selected-cluster-at-z1-75/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>IDCS J1426.5+3508: Cosmological implications of a massive, strong lensing cluster at Z = 1.75</title>
		<link>http://voxcharta.org/2012/05/17/idcs-j1426-53508-cosmological-implications-of-a-massive-strong-lensing-cluster-at-z-1-75/</link>
		<comments>http://voxcharta.org/2012/05/17/idcs-j1426-53508-cosmological-implications-of-a-massive-strong-lensing-cluster-at-z-1-75/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:54:51 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[arc]]></category>
		<category><![CDATA[background field]]></category>
		<category><![CDATA[cluster]]></category>
		<category><![CDATA[cluster galaxy]]></category>
		<category><![CDATA[cluster survey]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[cosmological implications]]></category>
		<category><![CDATA[curvature]]></category>
		<category><![CDATA[discrepancy]]></category>
		<category><![CDATA[galaxy cluster]]></category>
		<category><![CDATA[geq]]></category>
		<category><![CDATA[lens system]]></category>
		<category><![CDATA[lensed galaxy]]></category>
		<category><![CDATA[m200]]></category>
		<category><![CDATA[massive galaxy]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[statistic results]]></category>
		<category><![CDATA[structure formation]]></category>
		<category><![CDATA[Zel]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/idcs-j1426-53508-cosmological-implications-of-a-massive-strong-lensing-cluster-at-z-1-75/</guid>
		<description><![CDATA[The galaxy cluster IDCS J1426.5+3508 at z = 1.75 is the most massive galaxy cluster yet discovered at z &#62; 1.4 and the first cluster at this epoch for which the Sunyaev-Zel&#8217;Dovich effect has been observed. In this paper we report on the discovery with HST imaging of a giant arc associated with this cluster. [...]]]></description>
			<content:encoded><![CDATA[<p>The galaxy cluster IDCS J1426.5+3508 at z = 1.75 is the most massive galaxy cluster yet discovered at z &gt; 1.4 and the first cluster at this epoch for which the Sunyaev-Zel&#8217;Dovich effect has been observed. In this paper we report on the discovery with HST imaging of a giant arc associated with this cluster. The curvature of the arc suggests that the lensing mass is nearly coincident with the brightest cluster galaxy, and the color is consistent with the arc being a star-forming galaxy. We compare the constraint on M200 based upon strong lensing with Sunyaev-Zel&#8217;Dovich results, finding that the two are consistent if the redshift of the arc is z &gt; 3. Finally, we explore the cosmological implications of this system, considering the likelihood of the existence of a strongly lensing galaxy cluster at this epoch in an LCDM universe. While the existence of the cluster itself can potentially be accomodated if one considers the entire volume covered at this redshift by all current high-redshift cluster surveys, the existence of this strongly lensed galaxy greatly exacerbates the long-standing giant arc problem. For standard LCDM structure formation and observed background field galaxy counts this lens system should not exist. Specifically, there should be no giant arcs in the entire sky as bright in F814W as the observed arc for clusters at z \geq 1.75, and only \sim 0.3 as bright in F160W as the observed arc. If we relax the redshift constraint to consider all clusters at z \geq 1.5, the expected number of giant arcs rises to \sim15 in F160W, but the number of giant arcs of this brightness in F814W remains zero. These arc statistic results are independent of the mass of IDCS J1426.5+3508. We consider possible explanations for this discrepancy.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/idcs-j1426-53508-cosmological-implications-of-a-massive-strong-lensing-cluster-at-z-1-75/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<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>Spherically Symmetric Inflation [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/17/spherically-symmetric-inflation-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/17/spherically-symmetric-inflation-cross-listing/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:54:15 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[conclusion]]></category>
		<category><![CDATA[generalization]]></category>
		<category><![CDATA[geometry]]></category>
		<category><![CDATA[horizon]]></category>
		<category><![CDATA[inflation]]></category>
		<category><![CDATA[initial condition]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[scalar field]]></category>
		<category><![CDATA[spatial distribution]]></category>
		<category><![CDATA[spherical symmetry]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/spherically-symmetric-inflation-cross-listing/</guid>
		<description><![CDATA[It is shown in this letter that in the framework of an inhomogeneous geometry and a massive non self-interacting scalar field with spherical symmetry, one needs a homogeneous patch bigger than a dizaine of horizons in order to start inflation. The results are completly independent of initial conditions on the spatial distribution of the scalar [...]]]></description>
			<content:encoded><![CDATA[<p>It is shown in this letter that in the framework of an inhomogeneous geometry and a massive non self-interacting scalar field with spherical symmetry, one needs a homogeneous patch bigger than a dizaine of horizons in order to start inflation. The results are completly independent of initial conditions on the spatial distribution of the scalar field. The initial condition on the metric parameters are also justified. This is a generalization of the results obtained in Ref.[1], showing that their conclusions are rather robust.</p>
]]></content:encoded>
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		<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>
		<item>
		<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>Constraints on model atmospheres from complex asteroseismology of the \beta Cephei stars</title>
		<link>http://voxcharta.org/2012/05/17/constraints-on-model-atmospheres-from-complex-asteroseismology-of-the-beta-cephei-stars/</link>
		<comments>http://voxcharta.org/2012/05/17/constraints-on-model-atmospheres-from-complex-asteroseismology-of-the-beta-cephei-stars/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:52:56 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[beta]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[gamma]]></category>
		<category><![CDATA[kurucz]]></category>
		<category><![CDATA[model atmosphere]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[peg]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/constraints-on-model-atmospheres-from-complex-asteroseismology-of-the-beta-cephei-stars/</guid>
		<description><![CDATA[Using the method termed complex asteroseismology, we derive constraints on model atmospheres, in particular, on the NLTE effects. We fit simultaneously pulsational frequencies and the corresponding values of the nonadiabatic complex parameter f for the four \beta Cephei stars: \theta Oph, \nu Eri, \gamma Peg and 12 Lac. The LTE Kurucz models and the BSTAR2006 [...]]]></description>
			<content:encoded><![CDATA[<p>Using the method termed complex asteroseismology, we derive constraints on model atmospheres, in particular, on the NLTE effects. We fit simultaneously pulsational frequencies and the corresponding values of the nonadiabatic complex parameter f for the four \beta Cephei stars: \theta Oph, \nu Eri, \gamma Peg and 12 Lac. The LTE Kurucz models and the BSTAR2006 NLTE models are tested.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/constraints-on-model-atmospheres-from-complex-asteroseismology-of-the-beta-cephei-stars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Studying the hybrid pulsator 12 Lacertae: mode identification and complex seismic modelling</title>
		<link>http://voxcharta.org/2012/05/17/studying-the-hybrid-pulsator-12-lacertae-mode-identification-and-complex-seismic-modelling/</link>
		<comments>http://voxcharta.org/2012/05/17/studying-the-hybrid-pulsator-12-lacertae-mode-identification-and-complex-seismic-modelling/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:52:25 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[atmosphere]]></category>
		<category><![CDATA[chemical composition]]></category>
		<category><![CDATA[hybrid]]></category>
		<category><![CDATA[mode frequency]]></category>
		<category><![CDATA[mode identification]]></category>
		<category><![CDATA[parameter effects]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/studying-the-hybrid-pulsator-12-lacertae-mode-identification-and-complex-seismic-modelling/</guid>
		<description><![CDATA[We present identification of the mode degree, l, for all observed frequencies of 12 Lac and results of seismic modelling which consists in fitting simultaneously the centroid mode frequencies and the corresponding values of the complex nonadiabatic f-parameter. Effects of chemical composition, opacities, core overshooting and non-LTE atmospheres were taken into account.
]]></description>
			<content:encoded><![CDATA[<p>We present identification of the mode degree, l, for all observed frequencies of 12 Lac and results of seismic modelling which consists in fitting simultaneously the centroid mode frequencies and the corresponding values of the complex nonadiabatic f-parameter. Effects of chemical composition, opacities, core overshooting and non-LTE atmospheres were taken into account.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/studying-the-hybrid-pulsator-12-lacertae-mode-identification-and-complex-seismic-modelling/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Constraining stellar assembly and AGN feedback at the peak epoch of star formation</title>
		<link>http://voxcharta.org/2012/05/17/constraining-stellar-assembly-and-agn-feedback-at-the-peak-epoch-of-star-formation/</link>
		<comments>http://voxcharta.org/2012/05/17/constraining-stellar-assembly-and-agn-feedback-at-the-peak-epoch-of-star-formation/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:51:50 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[star formation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/constraining-stellar-assembly-and-agn-feedback-at-the-peak-epoch-of-star-formation/</guid>
		<description><![CDATA[We study stellar assembly and feedback from active galactic nuclei (AGN) around the epoch of peak star formation (1&#60;z&#60;2), by comparing hydrodynamic simulations to rest-frame UV-optical galaxy colours from the Wide Field Camera 3 (WFC3) Early-Release Science (ERS) Programme. Our Adaptive Mesh Refinement simulations include metal-dependent radiative cooling, star formation, kinetic outflows due to supernova [...]]]></description>
			<content:encoded><![CDATA[<p>We study stellar assembly and feedback from active galactic nuclei (AGN) around the epoch of peak star formation (1&lt;z&lt;2), by comparing hydrodynamic simulations to rest-frame UV-optical galaxy colours from the Wide Field Camera 3 (WFC3) Early-Release Science (ERS) Programme. Our Adaptive Mesh Refinement simulations include metal-dependent radiative cooling, star formation, kinetic outflows due to supernova explosions, and feedback from supermassive black holes. Our model assumes that when gas accretes onto black holes, a fraction of the energy is used to form either thermal winds or sub-relativistic momentum-imparting collimated jets, depending on the accretion rate. We find that the predicted rest-frame UV-optical colours of galaxies in the model that includes AGN feedback is in broad agreement with the observed colours of the WFC3 ERS sample at 1&lt;z&lt;2. The predicted number of massive galaxies also matches well with observations in this redshift range. However, the massive galaxies are predicted to show higher levels of residual star formation activity than the observational estimates, suggesting the need for further suppression of star formation without significantly altering the stellar mass function. We discuss possible improvements, involving faster stellar assembly through enhanced star formation during galaxy mergers while star formation at the peak epoch is still modulated by the AGN feedback.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/constraining-stellar-assembly-and-agn-feedback-at-the-peak-epoch-of-star-formation/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Progenitor mass constraints for core-collapse supernovae from correlations with host galaxy star formation</title>
		<link>http://voxcharta.org/2012/05/17/progenitor-mass-constraints-for-core-collapse-supernovae-from-correlations-with-host-galaxy-star-formation/</link>
		<comments>http://voxcharta.org/2012/05/17/progenitor-mass-constraints-for-core-collapse-supernovae-from-correlations-with-host-galaxy-star-formation/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:51:34 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[alpha emission]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[core collapse supernovae]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[host galaxy]]></category>
		<category><![CDATA[star formation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/progenitor-mass-constraints-for-core-collapse-supernovae-from-correlations-with-host-galaxy-star-formation/</guid>
		<description><![CDATA[Using H-alpha emission as a tracer of on-going (&#60;16 Myr old) and near-UV emission as a tracer of recent (16-100 Myr old) star formation (SF), we present constraints on core-collapse (CC) supernova (SN) progenitors through their association with SF regions. We present statistics of a large sample of SNe; 163.5 type II (58 IIP, 13 [...]]]></description>
			<content:encoded><![CDATA[<p>Using H-alpha emission as a tracer of on-going (&lt;16 Myr old) and near-UV emission as a tracer of recent (16-100 Myr old) star formation (SF), we present constraints on core-collapse (CC) supernova (SN) progenitors through their association with SF regions. We present statistics of a large sample of SNe; 163.5 type II (58 IIP, 13 IIL, 13.5 IIb, 19 IIn and 12 &#039;impostors&#039;) and 96.5 type Ib/c (39.5 Ib and 52 Ic). Using pixel statistics our main findings and conclusions are: 1) An increasing progenitor mass sequence is observed, implied from an increasing association of SNe to host galaxy H-alpha emission. This commences with the type Ia (SNIa) showing the weakest association, followed by the SNII, then the SNIb, with the SNIc showing the strongest correlation to SF regions. Thus our progenitor mass sequence runs Ia-II-Ib-Ic. 2) Overall SNIbc are found to occur nearer to bright HII regions than SNII. This implies that the former have shorter stellar lifetimes thus arising from more massive progenitor stars. 3) While SNIIP do not closely follow the on-going SF, they accurately trace the recent formation. This implies that their progenitors arise from stars at the low end of the CC SN mass sequence, consistent with direct detections of progenitors in pre-explosion imaging. 4) Similarly SNIIn trace recent but not the on-going SF. This implies that, contrary to the general consensus, the majority of these SNe do not arise from the most massive stars. Results and constraints are also presented for the less numerous SNIIL, IIb, and &#039;impostors&#039;. Finally we present analysis of possible biases in the data, the results of which argue strongly against any selection effects that could explain the relative excess of SNIbc within bright HII regions. Thus intrinsic progenitor differences in the sense of the mass sequence we propose remain the most plausible explanation of our findings.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/progenitor-mass-constraints-for-core-collapse-supernovae-from-correlations-with-host-galaxy-star-formation/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A solar tornado observed by AIA/SDO: Rotational flow and evolution of magnetic helicity in a prominence and cavity</title>
		<link>http://voxcharta.org/2012/05/17/a-solar-tornado-observed-by-aiasdo-rotational-flow-and-evolution-of-magnetic-helicity-in-a-prominence-and-cavity/</link>
		<comments>http://voxcharta.org/2012/05/17/a-solar-tornado-observed-by-aiasdo-rotational-flow-and-evolution-of-magnetic-helicity-in-a-prominence-and-cavity/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:51:13 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[aia]]></category>
		<category><![CDATA[blob]]></category>
		<category><![CDATA[cavity]]></category>
		<category><![CDATA[coherent rotation]]></category>
		<category><![CDATA[complexity]]></category>
		<category><![CDATA[cyclone]]></category>
		<category><![CDATA[fades]]></category>
		<category><![CDATA[helical structure]]></category>
		<category><![CDATA[helium lines]]></category>
		<category><![CDATA[helix axis]]></category>
		<category><![CDATA[hydrogen]]></category>
		<category><![CDATA[line of sight]]></category>
		<category><![CDATA[magnetic helicity]]></category>
		<category><![CDATA[narrow loop]]></category>
		<category><![CDATA[observatory]]></category>
		<category><![CDATA[prominence]]></category>
		<category><![CDATA[sdo]]></category>
		<category><![CDATA[streaks]]></category>
		<category><![CDATA[telescopes]]></category>
		<category><![CDATA[tornado]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/a-solar-tornado-observed-by-aiasdo-rotational-flow-and-evolution-of-magnetic-helicity-in-a-prominence-and-cavity/</guid>
		<description><![CDATA[During 2011/09/24, as observed by the Atmospheric Imaging Assembly (AIA) instrument of the Solar Dynamic Observatory (SDO) and ground-based \Ha\ telescopes, a prominence and associated cavity appeared above the southwest limb. On 2011/09/25 8:00UT material flows upwards from the prominence core along a narrow loop-like structure, accompanied by a rise ($\geq$50,000km) of the prominence core [...]]]></description>
			<content:encoded><![CDATA[<p>During 2011/09/24, as observed by the Atmospheric Imaging Assembly (AIA) instrument of the Solar Dynamic Observatory (SDO) and ground-based \Ha\ telescopes, a prominence and associated cavity appeared above the southwest limb. On 2011/09/25 8:00UT material flows upwards from the prominence core along a narrow loop-like structure, accompanied by a rise ($\geq$50,000km) of the prominence core and the loop. As the loop fades by 10:00, small blobs and streaks of varying brightness rotate around the top part of the prominence and cavity, mimicking a cyclone. The most intense and coherent rotation lasts for over three hours, with emission in both hot ($\sim$1MK) and cold (hydrogen and helium) lines. We suggest that the cyclonic appearance and overall evolution of the structure can be interpreted in terms of the expansion of helical structures into the cavity, and the movement of plasma along helical structures which appears as a rotation when viewed along the helix axis. The coordinated movement of material between prominence and cavity suggest that they are structurally linked. Complexity is great due to the combined effect of these actions and the line-of-sight integration through the structure which contains tangled fields.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/a-solar-tornado-observed-by-aiasdo-rotational-flow-and-evolution-of-magnetic-helicity-in-a-prominence-and-cavity/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Recent Observations of Plasma and Alfvenic Wave Energy Injection at the Base of the Fast Solar Wind</title>
		<link>http://voxcharta.org/2012/05/17/recent-observations-of-plasma-and-alfvenic-wave-energy-injection-at-the-base-of-the-fast-solar-wind/</link>
		<comments>http://voxcharta.org/2012/05/17/recent-observations-of-plasma-and-alfvenic-wave-energy-injection-at-the-base-of-the-fast-solar-wind/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:50:57 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[avenues]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[coronal hole]]></category>
		<category><![CDATA[counterpart]]></category>
		<category><![CDATA[energy content]]></category>
		<category><![CDATA[energy injection]]></category>
		<category><![CDATA[high speed]]></category>
		<category><![CDATA[occurrence]]></category>
		<category><![CDATA[plasma heating]]></category>
		<category><![CDATA[premise]]></category>
		<category><![CDATA[punch]]></category>
		<category><![CDATA[radiation]]></category>
		<category><![CDATA[slow solar wind]]></category>
		<category><![CDATA[solar atmosphere]]></category>
		<category><![CDATA[spicule]]></category>
		<category><![CDATA[transverse motion]]></category>
		<category><![CDATA[wave energy]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/recent-observations-of-plasma-and-alfvenic-wave-energy-injection-at-the-base-of-the-fast-solar-wind/</guid>
		<description><![CDATA[We take stock of recent observations that identify the episodic plasma heating and injection of Alfvenic energy at the base of fast solar wind (in coronal holes). The plasma heating is associated with the occurrence of chromospheric spicules that leave the lower solar atmosphere at speeds of order 100km/s, the hotter coronal counterpart of the [...]]]></description>
			<content:encoded><![CDATA[<p>We take stock of recent observations that identify the episodic plasma heating and injection of Alfvenic energy at the base of fast solar wind (in coronal holes). The plasma heating is associated with the occurrence of chromospheric spicules that leave the lower solar atmosphere at speeds of order 100km/s, the hotter coronal counterpart of the spicule emits radiation characteristic of root heating that rapidly reaches temperatures of the order of 1MK. Furthermore, the same spicules and their coronal counterparts (&#8220;Propagating Coronal Disturbances&#8221;; PCD) exhibit large amplitude, high speed, Alfvenic (transverse) motion of sufficient energy content to accelerate the material to high speeds. We propose that these (disjointed) heating and accelerating components form a one-two punch to supply, and then accelerate, the fast solar wind. We consider some compositional constraints on this concept, extend the premise to the slow solar wind, and identify future avenues of exploration.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/recent-observations-of-plasma-and-alfvenic-wave-energy-injection-at-the-base-of-the-fast-solar-wind/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Gas Accretion is Dominated by Warm Ionized Gas in Milky Way-Mass Galaxies at z ~ 0</title>
		<link>http://voxcharta.org/2012/05/17/gas-accretion-is-dominated-by-warm-ionized-gas-in-milky-way-mass-galaxies-at-z-0/</link>
		<comments>http://voxcharta.org/2012/05/17/gas-accretion-is-dominated-by-warm-ionized-gas-in-milky-way-mass-galaxies-at-z-0/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:50:40 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[adaptive mesh refinement]]></category>
		<category><![CDATA[distance]]></category>
		<category><![CDATA[enzo]]></category>
		<category><![CDATA[filamentary structure]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[galactic halo]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gas inflow]]></category>
		<category><![CDATA[gases]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[ionized gas]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[mass galaxy]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[radius]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[vicinity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/gas-accretion-is-dominated-by-warm-ionized-gas-in-milky-way-mass-galaxies-at-z-0/</guid>
		<description><![CDATA[We perform high-resolution hydrodynamic simulations of a Milky Way-mass galaxy in a fully cosmological setting using the adaptive mesh refinement code, Enzo, and study the kinematics of gas in the simulated galactic halo. We find that the gas inflow occurs mostly along filamentary structures in the halo. The warm-hot (10^5 K &#60; T  10^6 [...]]]></description>
			<content:encoded><![CDATA[<p>We perform high-resolution hydrodynamic simulations of a Milky Way-mass galaxy in a fully cosmological setting using the adaptive mesh refinement code, Enzo, and study the kinematics of gas in the simulated galactic halo. We find that the gas inflow occurs mostly along filamentary structures in the halo. The warm-hot (10^5 K &lt; T  10^6 K) ionized gases are found to dominate the overall mass accretion in the system (with dM/dt = 3-5 M_solar/yr) over a large range of distances, extending from the virial radius to the vicinity of the disk. Most of the inflowing gas (by mass) does not cool, and the small fraction that manages to cool does so primarily close to the galaxy (R &lt;~ 20 kpc), perhaps comprising the neutral gas that may be detectable as, e.g., high-velocity clouds. The neutral clouds are embedded within larger, accreting filamentary flows, and represent only a small fraction of the total mass inflow rate. The inflowing gas has relatively low metallicity (Z/Z_solar &lt; 0.2). The outer layers of the filamentary inflows are heated due to compression as they approach the disk. In addition to the inflow, we find high-velocity, metal-enriched outflows of hot gas driven by supernova feedback. Our results are consistent with observations of halo gas at low z.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/gas-accretion-is-dominated-by-warm-ionized-gas-in-milky-way-mass-galaxies-at-z-0/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>The Infrared Light Curve of SN 2011fe in M101 and the Distance to M101</title>
		<link>http://voxcharta.org/2012/05/17/the-infrared-light-curve-of-sn-2011fe-in-m101-and-the-distance-to-m101/</link>
		<comments>http://voxcharta.org/2012/05/17/the-infrared-light-curve-of-sn-2011fe-in-m101-and-the-distance-to-m101/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:50:15 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absolute calibration]]></category>
		<category><![CDATA[b band]]></category>
		<category><![CDATA[curve data]]></category>
		<category><![CDATA[epochs]]></category>
		<category><![CDATA[fourteen days]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[infrared camera]]></category>
		<category><![CDATA[light curve]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[m101]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[maximum brightness]]></category>
		<category><![CDATA[modulus]]></category>
		<category><![CDATA[SNe]]></category>
		<category><![CDATA[templates]]></category>
		<category><![CDATA[type ia]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/the-infrared-light-curve-of-sn-2011fe-in-m101-and-the-distance-to-m101/</guid>
		<description><![CDATA[We present near infra-red light curves of supernova (SN) 2011fe in M101, including 34 epochs in H band starting fourteen days before maximum brightness in the B-band. The light curve data were obtained with the WIYN High-Resolution Infrared Camera (WHIRC). When the data are calibrated using templates of other Type Ia SNe, we derive an [...]]]></description>
			<content:encoded><![CDATA[<p>We present near infra-red light curves of supernova (SN) 2011fe in M101, including 34 epochs in H band starting fourteen days before maximum brightness in the B-band. The light curve data were obtained with the WIYN High-Resolution Infrared Camera (WHIRC). When the data are calibrated using templates of other Type Ia SNe, we derive an apparent H-band magnitude at the epoch of B-band maximum of 10.85 \pm 0.04. This implies a distance modulus for M101 that ranges from 28.86 to 29.17 mag, depending on which absolute calibration for Type Ia SNe is used.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/the-infrared-light-curve-of-sn-2011fe-in-m101-and-the-distance-to-m101/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>The nature of dust in compact Galactic planetary nebulae from Spitzer spectra</title>
		<link>http://voxcharta.org/2012/05/17/the-nature-of-dust-in-compact-galactic-planetary-nebulae-from-spitzer-spectra/</link>
		<comments>http://voxcharta.org/2012/05/17/the-nature-of-dust-in-compact-galactic-planetary-nebulae-from-spitzer-spectra/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:49:48 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[continuum]]></category>
		<category><![CDATA[dust grains]]></category>
		<category><![CDATA[enhancement]]></category>
		<category><![CDATA[equilibrium]]></category>
		<category><![CDATA[evolutionary sequence]]></category>
		<category><![CDATA[galactic center]]></category>
		<category><![CDATA[galactic disk]]></category>
		<category><![CDATA[galactic planetary nebulae]]></category>
		<category><![CDATA[group properties]]></category>
		<category><![CDATA[interstellar environments]]></category>
		<category><![CDATA[irs]]></category>
		<category><![CDATA[magellanic cloud]]></category>
		<category><![CDATA[mcd]]></category>
		<category><![CDATA[pne]]></category>
		<category><![CDATA[point symmetry]]></category>
		<category><![CDATA[radiation field]]></category>
		<category><![CDATA[solid state]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[state feature]]></category>
		<category><![CDATA[symmetric point]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/the-nature-of-dust-in-compact-galactic-planetary-nebulae-from-spitzer-spectra/</guid>
		<description><![CDATA[We present the Spitzer/IRS spectra of 157 compact Galactic PNe. These young PNe provide insight on the effects of dust in early post-AGB evolution, before much of the dust is altered or destroyed by the hardening stellar radiation field. Most of the selected targets have PN-type IRS spectra, while a few turned out to be [...]]]></description>
			<content:encoded><![CDATA[<p>We present the Spitzer/IRS spectra of 157 compact Galactic PNe. These young PNe provide insight on the effects of dust in early post-AGB evolution, before much of the dust is altered or destroyed by the hardening stellar radiation field. Most of the selected targets have PN-type IRS spectra, while a few turned out to be misclassified stars. We inspected the group properties of the PN spectra and classified them based on the different dust classes (featureless, carbon-rich dust; oxygen-rich dust; mixed-chemistry dust) and subclasses (aromatic and aliphatic; crystalline and amorphous). All PNe are characterized by dust continuum and more than 80% of the sample shows solid state features above the continuum, in contrast with the Magellanic Cloud sample where only ~40% of the entire sample displays solid state features; this is an indication of the strong link between dust properties and metallicity. The Galactic PNe that show solid state features are almost equally divided among the CRD, ORD, and MCD. We analyzed dust properties together with other PN properties and found that (i) there is an enhancement of MCD PNe toward the Galactic center; (ii) CRD PNe could be seen as defining an evolutionary sequence, contrary to the ORD and MCD PNe; (iii) C- and O-rich grains retain different equilibrium temperatures, as expected from models; (iv) ORD PNe are highly asymmetric and CRD PNe highly symmetric; point-symmetry is statistically more common in MCD. We find that the Galactic Disk sample does not include MCD PNe, and the other dust classes are differently populated from high to low metallicity environments. The MCPNe seem to attain higher dust temperatures at similar evolutionary stages, in agreement with the observational findings of smaller dust grains in low metallicity interstellar environments.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/the-nature-of-dust-in-compact-galactic-planetary-nebulae-from-spitzer-spectra/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Star Formation in the First Galaxies I: Collapse Delayed by Lyman-Werner Radiation</title>
		<link>http://voxcharta.org/2012/05/17/star-formation-in-the-first-galaxies-i-collapse-delayed-by-lyman-werner-radiation/</link>
		<comments>http://voxcharta.org/2012/05/17/star-formation-in-the-first-galaxies-i-collapse-delayed-by-lyman-werner-radiation/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:48:49 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[background intensity]]></category>
		<category><![CDATA[cold gas]]></category>
		<category><![CDATA[collapse]]></category>
		<category><![CDATA[computational grid]]></category>
		<category><![CDATA[dark matter halo]]></category>
		<category><![CDATA[fragmentation]]></category>
		<category><![CDATA[free star]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gas density]]></category>
		<category><![CDATA[james webb]]></category>
		<category><![CDATA[james webb space telescope]]></category>
		<category><![CDATA[line emission]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[lyman]]></category>
		<category><![CDATA[molecular hydrogen]]></category>
		<category><![CDATA[molecule]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[stellar cluster]]></category>
		<category><![CDATA[webb space telescope]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/star-formation-in-the-first-galaxies-i-collapse-delayed-by-lyman-werner-radiation/</guid>
		<description><![CDATA[We investigate the process of metal-free star formation in the first galaxies with a high-resolution cosmological simulation. We consider the cosmologically motivated scenario in which a strong molecule-destroying Lyman-Werner (LW) background inhibits effective cooling in low-mass haloes, delaying star formation until the collapse or more massive haloes. Only when molecular hydrogen (H2) can self-shield from [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate the process of metal-free star formation in the first galaxies with a high-resolution cosmological simulation. We consider the cosmologically motivated scenario in which a strong molecule-destroying Lyman-Werner (LW) background inhibits effective cooling in low-mass haloes, delaying star formation until the collapse or more massive haloes. Only when molecular hydrogen (H2) can self-shield from LW radiation, which requires a halo capable of cooling by atomic line emission, will star formation be possible. To follow the formation of multiple gravitationally bound objects, at high gas densities we introduce sink particles which accrete gas directly from the computational grid. We find that in a 1 Mpc^3 (comoving) box, runaway collapse first occurs in a 3&#215;10^7 M_sun dark matter halo at z~12 assuming a background intensity of J21=100. Due to a runaway increase in the H2 abundance and cooling rate, a self-shielding, supersonically turbulent core develops abruptly with ~10^4 M_sun in cold gas available for star formation. We analyze the formation of this self-shielding core, the character of turbulence, and the prospects for star formation. Due to a lack of fragmentation on scales we resolve, we argue that LW-delayed metal-free star formation in atomic cooling haloes is very similar to star formation in primordial minihaloes, although in making this conclusion we ignore internal stellar feedback. Finally, we briefly discuss the detectability of metal-free stellar clusters with the James Webb Space Telescope.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/star-formation-in-the-first-galaxies-i-collapse-delayed-by-lyman-werner-radiation/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<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>
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		<title>Detection of the 128 day radial velocity variations in the supergiant {\alpha} Persei. Rotational modulations, pulsations, or a planet?</title>
		<link>http://voxcharta.org/2012/05/17/detection-of-the-128-day-radial-velocity-variations-in-the-supergiant-alpha-persei-rotational-modulations-pulsations-or-a-planet/</link>
		<comments>http://voxcharta.org/2012/05/17/detection-of-the-128-day-radial-velocity-variations-in-the-supergiant-alpha-persei-rotational-modulations-pulsations-or-a-planet/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:48:16 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[alpha persei]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[boao]]></category>
		<category><![CDATA[boes]]></category>
		<category><![CDATA[bvs]]></category>
		<category><![CDATA[cepheid]]></category>
		<category><![CDATA[clear evidence]]></category>
		<category><![CDATA[exoplanet]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[modulation]]></category>
		<category><![CDATA[observational data]]></category>
		<category><![CDATA[optical astronomy observatory]]></category>
		<category><![CDATA[pulsation]]></category>
		<category><![CDATA[radial velocity variations]]></category>
		<category><![CDATA[resolution spectra]]></category>
		<category><![CDATA[rotation period]]></category>
		<category><![CDATA[rotational modulation]]></category>
		<category><![CDATA[supergiant]]></category>
		<category><![CDATA[surface activity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/detection-of-the-128-day-radial-velocity-variations-in-the-supergiant-alpha-persei-rotational-modulations-pulsations-or-a-planet/</guid>
		<description><![CDATA[Aims. In order to search for and study the nature of the low-amplitude and long-periodic radial velocity (RV) variations of massive stars, we have been carrying out a precise RV survey for supergiants that lie near or inside the Cepheid instability strip.   Methods. We have obtained high-resolution spectra of {\alpha} Per (F5 Ib) [...]]]></description>
			<content:encoded><![CDATA[<p>Aims. In order to search for and study the nature of the low-amplitude and long-periodic radial velocity (RV) variations of massive stars, we have been carrying out a precise RV survey for supergiants that lie near or inside the Cepheid instability strip.   Methods. We have obtained high-resolution spectra of {\alpha} Per (F5 Ib) from November 2005 to September 2011 using the fiber-fed Bohyunsan Observatory Echelle Spectrograph (BOES) at Bohyunsan Optical Astronomy Observatory (BOAO).   Results. Our measurements reveal that {\alpha} Per shows a periodic RV variation of 128 days and a semi-amplitude of 70 m/s. We find no strong correlation between RV variations and bisector velocity span (BVS), but the 128-d peak is indeed present in the BVS variations among several other significant peaks in periodogram.   Conclusions. {\alpha} Per may have an exoplanet, but the combined data spanning over 20 years seem to suggest that the 128-d RV variations have not been stable on long-term scale, which is somewhat difficult to reconcile with the exoplanet explanation. We do not exclude the pulsational nature of the 128-d variations in {\alpha} Per. Although we do not find clear evidence for surface activity or rotational modulations by spots, coupled with the fact that the expected rotation period is ~ 130 days the rotational modulation seems to be the most likely cause of the RV variations. More observational data and research are needed to clearly determine the origin of RV the variations in {\alpha} Per.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/detection-of-the-128-day-radial-velocity-variations-in-the-supergiant-alpha-persei-rotational-modulations-pulsations-or-a-planet/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Radiation reaction at 3.5 post-Newtonian order in effective field theory [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/17/radiation-reaction-at-3-5-post-newtonian-order-in-effective-field-theory-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/17/radiation-reaction-at-3-5-post-newtonian-order-in-effective-field-theory-cross-listing/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:48:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[confirmation]]></category>
		<category><![CDATA[constituent]]></category>
		<category><![CDATA[field theory]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[inspiral]]></category>
		<category><![CDATA[lagrangian]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[previous results]]></category>
		<category><![CDATA[radiation reaction]]></category>
		<category><![CDATA[theory approach]]></category>
		<category><![CDATA[variational principle]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/radiation-reaction-at-3-5-post-newtonian-order-in-effective-field-theory-cross-listing/</guid>
		<description><![CDATA[We derive the radiation reaction forces on a compact binary inspiral through 3.5 order in the post-Newtonian expansion using the effective field theory approach. We utilize a recent formulation of Hamilton&#8217;s variational principle that rigorously extends the usual Lagrangian and Hamiltonian formalisms to dissipative systems, including the inspiral of a compact binary from the emission [...]]]></description>
			<content:encoded><![CDATA[<p>We derive the radiation reaction forces on a compact binary inspiral through 3.5 order in the post-Newtonian expansion using the effective field theory approach. We utilize a recent formulation of Hamilton&#8217;s variational principle that rigorously extends the usual Lagrangian and Hamiltonian formalisms to dissipative systems, including the inspiral of a compact binary from the emission of gravitational waves. We find agreement with previous results, which thus provides a non-trivial confirmation of the extended variational principle. The results from this work nearly complete the equations of motion for the generic inspiral of a compact binary with spinning constituents through 3.5 post-Newtonian order, as derived entirely with effective field theory, with only the spin-orbit corrections to the potential at 3.5 post-Newtonian remaining.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/radiation-reaction-at-3-5-post-newtonian-order-in-effective-field-theory-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<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>Improvement of xenon purification system using a combination of a pulse tube refrigerator and a coaxial heat exchanger</title>
		<link>http://voxcharta.org/2012/05/17/improvement-of-xenon-purification-system-using-a-combination-of-a-pulse-tube-refrigerator-and-a-coaxial-heat-exchanger/</link>
		<comments>http://voxcharta.org/2012/05/17/improvement-of-xenon-purification-system-using-a-combination-of-a-pulse-tube-refrigerator-and-a-coaxial-heat-exchanger/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:47:35 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cryogenic system]]></category>
		<category><![CDATA[efficiency]]></category>
		<category><![CDATA[heat exchanger]]></category>
		<category><![CDATA[high speed]]></category>
		<category><![CDATA[large scale]]></category>
		<category><![CDATA[pulse tube refrigerator]]></category>
		<category><![CDATA[purification system]]></category>
		<category><![CDATA[storage]]></category>
		<category><![CDATA[thermal losses]]></category>
		<category><![CDATA[xenon gas]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/improvement-of-xenon-purification-system-using-a-combination-of-a-pulse-tube-refrigerator-and-a-coaxial-heat-exchanger/</guid>
		<description><![CDATA[We have developed a compact cryogenic system with a pulse tube refrigerator and a coaxial heat exchanger. This liquefaction-purification system not only saves the cooling power used to reach high gaseous recirculation rate, but also reduces the impurity level with high speed. The heat exchanger operates with an efficiency of 99%, which indicates the possibility [...]]]></description>
			<content:encoded><![CDATA[<p>We have developed a compact cryogenic system with a pulse tube refrigerator and a coaxial heat exchanger. This liquefaction-purification system not only saves the cooling power used to reach high gaseous recirculation rate, but also reduces the impurity level with high speed. The heat exchanger operates with an efficiency of 99%, which indicates the possibility for fast xenon gas recirculation in a highpressurized large-scale xenon storage with much less thermal losses.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/improvement-of-xenon-purification-system-using-a-combination-of-a-pulse-tube-refrigerator-and-a-coaxial-heat-exchanger/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>Optimization of Bandpass Calibration in Radio Spectroscopy</title>
		<link>http://voxcharta.org/2012/05/17/optimization-of-bandpass-calibration-in-radio-spectroscopy/</link>
		<comments>http://voxcharta.org/2012/05/17/optimization-of-bandpass-calibration-in-radio-spectroscopy/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:46:50 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[allan variance]]></category>
		<category><![CDATA[archival data]]></category>
		<category><![CDATA[blank sky]]></category>
		<category><![CDATA[conventional method]]></category>
		<category><![CDATA[dual beam]]></category>
		<category><![CDATA[integration time]]></category>
		<category><![CDATA[iriki]]></category>
		<category><![CDATA[otf]]></category>
		<category><![CDATA[radio spectroscopy]]></category>
		<category><![CDATA[receiving system]]></category>
		<category><![CDATA[scan pattern]]></category>
		<category><![CDATA[signal to noise ratio]]></category>
		<category><![CDATA[single beam]]></category>
		<category><![CDATA[spectral resolution]]></category>
		<category><![CDATA[system noise]]></category>
		<category><![CDATA[target source]]></category>
		<category><![CDATA[telescope time]]></category>
		<category><![CDATA[time efficiency]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/optimization-of-bandpass-calibration-in-radio-spectroscopy/</guid>
		<description><![CDATA[We have developed the Smoothed Bandpass Calibration (SBC) method and the best suitable scan pattern to optimize radio spectroscopic observations. Adequate spectral smoothing is applied to the spectrum toward OFF-source blank sky adjacent to a target source direction for the purpose of bandpass correction. Because the smoothing process reduces noise, the integration time for OFF-source [...]]]></description>
			<content:encoded><![CDATA[<p>We have developed the Smoothed Bandpass Calibration (SBC) method and the best suitable scan pattern to optimize radio spectroscopic observations. Adequate spectral smoothing is applied to the spectrum toward OFF-source blank sky adjacent to a target source direction for the purpose of bandpass correction. Because the smoothing process reduces noise, the integration time for OFF-source scans can be reduced keeping the signal-to-noise ratio. Since the smoothing is not applied to ON-source scans, the spectral resolution for line features is kept. An optimal smoothing window is determined by bandpass flatness evaluated by Spectral Allan Variance (SAV). An efficient scan pattern is designed to the OFF-source scans within the bandpass stability timescale estimated by Time-based Allan Variance (TAV). We have tested the SBC using the digital spectrometer, VESPA, on the VERA Iriki station. For the targeted noise level of 5e-4 as a ratio to the system noise, the optimal smoothing window was 32 &#8211; 60 ch in the whole bandwidth of 1024 ch, and the optimal scan pattern was designed as a sequence of 70-s ON + 10-s OFF scan pairs. The noise level with the SBC was reduced by a factor of 1.74 compared with the conventional method. The total telescope time to achieve the goal with the SBC was 400 s, which was 1/3 of 1200 s required by the conventional way. Improvement in telescope time efficiency with the SBC was calculated as 3x, 2x and 1.3x for single-beam, dual-beam, and on-the-fly (OTF) scans, respectively. The SBC works to optimize scan patterns for observations from now, and also works to improve signal-to-noise ratios of archival data if ON- and OFF-source spectra are individually recorded, though the efficiency depends on the spectral stability of the receiving system.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/optimization-of-bandpass-calibration-in-radio-spectroscopy/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Non-axisymmetric oscillations of rapidly rotating relativistic stars by conformal flatness approximation [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/17/non-axisymmetric-oscillations-of-rapidly-rotating-relativistic-stars-by-conformal-flatness-approximation-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/17/non-axisymmetric-oscillations-of-rapidly-rotating-relativistic-stars-by-conformal-flatness-approximation-cross-listing/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:46:39 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[approximation]]></category>
		<category><![CDATA[degree of freedom]]></category>
		<category><![CDATA[flatness]]></category>
		<category><![CDATA[general relativity]]></category>
		<category><![CDATA[gravitational radiation]]></category>
		<category><![CDATA[modes]]></category>
		<category><![CDATA[numerical code]]></category>
		<category><![CDATA[oscillation]]></category>
		<category><![CDATA[relativistic gravity]]></category>
		<category><![CDATA[relativistic stars]]></category>
		<category><![CDATA[rotating stars]]></category>
		<category><![CDATA[sequence]]></category>
		<category><![CDATA[similarity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/non-axisymmetric-oscillations-of-rapidly-rotating-relativistic-stars-by-conformal-flatness-approximation-cross-listing/</guid>
		<description><![CDATA[We present a new numerical code to compute non-axisymmetric eigenmodes of rapidly rotating relativistic stars by adopting spatially conformal flat approximation of general relativity. The approximation omits the radiative degree of freedom of relativistic gravity and the set of equations can be cast into the similar form as those in the corresponding Newtonian problem. The [...]]]></description>
			<content:encoded><![CDATA[<p>We present a new numerical code to compute non-axisymmetric eigenmodes of rapidly rotating relativistic stars by adopting spatially conformal flat approximation of general relativity. The approximation omits the radiative degree of freedom of relativistic gravity and the set of equations can be cast into the similar form as those in the corresponding Newtonian problem. The code developed computes eigenmodes of rapidly rotating stars by taking advantage of this similarity to Newtonian problem. The code is tested against the low order f- and p-modes of slowly rotating stars which shows a good agreement of frequencies computed by our new code and those by the full theory. Also entire sequences of the low order counter-rotating f-modes are computed, which are susceptible to an instability driven by gravitational radiation.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/non-axisymmetric-oscillations-of-rapidly-rotating-relativistic-stars-by-conformal-flatness-approximation-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Spectroscopy of extended Ly\alpha\ envelopes around z=4.5 quasars</title>
		<link>http://voxcharta.org/2012/05/17/spectroscopy-of-extended-lyalpha-envelopes-around-z4-5-quasars/</link>
		<comments>http://voxcharta.org/2012/05/17/spectroscopy-of-extended-lyalpha-envelopes-around-z4-5-quasars/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:46:26 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[diameter]]></category>
		<category><![CDATA[envelopes]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[point spread function]]></category>
		<category><![CDATA[quasar]]></category>
		<category><![CDATA[radio]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[shape]]></category>
		<category><![CDATA[slit]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[Telescope]]></category>
		<category><![CDATA[unprecedented depth]]></category>
		<category><![CDATA[ut1]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/spectroscopy-of-extended-lyalpha-envelopes-around-z4-5-quasars/</guid>
		<description><![CDATA[What are the frequency, shape, kinematics, and luminosity of Ly\alpha\ envelopes surrounding radio-quiet quasars at high redshift, and is the luminosity of these envelopes related to that of the quasar or not? As a first step towards answering these questions, we have searched for Ly\alpha\ envelopes around six radio-quiet quasars at z~4.5, using deep spectra [...]]]></description>
			<content:encoded><![CDATA[<p>What are the frequency, shape, kinematics, and luminosity of Ly\alpha\ envelopes surrounding radio-quiet quasars at high redshift, and is the luminosity of these envelopes related to that of the quasar or not? As a first step towards answering these questions, we have searched for Ly\alpha\ envelopes around six radio-quiet quasars at z~4.5, using deep spectra taken with the FORS2 spectrograph attached to the UT1 of the Very Large Telescope (VLT). Using the multi-slit mode allows us to observe several point spread function stars simultaneously with the quasar, and to remove the point-like emission from the quasar, unveiling the faint underlying Ly\alpha\ envelope with unprecedented depth. An envelope is detected around four of the six quasars, which suggests that these envelopes are very frequent. Their diameter varies in the range 26&lt;d&lt;64 kpc, their surface brightness in the range 3&#215;10^{-19}&lt;\mu&lt;2&#215;10^{-17} erg/s/cm^2/arcsec^2, and their luminosity in the range 10^{42}&lt;L(Ly\alpha)&lt;10^{44} erg/s. Their shape may be strongly asymmetric. The Ly\alpha\ emission line full width at half maximum (FWHM) is 900&lt;FWHM&lt;2200 km/s and its luminosity correlates with that of the broad line region (BLR) of the quasar, with the notable exception of BR2237-0607, the brightest object in our sample. The same holds for the relation between the envelope Ly\alpha\ luminosity and the ionizing luminosity of the quasar. While the deep slit spectroscopy presented in this paper is very efficient at detecting very faint Ly\alpha\ envelopes, narrow-band imaging is now needed to measure accurately their spatial extent, radial luminosity profile, and total luminosity. These observables are crucial to help us discriminate between the three possible radiation processes responsible for the envelope emission: (i) cold accretion, (ii) fluorescence induced by the quasar, and (iii) scattering of the BLR photons by cool gas.</p>
]]></content:encoded>
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		<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>The evolution of the X-ray emission of HH 2 &#8211; Investigating heating and cooling processes</title>
		<link>http://voxcharta.org/2012/05/17/the-evolution-of-the-x-ray-emission-of-hh-2-investigating-heating-and-cooling-processes/</link>
		<comments>http://voxcharta.org/2012/05/17/the-evolution-of-the-x-ray-emission-of-hh-2-investigating-heating-and-cooling-processes/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:45:57 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[alignment]]></category>
		<category><![CDATA[bipolar]]></category>
		<category><![CDATA[bipolar outflows]]></category>
		<category><![CDATA[chandra observation]]></category>
		<category><![CDATA[constancy]]></category>
		<category><![CDATA[heating and cooling]]></category>
		<category><![CDATA[herbig haro]]></category>
		<category><![CDATA[optical emission]]></category>
		<category><![CDATA[proper motion]]></category>
		<category><![CDATA[radiative loss]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[stellar object]]></category>
		<category><![CDATA[temperature gas]]></category>
		<category><![CDATA[thermal conduction]]></category>
		<category><![CDATA[time scale]]></category>
		<category><![CDATA[wavelength]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/the-evolution-of-the-x-ray-emission-of-hh-2-investigating-heating-and-cooling-processes/</guid>
		<description><![CDATA[Young stellar objects often drive powerful bipolar outflows which evolve on time scales of a few years. An increasing number of these outflows has been detected in X-rays implying the existence of million degree plasma almost co-spatial with the lower temperature gas observed in the optical and near-IR. The details of the heating and cooling [...]]]></description>
			<content:encoded><![CDATA[<p>Young stellar objects often drive powerful bipolar outflows which evolve on time scales of a few years. An increasing number of these outflows has been detected in X-rays implying the existence of million degree plasma almost co-spatial with the lower temperature gas observed in the optical and near-IR. The details of the heating and cooling processes of the X-ray emitting part of these so-called Herbig-Haro objects are still ambiguous, e.g., whether the cooling is dominated by expansion, radiation or thermal conduction.   We present a second epoch Chandra observation of the first X-ray detected Herbig-Haro object (HH 2) and derive the proper-motion of the X-ray emitting plasma and its cooling history. We argue that the most likely explanation for the constancy of the X-ray luminosity, the alignment with the optical emission and the proper-motion is that the cooling is dominated by radiative losses leading to cooling times exceeding a decade. We explain that a strong shock caused by fast material ramming into slower gas in front of it about ten years ago can explain the X-ray emission while being compatible with the available multi-wavelength data of HH 2.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/the-evolution-of-the-x-ray-emission-of-hh-2-investigating-heating-and-cooling-processes/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>
		</item>
		<item>
		<title>Relativistic jet models for two low-luminosity radio galaxies: evidence for backflow?</title>
		<link>http://voxcharta.org/2012/05/17/relativistic-jet-models-for-two-low-luminosity-radio-galaxies-evidence-for-backflow/</link>
		<comments>http://voxcharta.org/2012/05/17/relativistic-jet-models-for-two-low-luminosity-radio-galaxies-evidence-for-backflow/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:45:29 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[25c]]></category>
		<category><![CDATA[added component]]></category>
		<category><![CDATA[asymmetry]]></category>
		<category><![CDATA[backflow]]></category>
		<category><![CDATA[component structure]]></category>
		<category><![CDATA[jet axis]]></category>
		<category><![CDATA[jet model]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[linear polarization]]></category>
		<category><![CDATA[lobes]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[radio emission]]></category>
		<category><![CDATA[radio galaxy]]></category>
		<category><![CDATA[radio jet]]></category>
		<category><![CDATA[relativistic jet]]></category>
		<category><![CDATA[relativistic outflows]]></category>
		<category><![CDATA[spectral index]]></category>
		<category><![CDATA[ugc]]></category>
		<category><![CDATA[very large array]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/relativistic-jet-models-for-two-low-luminosity-radio-galaxies-evidence-for-backflow/</guid>
		<description><![CDATA[We show that asymmetries in total intensity and linear polarization between the radio jets and counter-jets in two lobed Fanaroff-Riley Class I (FR I) radio galaxies, B2 0206+35 (UGC 1651) and B2 0755+37 (NGC 2484), can be accounted for if these jets are intrinsically symmetrical, with decelerating relativistic outflows surrounded by mildly relativistic backflows. Our [...]]]></description>
			<content:encoded><![CDATA[<p>We show that asymmetries in total intensity and linear polarization between the radio jets and counter-jets in two lobed Fanaroff-Riley Class I (FR I) radio galaxies, B2 0206+35 (UGC 1651) and B2 0755+37 (NGC 2484), can be accounted for if these jets are intrinsically symmetrical, with decelerating relativistic outflows surrounded by mildly relativistic backflows. Our interpretation is motivated by sensitive, well-resolved Very Large Array imaging which shows that both jets in both sources have a two-component structure transverse to their axes. Close to the jet axis, a centrally-darkened counter-jet lies opposite a centrally-brightened jet, but both are surrounded by broader collimated emission that is brighter on the counter-jet side. We have adapted our previous models of FR I jets as relativistic outflows to include an added component of symmetric backflow. We find that the observed radio emission, after subtracting contributions from the extended lobes, is well described by models in which decelerating outflows with parameters similar to those derived for jets in plumed FR I sources are surrounded by backflows containing predominantly toroidal magnetic fields. These return to within a few kpc of the galaxies with velocities of roughly 0.25c and radiate with a synchrotron spectral index close to 0.55. We discuss whether such backflow is to be expected in lobed FR I sources and suggest ways in which our hypothesis can be tested by further observations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/relativistic-jet-models-for-two-low-luminosity-radio-galaxies-evidence-for-backflow/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>INTEGRAL/IBIS 9-year Galactic Hard X-Ray Survey</title>
		<link>http://voxcharta.org/2012/05/17/integralibis-9-year-galactic-hard-x-ray-survey/</link>
		<comments>http://voxcharta.org/2012/05/17/integralibis-9-year-galactic-hard-x-ray-survey/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:45:18 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[aim]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[gamma]]></category>
		<category><![CDATA[maximum exposure]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[nine years]]></category>
		<category><![CDATA[observational data]]></category>
		<category><![CDATA[observatory]]></category>
		<category><![CDATA[population study]]></category>
		<category><![CDATA[source population]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/integralibis-9-year-galactic-hard-x-ray-survey/</guid>
		<description><![CDATA[Context. The INTEGRAL observatory operating in a hard X-ray/gamma domain gathered a large observational data set over nine years since 2003. Dominant fraction of the observing time was dedicated to the Galactic source population study making the possibility of the deepest Galactic survey in hard X-rays ever compiled. Aims. The aim of the current Galactic [...]]]></description>
			<content:encoded><![CDATA[<p>Context. The INTEGRAL observatory operating in a hard X-ray/gamma domain gathered a large observational data set over nine years since 2003. Dominant fraction of the observing time was dedicated to the Galactic source population study making the possibility of the deepest Galactic survey in hard X-rays ever compiled. Aims. The aim of the current Galactic survey is to make a basis for Galactic source population studies, and perform mapping of the Milky Way in hard X-rays over the maximum exposure available at |b|&lt;17.5 deg. Methods. We used sky reconstruction algorithms specially developed for the high quality imaging of INTEGRAL/IBIS data. Results. We present sky images, sensitivity maps, and catalogs of detected sources in three energy bands: 17-60, 17-35, and 35-80 keV in the Galactic plane at |b|5 sigma has an identification completeness of ~91%, which is valuable for population studies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/integralibis-9-year-galactic-hard-x-ray-survey/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The analysis of the hydrogen broad Balmer line ratios: possible implications to the physical properties of the BLR of AGN</title>
		<link>http://voxcharta.org/2012/05/17/the-analysis-of-the-hydrogen-broad-balmer-line-ratios-possible-implications-to-the-physical-properties-of-the-blr-of-agn/</link>
		<comments>http://voxcharta.org/2012/05/17/the-analysis-of-the-hydrogen-broad-balmer-line-ratios-possible-implications-to-the-physical-properties-of-the-blr-of-agn/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:44:54 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[AGN]]></category>
		<category><![CDATA[atomic data]]></category>
		<category><![CDATA[balmer lines]]></category>
		<category><![CDATA[blr]]></category>
		<category><![CDATA[boltzmann]]></category>
		<category><![CDATA[decrement]]></category>
		<category><![CDATA[digital sky survey]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[epsilon]]></category>
		<category><![CDATA[high density plasma]]></category>
		<category><![CDATA[hydrogen]]></category>
		<category><![CDATA[line ratio]]></category>
		<category><![CDATA[recombination]]></category>
		<category><![CDATA[sloan digital]]></category>
		<category><![CDATA[spectral synthesis]]></category>
		<category><![CDATA[survey database]]></category>
		<category><![CDATA[thermodynamic parameters]]></category>
		<category><![CDATA[three ways]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/the-analysis-of-the-hydrogen-broad-balmer-line-ratios-possible-implications-to-the-physical-properties-of-the-blr-of-agn/</guid>
		<description><![CDATA[We analyze the ratios of the broad hydrogen Balmer emission lines (from H\alpha to H\epsilon) in the context of estimating the physical conditions in the broad line region (BLR) of active galactic nuclei (AGN). The Balmer emission lines are obtained in three ways: i) using photoionization models obtained by a spectral synthesis code CLOUDY; ii) [...]]]></description>
			<content:encoded><![CDATA[<p>We analyze the ratios of the broad hydrogen Balmer emission lines (from H\alpha to H\epsilon) in the context of estimating the physical conditions in the broad line region (BLR) of active galactic nuclei (AGN). The Balmer emission lines are obtained in three ways: i) using photoionization models obtained by a spectral synthesis code CLOUDY; ii) calculated using the recombination theory for hydrogenic ions; iii) measured from the sample of observed spectra taken from the Sloan Digital Sky Survey database. We investigate the Balmer line ratios in the frame of the so called Boltzmann-plot (BP), analyzing physical conditions of the emitting plasma for which we could use the BP method. The BP considers the ratio of Balmer lines normalized to the atomic data of the corresponding line transition, and is in that way different from the Balmer decrement. We found that for a certain range of thermodynamic parameters, there are objects that follow the BP. These AGN may have a BLR consisting of mostly high density plasma.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/the-analysis-of-the-hydrogen-broad-balmer-line-ratios-possible-implications-to-the-physical-properties-of-the-blr-of-agn/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A new Skyrme interaction with improved spin-isospin properties [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/17/a-new-skyrme-interaction-with-improved-spin-isospin-properties-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/17/a-new-skyrme-interaction-with-improved-spin-isospin-properties-cross-listing/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:43:50 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accurate description]]></category>
		<category><![CDATA[charge exchange]]></category>
		<category><![CDATA[core collapse]]></category>
		<category><![CDATA[decay]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[earth]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[finite nuclei]]></category>
		<category><![CDATA[improvements]]></category>
		<category><![CDATA[interaction]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[physical processes]]></category>
		<category><![CDATA[resonance]]></category>
		<category><![CDATA[saturation]]></category>
		<category><![CDATA[spin isospin]]></category>
		<category><![CDATA[stars in the universe]]></category>
		<category><![CDATA[stellar nucleosynthesis]]></category>
		<category><![CDATA[stringent test]]></category>
		<category><![CDATA[supernova explosion]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/a-new-skyrme-interaction-with-improved-spin-isospin-properties-cross-listing/</guid>
		<description><![CDATA[A correct determination of the spin-isospin properties of the nuclear effective interaction should lead, among other improvements, to an accurate description of the Gamow-Teller Resonances (GTR). These nuclear excitations impact on a variety of physical processes: from the response in charge-exchange reactions of nuclei naturally present in the Earth, to the description of the stellar [...]]]></description>
			<content:encoded><![CDATA[<p>A correct determination of the spin-isospin properties of the nuclear effective interaction should lead, among other improvements, to an accurate description of the Gamow-Teller Resonances (GTR). These nuclear excitations impact on a variety of physical processes: from the response in charge-exchange reactions of nuclei naturally present in the Earth, to the description of the stellar nucleosynthesis, and of the pre-supernova explosion core-collapse evolution of massive stars in the Universe. A reliable description of the GTR provides also stringent tests for neutrinoless double-$\beta$ decay calculations. We present a new Skyrme interaction as accurate as previous forces in the description of finite nuclei and of uniform matter properties around saturation density, and that accurately accounts for the GTR in ${}^{48}$Ca, ${}^{90}$Zr and ${}^{208}$Pb.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/a-new-skyrme-interaction-with-improved-spin-isospin-properties-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Optimization of the Collection Efficiency of a Hexagonal Light Collector using Quadratic and Cubic B\&#8217;ezier Curves</title>
		<link>http://voxcharta.org/2012/05/17/optimization-of-the-collection-efficiency-of-a-hexagonal-light-collector-using-quadratic-and-cubic-bezier-curves/</link>
		<comments>http://voxcharta.org/2012/05/17/optimization-of-the-collection-efficiency-of-a-hexagonal-light-collector-using-quadratic-and-cubic-bezier-curves/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:43:27 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[aperture]]></category>
		<category><![CDATA[cherenkov photons]]></category>
		<category><![CDATA[collection efficiency]]></category>
		<category><![CDATA[curves]]></category>
		<category><![CDATA[focal plane]]></category>
		<category><![CDATA[gamma ray telescope]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[incident angle]]></category>
		<category><![CDATA[night sky]]></category>
		<category><![CDATA[optical system]]></category>
		<category><![CDATA[optimization]]></category>
		<category><![CDATA[shape]]></category>
		<category><![CDATA[sky background]]></category>
		<category><![CDATA[telescopes]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/optimization-of-the-collection-efficiency-of-a-hexagonal-light-collector-using-quadratic-and-cubic-bezier-curves/</guid>
		<description><![CDATA[Reflective light collectors with hexagonal entrance and exit apertures are frequently used in front of the focal-plane camera of a very-high-energy gamma-ray telescope to increase the collection efficiency of atmospheric Cherenkov photons and reduce the night-sky background entering at large incident angles. The shape of a hexagonal light collector is usually based on Winston&#8217;s design, [...]]]></description>
			<content:encoded><![CDATA[<p>Reflective light collectors with hexagonal entrance and exit apertures are frequently used in front of the focal-plane camera of a very-high-energy gamma-ray telescope to increase the collection efficiency of atmospheric Cherenkov photons and reduce the night-sky background entering at large incident angles. The shape of a hexagonal light collector is usually based on Winston&#8217;s design, which is optimized for only two-dimensional optical systems. However, it is not known whether a hexagonal Winston cone is optimal for the real three-dimensional optical systems of gamma-ray telescopes. For the first time we optimize the shape of a hexagonal light collector using quadratic and cubic B\&#8217;ezier curves. We demonstrate that our optimized designs simultaneously achieve a higher collection efficiency and background reduction rate than traditional designs.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/optimization-of-the-collection-efficiency-of-a-hexagonal-light-collector-using-quadratic-and-cubic-bezier-curves/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Anisotropy of TeV and PeV cosmic rays with IceCube and IceTop</title>
		<link>http://voxcharta.org/2012/05/17/anisotropy-of-tev-and-pev-cosmic-rays-with-icecube-and-icetop/</link>
		<comments>http://voxcharta.org/2012/05/17/anisotropy-of-tev-and-pev-cosmic-rays-with-icecube-and-icetop/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:43:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[angular scale]]></category>
		<category><![CDATA[anisotropy]]></category>
		<category><![CDATA[array]]></category>
		<category><![CDATA[arrival direction]]></category>
		<category><![CDATA[atmosphere]]></category>
		<category><![CDATA[cosmic ray data]]></category>
		<category><![CDATA[cosmic ray studies]]></category>
		<category><![CDATA[earth]]></category>
		<category><![CDATA[energy range]]></category>
		<category><![CDATA[extensive air showers]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[IceCube]]></category>
		<category><![CDATA[interaction]]></category>
		<category><![CDATA[neutrino telescope]]></category>
		<category><![CDATA[observation]]></category>
		<category><![CDATA[primary cosmic rays]]></category>
		<category><![CDATA[secondary particles]]></category>
		<category><![CDATA[statistics data]]></category>
		<category><![CDATA[TeV]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/anisotropy-of-tev-and-pev-cosmic-rays-with-icecube-and-icetop/</guid>
		<description><![CDATA[The interaction of high energy cosmic rays with the Earth&#8217;s atmosphere produces extensive air showers of secondary particles with a large muon component. By exploiting the sensitivity of neutrino telescopes to high energy muons, it is possible to use these detectors for precision cosmic ray studies. The high rate of cosmic-ray muon events provides a [...]]]></description>
			<content:encoded><![CDATA[<p>The interaction of high energy cosmic rays with the Earth&#8217;s atmosphere produces extensive air showers of secondary particles with a large muon component. By exploiting the sensitivity of neutrino telescopes to high energy muons, it is possible to use these detectors for precision cosmic ray studies. The high rate of cosmic-ray muon events provides a high-statistics data sample that can be used to look for anisotropy in the arrival directions of the parent particles at the per-mille level.   This paper reports on the observation of anisotropy in the cosmic ray data collected with the IceCube neutrino telescope in the 20-400 TeV energy range at multiple angular scales. New data from the IceTop air shower array, located on the ice surface above IceCube, shows an anisotropy that is consistent with the high-energy IceCube results. The sensitivity of IceTop to all the components of the extensive air shower will allow us to explore in more detail the characteristics of the primary cosmic rays associated with the observed anisotropy.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/anisotropy-of-tev-and-pev-cosmic-rays-with-icecube-and-icetop/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>On the Validity of Cosmological Fisher Matrix Forecasts</title>
		<link>http://voxcharta.org/2012/05/17/on-the-validity-of-cosmological-fisher-matrix-forecasts/</link>
		<comments>http://voxcharta.org/2012/05/17/on-the-validity-of-cosmological-fisher-matrix-forecasts/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:42:26 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acoustic oscillations]]></category>
		<category><![CDATA[approximation]]></category>
		<category><![CDATA[cosmological probes]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[discrepancy]]></category>
		<category><![CDATA[elliptical shape]]></category>
		<category><![CDATA[energy equation]]></category>
		<category><![CDATA[energy survey]]></category>
		<category><![CDATA[energy task force]]></category>
		<category><![CDATA[equation of state]]></category>
		<category><![CDATA[figure of merit]]></category>
		<category><![CDATA[fom]]></category>
		<category><![CDATA[likelihood estimation]]></category>
		<category><![CDATA[likelihood function]]></category>
		<category><![CDATA[linear transformation]]></category>
		<category><![CDATA[markov chain]]></category>
		<category><![CDATA[posterior probability]]></category>
		<category><![CDATA[quantitative difference]]></category>
		<category><![CDATA[stage iii]]></category>
		<category><![CDATA[structure formation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/on-the-validity-of-cosmological-fisher-matrix-forecasts/</guid>
		<description><![CDATA[We present a comparison of Fisher matrix forecasts for cosmological probes with Monte Carlo Markov Chain (MCMC) posterior likelihood estimation methods. We analyse the performance of future Dark Energy Task Force (DETF) stage-III and stage-IV dark-energy surveys using supernovae, baryon acoustic oscillations and weak lensing as probes. We concentrate in particular on the dark-energy equation [...]]]></description>
			<content:encoded><![CDATA[<p>We present a comparison of Fisher matrix forecasts for cosmological probes with Monte Carlo Markov Chain (MCMC) posterior likelihood estimation methods. We analyse the performance of future Dark Energy Task Force (DETF) stage-III and stage-IV dark-energy surveys using supernovae, baryon acoustic oscillations and weak lensing as probes. We concentrate in particular on the dark-energy equation of state parameters $w_0$ and $w_a$. For forecasts with fixed $w_a=0$, there is no qualitative discrepancy between the Fisher matrix approximation and the full likelihood via MCMC exploration, although there are significant quantitative differences; when marginalising over $w_a$ however, we find considerable disagreement between the two methods, since for geometrical probes the Fisher matrix can not reproduce the highly non-elliptical shape of the likelihood function. More quantitatively, the Fisher method overestimates the DETF figure of merit (FoM) for purely geometrical probes by a factor of up to seven. Even in the cases including additional information from structure formation, such as weak lensing, where the likelihood is fairly elliptical, the posterior probability contours from the Fisher matrix estimation are too small: the resulting FoM is biased low by a factor of two. We then explore non-linear transformations resulting in physically-motivated parameters and investigate whether these parameterisations exhibit a Gaussian behaviour. We conclude that, especially for the purely geometrical probes, but also for tests of structure formation, the Fisher matrix is not the appropriate tool to produce reliable forecasts.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/on-the-validity-of-cosmological-fisher-matrix-forecasts/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A New Method for Cross Polarized Delay Calibration of Radio Interferometers</title>
		<link>http://voxcharta.org/2012/05/17/a-new-method-for-cross-polarized-delay-calibration-of-radio-interferometers/</link>
		<comments>http://voxcharta.org/2012/05/17/a-new-method-for-cross-polarized-delay-calibration-of-radio-interferometers/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:41:40 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[antenna]]></category>
		<category><![CDATA[calibration]]></category>
		<category><![CDATA[combinations]]></category>
		<category><![CDATA[data stream]]></category>
		<category><![CDATA[differential]]></category>
		<category><![CDATA[group delay]]></category>
		<category><![CDATA[incoming wave]]></category>
		<category><![CDATA[independent set]]></category>
		<category><![CDATA[parallel systems]]></category>
		<category><![CDATA[polarization state]]></category>
		<category><![CDATA[radio interferometer]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/a-new-method-for-cross-polarized-delay-calibration-of-radio-interferometers/</guid>
		<description><![CDATA[Radio interferometers can measure the full polarization state of incoming waves by cross&#8211;correlating all combinations of two orthogonal polarizations at each antenna. The independent sets of electronics used to detect the two polarization states will introduce a differential instrumental delay between the two data streams. The usual technique of separate calibration of the parallel&#8211;hand sets [...]]]></description>
			<content:encoded><![CDATA[<p>Radio interferometers can measure the full polarization state of incoming waves by cross&#8211;correlating all combinations of two orthogonal polarizations at each antenna. The independent sets of electronics used to detect the two polarization states will introduce a differential instrumental delay between the two data streams. The usual technique of separate calibration of the parallel&#8211;hand sets of visibilities still allows for an arbitrary offset in group delay and phase between the two parallel systems. In order to use the cross&#8211;polarized visibilities, this instrumental offset must be determined and removed. This paper describes one such technique and explores its application in the Obit package. The technique is successfully applied to some EVLA data using both strongly and weakly polarized calibrators.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/a-new-method-for-cross-polarized-delay-calibration-of-radio-interferometers/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Big Bang nucleosynthesis with a non-Maxwellian distribution [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/17/big-bang-nucleosynthesis-with-a-non-maxwellian-distribution-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/17/big-bang-nucleosynthesis-with-a-non-maxwellian-distribution-cross-listing/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:40:52 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abundance]]></category>
		<category><![CDATA[bang model]]></category>
		<category><![CDATA[big bang nucleosynthesis]]></category>
		<category><![CDATA[boltzmann statistics]]></category>
		<category><![CDATA[light element]]></category>
		<category><![CDATA[maxwellian distribution]]></category>
		<category><![CDATA[unity]]></category>
		<category><![CDATA[variation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/big-bang-nucleosynthesis-with-a-non-maxwellian-distribution-cross-listing/</guid>
		<description><![CDATA[The abundances of light elements based on the big bang nucleosynthesis model are calculated using the Tsallis non-extensive statistics. The impact of the variation of the non-extensive parameter q from the unity value is compared to observations and to the abundance yields from the standard big bang model. We find large differences between the reaction [...]]]></description>
			<content:encoded><![CDATA[<p>The abundances of light elements based on the big bang nucleosynthesis model are calculated using the Tsallis non-extensive statistics. The impact of the variation of the non-extensive parameter q from the unity value is compared to observations and to the abundance yields from the standard big bang model. We find large differences between the reaction rates and the abundance of light elements calculated with the extensive and the non-extensive statistics. A large deviation of the non-extensive parameter from q=1 (corresponding to Boltzmann statistics) does not seem to be compatible with observations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/big-bang-nucleosynthesis-with-a-non-maxwellian-distribution-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Angular Momentum Transport and Variability in Boundary Layers of Accretion Disks Driven by Global Acoustic Modes</title>
		<link>http://voxcharta.org/2012/05/17/angular-momentum-transport-and-variability-in-boundary-layers-of-accretion-disks-driven-by-global-acoustic-modes/</link>
		<comments>http://voxcharta.org/2012/05/17/angular-momentum-transport-and-variability-in-boundary-layers-of-accretion-disks-driven-by-global-acoustic-modes/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:40:34 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion disk]]></category>
		<category><![CDATA[acoustic mode]]></category>
		<category><![CDATA[amplifier]]></category>
		<category><![CDATA[angular momentum transport]]></category>
		<category><![CDATA[boundary layer]]></category>
		<category><![CDATA[compact object]]></category>
		<category><![CDATA[dissipation]]></category>
		<category><![CDATA[equatorial plane]]></category>
		<category><![CDATA[global mode]]></category>
		<category><![CDATA[inner edge]]></category>
		<category><![CDATA[mass transport]]></category>
		<category><![CDATA[orbital period]]></category>
		<category><![CDATA[orbital velocity]]></category>
		<category><![CDATA[pattern speed]]></category>
		<category><![CDATA[resonance]]></category>
		<category><![CDATA[rotational velocity]]></category>
		<category><![CDATA[shock]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[variability]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/angular-momentum-transport-and-variability-in-boundary-layers-of-accretion-disks-driven-by-global-acoustic-modes/</guid>
		<description><![CDATA[Disk accretion onto a weakly magnetized central object, e.g. a star, is inevitably accompanied by the formation of a boundary layer near the surface, in which matter slows down from the highly supersonic orbital velocity of the disk to the rotational velocity of the star. We perform high resolution 2D hydrodynamical simulations in the equatorial [...]]]></description>
			<content:encoded><![CDATA[<p>Disk accretion onto a weakly magnetized central object, e.g. a star, is inevitably accompanied by the formation of a boundary layer near the surface, in which matter slows down from the highly supersonic orbital velocity of the disk to the rotational velocity of the star. We perform high resolution 2D hydrodynamical simulations in the equatorial plane of an astrophysical boundary layer with the goal of exploring the dynamics of non-axisymmetric structures that form there. We generically find that the supersonic shear in the boundary layer excites non-axisymmetric quasi-stationary acoustic modes that are trapped between the surface of the star and a Lindblad resonance in the disk. These modes rotate in a prograde fashion, are stable for hundreds of orbital periods, and have a pattern speed that is less than and of order the rotational velocity at the inner edge of the disk. The origin of these intrinsically global modes is intimately related to the operation of a corotation amplifier in the system. Dissipation of acoustic modes in weak shocks provides a universal mechanism for angular momentum and mass transport even in purely hydrodynamic (i.e. non-magnetized) boundary layers. We discuss the possible implications of these trapped modes for explaining the variability seen in accreting compact objects.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/angular-momentum-transport-and-variability-in-boundary-layers-of-accretion-disks-driven-by-global-acoustic-modes/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Dark Matter Primordial Black Holes and Inflation Models</title>
		<link>http://voxcharta.org/2012/05/17/dark-matter-primordial-black-holes-and-inflation-models/</link>
		<comments>http://voxcharta.org/2012/05/17/dark-matter-primordial-black-holes-and-inflation-models/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:39:33 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[cosmological data]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[derivative]]></category>
		<category><![CDATA[field model]]></category>
		<category><![CDATA[first derivative]]></category>
		<category><![CDATA[inflation]]></category>
		<category><![CDATA[mass model]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[perturbation]]></category>
		<category><![CDATA[pivot scale]]></category>
		<category><![CDATA[power spectrum]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[scales]]></category>
		<category><![CDATA[spectral index]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/dark-matter-primordial-black-holes-and-inflation-models/</guid>
		<description><![CDATA[A broad range of single field models of inflation are analyzed in light of all relevant recent cosmological data, checking whether they can lead to the formation of long&#8211;lived Primordial Black Holes (PBHs) as candidate for dark matter. To that end we calculate the spectral index of the power spectrum of primordial perturbations as well [...]]]></description>
			<content:encoded><![CDATA[<p>A broad range of single field models of inflation are analyzed in light of all relevant recent cosmological data, checking whether they can lead to the formation of long&#8211;lived Primordial Black Holes (PBHs) as candidate for dark matter. To that end we calculate the spectral index of the power spectrum of primordial perturbations as well as its first and second derivatives. PBH formation is possible only if the spectral index $n_S(k_0)$ increases significantly at small scales. Since current data indicate that the first derivative $\alpha_S$ of the spectral index is negative at the pivot scale, PBH formation is only possible in the presence of a sizable and positive second derivative (&#8220;running of the running&#8221;) $\beta_S$. Among the three small-field and five large-field models we analyze, only the &#8220;running-mass&#8221; model allows PBH formation, for a narrow range of parameters.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/dark-matter-primordial-black-holes-and-inflation-models/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Importance of Disk Structure in Stalling Type I Migration</title>
		<link>http://voxcharta.org/2012/05/17/the-importance-of-disk-structure-in-stalling-type-i-migration/</link>
		<comments>http://voxcharta.org/2012/05/17/the-importance-of-disk-structure-in-stalling-type-i-migration/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:38:52 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion disk]]></category>
		<category><![CDATA[density gradient]]></category>
		<category><![CDATA[disk model]]></category>
		<category><![CDATA[disk structure]]></category>
		<category><![CDATA[dispersion]]></category>
		<category><![CDATA[earth mass]]></category>
		<category><![CDATA[gas giant]]></category>
		<category><![CDATA[mass range]]></category>
		<category><![CDATA[migration rate]]></category>
		<category><![CDATA[numerical simulation]]></category>
		<category><![CDATA[period orbits]]></category>
		<category><![CDATA[perturbation]]></category>
		<category><![CDATA[photon]]></category>
		<category><![CDATA[stellar irradiation]]></category>
		<category><![CDATA[structure parameters]]></category>
		<category><![CDATA[super earth]]></category>
		<category><![CDATA[surface density]]></category>
		<category><![CDATA[temperature profile]]></category>
		<category><![CDATA[torque]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/the-importance-of-disk-structure-in-stalling-type-i-migration/</guid>
		<description><![CDATA[As planets form they tidally interact with their natal disks. Though the tidal perturbation induced by Earth and super-Earth mass planets is generally too weak to significantly modify the structure of the disk, the interaction is potentially strong enough to cause the planets to undergo rapid type I migration. This physical process may provide a [...]]]></description>
			<content:encoded><![CDATA[<p>As planets form they tidally interact with their natal disks. Though the tidal perturbation induced by Earth and super-Earth mass planets is generally too weak to significantly modify the structure of the disk, the interaction is potentially strong enough to cause the planets to undergo rapid type I migration. This physical process may provide a source of short-period super-Earths, though it may also pose a challenge to the emergence and retention of cores on long-period orbits with sufficient mass to evolve into gas giants. Previous numerical simulations have shown that the type I migration rate sensitively depends upon the circumstellar disk&#8217;s properties, particularly the temperature and surface density gradients. Here, we derive these structure parameters for 1) a self-consistent viscous-disk model based on a constant \alpha-prescription, 2) an irradiated disk model that takes into account heating due to the absorption of stellar photons, and 3) a layered-accretion disk model with variable \alpha-parameter. We show that in the inner viscously-heated regions of typical protostellar disks, the horseshoe and corotation torques of super-Earths can exceed their differential Lindblad torque and cause them to undergo outward migration. However, the temperature profile due to passive stellar irradiation causes type I migration to be inwards throughout much of the disk. For disks in which there is outwards migration, we show that location and the mass range of the &#8220;planet traps&#8221; depends on some uncertain assumptions adopted for these disk models. Competing physical effects may lead to dispersion in super-Earths&#8217; mass-period distribution.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/the-importance-of-disk-structure-in-stalling-type-i-migration/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<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>
		</item>
		<item>
		<title>X-ray Emission from Transient Jet Model in Black Hole Binaries [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/x-ray-emission-from-transient-jet-model-in-black-hole-binaries-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/x-ray-emission-from-transient-jet-model-in-black-hole-binaries-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:37:51 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[compton]]></category>
		<category><![CDATA[electron]]></category>
		<category><![CDATA[hole binaries]]></category>
		<category><![CDATA[inflow and outflow]]></category>
		<category><![CDATA[infrared emission]]></category>
		<category><![CDATA[inner radius]]></category>
		<category><![CDATA[jet model]]></category>
		<category><![CDATA[keV]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[new model]]></category>
		<category><![CDATA[outburst]]></category>
		<category><![CDATA[possible connection]]></category>
		<category><![CDATA[radii]]></category>
		<category><![CDATA[ray binaries]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[synchrotron]]></category>
		<category><![CDATA[transient nature]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xte j1118]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/x-ray-emission-from-transient-jet-model-in-black-hole-binaries-replacement/</guid>
		<description><![CDATA[While the non-thermal radio through at least near-infrared emission in the hard state in X-ray binaries (XRBs) is known to originate in jets, the source of the non-thermal X-ray component is still uncertain. We introduce a new model for this emission, which takes into account the transient nature of outflows, and show that it can [...]]]></description>
			<content:encoded><![CDATA[<p>While the non-thermal radio through at least near-infrared emission in the hard state in X-ray binaries (XRBs) is known to originate in jets, the source of the non-thermal X-ray component is still uncertain. We introduce a new model for this emission, which takes into account the transient nature of outflows, and show that it can explain the observed properties of the X-ray spectrum. Rapid radiative cooling of the electrons naturally accounts for the break often seen below around 10 keV, and for the canonical spectral slope F_\nu ~ \nu^{-1/2} observed below the break. We derive the constraints set by the data for both synchrotron- and Compton-dominated models. We show that for the synchrotron-dominated case, the jet should be launched at radii comparable to the inner radius of the disk (~few 100 r_s for the 2000 outburst of XTE J1118+480), with typical magnetic field B &gt;~ 10^{6} G. We discuss the consequences of our results on the possible connection between the inflow and outflow in the hard state of XRBs.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/x-ray-emission-from-transient-jet-model-in-black-hole-binaries-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Flux and Photon Spectral Index Distributions of Fermi-LAT Blazars And Contribution To The Extragalactic Gamma-ray Background [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/flux-and-photon-spectral-index-distributions-of-fermi-lat-blazars-and-contribution-to-the-extragalactic-gamma-ray-background-replacement-3/</link>
		<comments>http://voxcharta.org/2012/05/17/flux-and-photon-spectral-index-distributions-of-fermi-lat-blazars-and-contribution-to-the-extragalactic-gamma-ray-background-replacement-3/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:37:36 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[background radiation]]></category>
		<category><![CDATA[best fit]]></category>
		<category><![CDATA[bia]]></category>
		<category><![CDATA[bl lac]]></category>
		<category><![CDATA[blazar]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[detection threshold]]></category>
		<category><![CDATA[distributions]]></category>
		<category><![CDATA[galactic latitude]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[parametric methods]]></category>
		<category><![CDATA[petrosian]]></category>
		<category><![CDATA[photon index]]></category>
		<category><![CDATA[ray space]]></category>
		<category><![CDATA[robustness]]></category>
		<category><![CDATA[sigma]]></category>
		<category><![CDATA[space telescope]]></category>
		<category><![CDATA[spectral index]]></category>
		<category><![CDATA[true distribution]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/flux-and-photon-spectral-index-distributions-of-fermi-lat-blazars-and-contribution-to-the-extragalactic-gamma-ray-background-replacement-3/</guid>
		<description><![CDATA[We present a determination of the distributions of photon spectral index and gamma-ray flux &#8211; the so called LogN-LogS relation &#8211; for the 352 blazars detected with a greater than approximately seven sigma detection threshold and located above +/- 20 degrees Galactic latitude by the Large Area Telescope of the Fermi Gamma-ray Space Telescope in [...]]]></description>
			<content:encoded><![CDATA[<p>We present a determination of the distributions of photon spectral index and gamma-ray flux &#8211; the so called LogN-LogS relation &#8211; for the 352 blazars detected with a greater than approximately seven sigma detection threshold and located above +/- 20 degrees Galactic latitude by the Large Area Telescope of the Fermi Gamma-ray Space Telescope in its first year catalog. Because the flux detection threshold depends on the photon index, the observed raw distributions do not provide the true LogN-LogS counts or the true distribution of the photon index. We use the non-parametric methods developed by Efron and Petrosian to reconstruct the intrinsic distributions from the observed ones which account for the data truncations introduced by observational bias and includes the effects of the possible correlation between the two variables. We demonstrate the robustness of our procedures using a simulated data set of blazars and then apply these to the real data and find that for the population as a whole the intrinsic flux distribution can be represented by a broken power law with high and low indexes of -2.37 +/- 0.13 and -1.70 +/- 0.26, respectively, and the intrinsic photon index distribution can be represented by a Gaussian with mean of 2.41 +/- 0.13 and width of 0.25 +/- 0.03. We also find the intrinsic distributions for the sub-populations of BL Lac and FSRQs type blazars separately. We then calculate the contribution of Fermi blazars to the diffuse extragalactic gamma-ray background radiation. Under the assumption that the flux distribution of blazars continues to arbitrarily low fluxes, we calculate the best fit contribution of all blazars to the total extragalactic gamma-ray output to be 60%, with a large uncertainty.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/flux-and-photon-spectral-index-distributions-of-fermi-lat-blazars-and-contribution-to-the-extragalactic-gamma-ray-background-replacement-3/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Cosmological Sakharov Oscillations and Quantum Mechanics of the Early Universe [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/cosmological-sakharov-oscillations-and-quantum-mechanics-of-the-early-universe-replacement-2/</link>
		<comments>http://voxcharta.org/2012/05/17/cosmological-sakharov-oscillations-and-quantum-mechanics-of-the-early-universe-replacement-2/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:37:23 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[academy of science]]></category>
		<category><![CDATA[brief summary]]></category>
		<category><![CDATA[early universe]]></category>
		<category><![CDATA[gravitational field]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[oscillation]]></category>
		<category><![CDATA[perturbation]]></category>
		<category><![CDATA[phenomena]]></category>
		<category><![CDATA[physical sciences division]]></category>
		<category><![CDATA[power spectrum]]></category>
		<category><![CDATA[quantum mechanics]]></category>
		<category><![CDATA[russian academy of science]]></category>
		<category><![CDATA[sciences moscow]]></category>
		<category><![CDATA[special session]]></category>
		<category><![CDATA[standing wave]]></category>
		<category><![CDATA[th anniversary]]></category>
		<category><![CDATA[wave pattern]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/cosmological-sakharov-oscillations-and-quantum-mechanics-of-the-early-universe-replacement-2/</guid>
		<description><![CDATA[This is a brief summary of a talk delivered at the Special Session of the Physical Sciences Division of the Russian Academy of Sciences, Moscow, 25 May 2011. The meeting was devoted to the 90-th anniversary of A. D. Sakharov. The focus of this contribution is on the standing-wave pattern of quantum-mechanically generated metric (gravitational [...]]]></description>
			<content:encoded><![CDATA[<p>This is a brief summary of a talk delivered at the Special Session of the Physical Sciences Division of the Russian Academy of Sciences, Moscow, 25 May 2011. The meeting was devoted to the 90-th anniversary of A. D. Sakharov. The focus of this contribution is on the standing-wave pattern of quantum-mechanically generated metric (gravitational field) perturbations as the origin of subsequent Sakharov oscillations in the matter power spectrum. Other related phenomena, particularly in the area of gravitational waves, and their observational significance are also discussed.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/cosmological-sakharov-oscillations-and-quantum-mechanics-of-the-early-universe-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Panchromatic Observations of SN 2011dh Point to a Compact Progenitor Star [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/panchromatic-observations-of-sn-2011dh-point-to-a-compact-progenitor-star-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/panchromatic-observations-of-sn-2011dh-point-to-a-compact-progenitor-star-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:37:05 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[circumstellar environment]]></category>
		<category><![CDATA[current instruments]]></category>
		<category><![CDATA[density profile]]></category>
		<category><![CDATA[emission radio]]></category>
		<category><![CDATA[equipartition]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[hst observation]]></category>
		<category><![CDATA[inverse compton]]></category>
		<category><![CDATA[mass loss]]></category>
		<category><![CDATA[optical emission]]></category>
		<category><![CDATA[optical photometry]]></category>
		<category><![CDATA[optical photons]]></category>
		<category><![CDATA[progenitor star]]></category>
		<category><![CDATA[radio data]]></category>
		<category><![CDATA[ray observations]]></category>
		<category><![CDATA[spatial coverage]]></category>
		<category><![CDATA[stellar density]]></category>
		<category><![CDATA[synchrotron emission]]></category>
		<category><![CDATA[type iib]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/panchromatic-observations-of-sn-2011dh-point-to-a-compact-progenitor-star-replacement/</guid>
		<description><![CDATA[We report the discovery and detailed monitoring of X-ray emission associated with the Type IIb SN 2011dh using data from the Swift and Chandra satellites, placing it among the best studied X-ray supernovae to date. We further present millimeter and radio data obtained with the SMA, CARMA, and EVLA during the first three weeks after [...]]]></description>
			<content:encoded><![CDATA[<p>We report the discovery and detailed monitoring of X-ray emission associated with the Type IIb SN 2011dh using data from the Swift and Chandra satellites, placing it among the best studied X-ray supernovae to date. We further present millimeter and radio data obtained with the SMA, CARMA, and EVLA during the first three weeks after explosion. Combining these observations with early optical photometry, we show that the panchromatic dataset is well-described by non-thermal synchrotron emission (radio/mm) with inverse Compton scattering (X-ray) of a thermal population of optical photons. In this scenario, the shock partition fractions deviate from equipartition by a factor, (e_e/e_B) ~ 30. We derive the properties of the shockwave and the circumstellar environment and find a shock velocity, v~0.1c, and a progenitor mass loss rate of ~6e-5 M_sun/yr. These properties are consistent with the sub-class of Type IIb SNe characterized by compact progenitors (Type cIIb) and dissimilar from those with extended progenitors (Type eIIb). Furthermore, we consider the early optical emission in the context of a cooling envelope model to estimate a progenitor radius of ~1e+11 cm, in line with the expectations for a Type cIIb SN. Together, these diagnostics are difficult to reconcile with the extended radius of the putative yellow supergiant progenitor star identified in archival HST observations, unless the stellar density profile is unusual. Finally, we searched for the high energy shock breakout pulse using X-ray and gamma-ray observations obtained during the purported explosion date range. Based on the compact radius of the progenitor, we estimate that the breakout pulse was detectable with current instruments but likely missed due to their limited temporal/spatial coverage. [Abridged]</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/panchromatic-observations-of-sn-2011dh-point-to-a-compact-progenitor-star-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Galaxy Zoo: dust and molecular gas in early-type galaxies with prominent dust lanes [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/galaxy-zoo-dust-and-molecular-gas-in-early-type-galaxies-with-prominent-dust-lanes-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/galaxy-zoo-dust-and-molecular-gas-in-early-type-galaxies-with-prominent-dust-lanes-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:36:55 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[density environments]]></category>
		<category><![CDATA[dust lane]]></category>
		<category><![CDATA[etg]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[merger]]></category>
		<category><![CDATA[population]]></category>
		<category><![CDATA[type galaxy]]></category>
		<category><![CDATA[zoo]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/galaxy-zoo-dust-and-molecular-gas-in-early-type-galaxies-with-prominent-dust-lanes-replacement/</guid>
		<description><![CDATA[We study dust and associated molecular gas in 352 nearby early-type galaxies (ETGs) with prominent dust lanes. 65% of these `dusty ETGs&#8217; (D-ETGs) are morphologically disturbed, suggesting a merger origin. This is consistent with the D-ETGs residing in lower density environments compared to the controls drawn from the general ETG population. 80% of D-ETGs inhabit [...]]]></description>
			<content:encoded><![CDATA[<p>We study dust and associated molecular gas in 352 nearby early-type galaxies (ETGs) with prominent dust lanes. 65% of these `dusty ETGs&#8217; (D-ETGs) are morphologically disturbed, suggesting a merger origin. This is consistent with the D-ETGs residing in lower density environments compared to the controls drawn from the general ETG population. 80% of D-ETGs inhabit the field (compared to 60% of the controls) and &lt;2% inhabit clusters (compared to 10% of the controls). Compared to the controls, D-ETGs exhibit bluer UV-optical colours (indicating enhanced star formation) and an AGN fraction that is more than an order of magnitude greater (indicating higher incidence of nuclear activity). The clumpy dust mass residing in large-scale features is estimated, using the SDSS r-band images, to be 10^{4.5}-10^{6.5} MSun. A comparison to the total (clumpy + diffuse) dust masses- calculated using the far-IR fluxes of 15% of the D-ETGs that are detected by the IRAS- indicates that only ~20% of the dust resides in these large-scale features. The dust masses are several times larger than the maximum value expected from stellar mass loss, ruling out an internal origin. The dust content shows no correlation with the blue luminosity, indicating that it is not related to a galactic scale cooling flow. No correlation is found with the age of the recent starburst, suggesting that the dust is accreted directly in the merger rather than being produced in situ by the triggered star formation. Using molecular gas-to-dust ratios of ETGs in the literature we estimate that the median current and initial molecular gas fraction are ~1.3% and ~4%, respectively. Recent work suggests that the merger activity in nearby ETGs largely involves minor mergers (mass ratios between 1:10 and 1:4). If the IRAS-detected D-ETGs form via this channel, then the original gas fractions of the accreted satellites are 20%-44%. [Abridged]</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/galaxy-zoo-dust-and-molecular-gas-in-early-type-galaxies-with-prominent-dust-lanes-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<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>
		</item>
		<item>
		<title>The relation between broad lines and gamma&#8211;ray luminosities in Fermi blazars [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/the-relation-between-broad-lines-and-gamma-ray-luminosities-in-fermi-blazars-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/the-relation-between-broad-lines-and-gamma-ray-luminosities-in-fermi-blazars-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:36:07 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absolute value]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[bl lac]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[blazar]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[digital sky survey]]></category>
		<category><![CDATA[eddington]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[energy emission]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[hole mass]]></category>
		<category><![CDATA[jet power]]></category>
		<category><![CDATA[mev]]></category>
		<category><![CDATA[proxy]]></category>
		<category><![CDATA[sdss]]></category>
		<category><![CDATA[sloan digital]]></category>
		<category><![CDATA[spectrum radio]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/the-relation-between-broad-lines-and-gamma-ray-luminosities-in-fermi-blazars-replacement/</guid>
		<description><![CDATA[We study the relation between the mass accretion rate, the jet power, and the black hole mass of blazars. To this aim, we make use of the Sloan Digital Sky Survey (SDSS) and the 11 months catalog of blazars detected at energies larger than 100 MeV by the Large Area Telescope (LAT) onboard the Fermi [...]]]></description>
			<content:encoded><![CDATA[<p>We study the relation between the mass accretion rate, the jet power, and the black hole mass of blazars. To this aim, we make use of the Sloan Digital Sky Survey (SDSS) and the 11 months catalog of blazars detected at energies larger than 100 MeV by the Large Area Telescope (LAT) onboard the Fermi satellite. This allows to construct a relatively large sample of blazars with information about the luminosity (or upper limits) of their emission lines used as a proxy for the strength of the disc luminosity and on the luminosity of the high energy emission, used as a proxy for the jet power. We find a good correlation between the luminosity of the broad lines and the gamma-ray luminosity as detected by Fermi, both using absolute values of the luminosities and normalising them to the Eddington value. The data we have analyzed confirm that the division of blazars into BL Lacs and Flat Spectrum Radio Quasars (FSRQs) is controlled by the line luminosity in Eddington units. For small values of this ratio the object is a BL Lac, while it is a FSRQs for large values. The transition appears smooth, but a much larger number of objects is needed to confirm this point.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/the-relation-between-broad-lines-and-gamma-ray-luminosities-in-fermi-blazars-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Direct MD simulation of liquid-solid phase equilibria for two-component plasmas [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/direct-md-simulation-of-liquid-solid-phase-equilibria-for-two-component-plasmas-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/direct-md-simulation-of-liquid-solid-phase-equilibria-for-two-component-plasmas-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:35:55 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bond angle]]></category>
		<category><![CDATA[carbon ions]]></category>
		<category><![CDATA[component model]]></category>
		<category><![CDATA[constants]]></category>
		<category><![CDATA[cumming]]></category>
		<category><![CDATA[electron screening]]></category>
		<category><![CDATA[equilibrium]]></category>
		<category><![CDATA[finite size effects]]></category>
		<category><![CDATA[liquid phase]]></category>
		<category><![CDATA[md simulation]]></category>
		<category><![CDATA[medin]]></category>
		<category><![CDATA[melting temperature]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[oxygen ions]]></category>
		<category><![CDATA[oxygen system]]></category>
		<category><![CDATA[phase diagram]]></category>
		<category><![CDATA[phase equilibrium]]></category>
		<category><![CDATA[rapid proton]]></category>
		<category><![CDATA[screening effects]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/direct-md-simulation-of-liquid-solid-phase-equilibria-for-two-component-plasmas-replacement/</guid>
		<description><![CDATA[We determine the liquid-solid phase diagram for carbon-oxygen and oxygen-selenium plasma mixtures using two-phase MD simulations. We identified liquid, solid, and interface regions using a bond angle metric. To study finite size effects, we perform 27648 and 55296 ion simulations. To help monitor non-equilibrium effects, we calculate diffusion constants $D_i$. For the carbon-oxygen system we [...]]]></description>
			<content:encoded><![CDATA[<p>We determine the liquid-solid phase diagram for carbon-oxygen and oxygen-selenium plasma mixtures using two-phase MD simulations. We identified liquid, solid, and interface regions using a bond angle metric. To study finite size effects, we perform 27648 and 55296 ion simulations. To help monitor non-equilibrium effects, we calculate diffusion constants $D_i$. For the carbon-oxygen system we find that $D_O$ for oxygen ions in the solid is much smaller than $D_C$ for carbon ions and that both diffusion constants are 80 or more times smaller than diffusion constants in the liquid phase. There is excellent agreement between our carbon-oxygen phase diagram and that predicted by Medin and Cumming. This suggests that errors from finite size and non-equilibrium effects are small and that the carbon-oxygen phase diagram is now accurately known. The oxygen-selenium system is a simple two-component model for more complex rapid proton capture nucleosynthesis ash compositions for an accreting neutron star. Diffusion of oxygen, in a predominately selenium crystal, is remarkably fast, comparable to diffusion in the liquid phase. We find a somewhat lower melting temperature for the oxygen-selenium system than that predicted by Medin and Cumming. This is probably because of electron screening effects.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/direct-md-simulation-of-liquid-solid-phase-equilibria-for-two-component-plasmas-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>Minimum Energy Configurations in the $N$-Body Problem and the Celestial Mechanics of Granular Systems [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/minimum-energy-configurations-in-the-n-body-problem-and-the-celestial-mechanics-of-granular-systems-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/minimum-energy-configurations-in-the-n-body-problem-and-the-celestial-mechanics-of-granular-systems-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:35:19 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[celestial mechanics]]></category>
		<category><![CDATA[density distribution]]></category>
		<category><![CDATA[finite density]]></category>
		<category><![CDATA[granular systems]]></category>
		<category><![CDATA[hypothesis]]></category>
		<category><![CDATA[minimum energy]]></category>
		<category><![CDATA[relative equilibria]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/minimum-energy-configurations-in-the-n-body-problem-and-the-celestial-mechanics-of-granular-systems-replacement/</guid>
		<description><![CDATA[Minimum energy configurations in celestial mechanics are investigated. It is shown that this is not a well defined problem for point-mass celestial mechanics but well-posed for finite density distributions. This naturally leads to a granular mechanics extension of usual celestial mechanics questions such as relative equilibria and stability. This paper specifically studies and finds all [...]]]></description>
			<content:encoded><![CDATA[<p>Minimum energy configurations in celestial mechanics are investigated. It is shown that this is not a well defined problem for point-mass celestial mechanics but well-posed for finite density distributions. This naturally leads to a granular mechanics extension of usual celestial mechanics questions such as relative equilibria and stability. This paper specifically studies and finds all relative equilibria and minimum energy configurations for $N=1,2,3$ and develops hypotheses on the relative equilibria and minimum energy configurations for $N\gg 1$ bodies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/minimum-energy-configurations-in-the-n-body-problem-and-the-celestial-mechanics-of-granular-systems-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The inner wind of IRC+10216 revisited: New exotic chemistry and diagnostic for dust condensation in carbon stars [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/the-inner-wind-of-irc10216-revisited-new-exotic-chemistry-and-diagnostic-for-dust-condensation-in-carbon-stars-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/the-inner-wind-of-irc10216-revisited-new-exotic-chemistry-and-diagnostic-for-dust-condensation-in-carbon-stars-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:35:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abundant species]]></category>
		<category><![CDATA[aromatics]]></category>
		<category><![CDATA[carbon dust]]></category>
		<category><![CDATA[carbon star]]></category>
		<category><![CDATA[chemical families]]></category>
		<category><![CDATA[dust formation]]></category>
		<category><![CDATA[formation region]]></category>
		<category><![CDATA[gas layers]]></category>
		<category><![CDATA[halogen]]></category>
		<category><![CDATA[herschel]]></category>
		<category><![CDATA[hydride]]></category>
		<category><![CDATA[inner wind]]></category>
		<category><![CDATA[mass ratio]]></category>
		<category><![CDATA[observational data]]></category>
		<category><![CDATA[polycyclic aromatic hydrocarbon]]></category>
		<category><![CDATA[pulsation period]]></category>
		<category><![CDATA[silicon carbide]]></category>
		<category><![CDATA[stellar pulsation]]></category>
		<category><![CDATA[supergiant star]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/the-inner-wind-of-irc10216-revisited-new-exotic-chemistry-and-diagnostic-for-dust-condensation-in-carbon-stars-replacement/</guid>
		<description><![CDATA[Aims. We model the chemistry of the inner wind of the carbon star IRC+10216 and consider the effect of periodic shocks induced by the stellar pulsation on the gas to follow the non-equilibrium chemistry in the shocked gas layers. We consider a very complete set of chemical families, including hydrocarbons and aromatics, hydrides, halogens and [...]]]></description>
			<content:encoded><![CDATA[<p>Aims. We model the chemistry of the inner wind of the carbon star IRC+10216 and consider the effect of periodic shocks induced by the stellar pulsation on the gas to follow the non-equilibrium chemistry in the shocked gas layers. We consider a very complete set of chemical families, including hydrocarbons and aromatics, hydrides, halogens and phosphorous-bearing species. Derived abundances are compared to the latest observational data from large surveys and Herschel. Results. The shocks induce a non-equilibrium chemistry in the dust formation zone of IRC+10216 where the collision destruction of CO in the post-shock gas triggers the formation of O-bearing species (H2O, SiO). Most of the modelled abundances agree very well with the latest values derived from Herschel data on IRC+10216. Hydrides form a family of abundant species that are expelled into the intermediate envelope. In particular, HF traps all the atomic fluorine in the dust formation zone. Halogens are also abundant and their chemistry is independent of the C/O ratio of the star. Therefore, HCl and other Cl-bearing species should also be present in the inner wind of O-rich AGB or supergiant stars. We identify a specific region ranging from 2.5 R* to 4 R*, where polycyclic aromatic hydrocarbons form and grow. The estimated carbon dust-to-gas mass ratio derived from the mass of aromatics ranges from 1.2 x 10^(-3) to 5.8 x 10^{-3} and agrees well with existing observational values. The aromatic formation region is located outside hot layers where SiC2 is produced as a bi-product of silicon carbide dust synthesis. Finally, we predict that some molecular lines will show flux variation with pulsation phase and time (e.g., H2O) while other species will not (e.g., CO). These variations merely reflect the non-equilibrium chemistry that destroys and reforms molecules over a pulsation period in the shocked gas of the dust formation zone.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/the-inner-wind-of-irc10216-revisited-new-exotic-chemistry-and-diagnostic-for-dust-condensation-in-carbon-stars-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Multiphase, non-spherical gas accretion onto a black hole [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/multiphase-non-spherical-gas-accretion-onto-a-black-hole-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/multiphase-non-spherical-gas-accretion-onto-a-black-hole-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:34:46 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[3d simulation]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[astrophysical implications]]></category>
		<category><![CDATA[central mass]]></category>
		<category><![CDATA[dense clump]]></category>
		<category><![CDATA[density region]]></category>
		<category><![CDATA[filament]]></category>
		<category><![CDATA[filamentary structure]]></category>
		<category><![CDATA[formation of clouds]]></category>
		<category><![CDATA[formation of stars]]></category>
		<category><![CDATA[inflow rate]]></category>
		<category><![CDATA[line regions]]></category>
		<category><![CDATA[low density]]></category>
		<category><![CDATA[radii]]></category>
		<category><![CDATA[spatial location]]></category>
		<category><![CDATA[supermassive black hole]]></category>
		<category><![CDATA[thermal instability]]></category>
		<category><![CDATA[x limit]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/multiphase-non-spherical-gas-accretion-onto-a-black-hole-replacement/</guid>
		<description><![CDATA[(Abridged) We investigate non-spherical behavior of gas accreting onto a central supermassive black hole performing simulations using the SPH code GADGET-3 including radiative cooling and heating by the central X-ray source. As found in earlier 1D studies, our 3D simulations show that the accretion mode depends on the X-ray luminosity (L_X) for a fixed density [...]]]></description>
			<content:encoded><![CDATA[<p>(Abridged) We investigate non-spherical behavior of gas accreting onto a central supermassive black hole performing simulations using the SPH code GADGET-3 including radiative cooling and heating by the central X-ray source. As found in earlier 1D studies, our 3D simulations show that the accretion mode depends on the X-ray luminosity (L_X) for a fixed density at infinity and accretion efficiency. In the low L_X limit, gas accretes in a stable, spherically symmetric fashion. In the high L_X limit, the inner gas is significantly heated up and expands, reducing the central mass inflow rate. The expanding gas can turn into a strong enough outflow capable of expelling most of the gas at larger radii. For some intermediate L_X, the accretion flow becomes unstable developing prominent non-spherical features, the key reason for which is thermal instability (TI) as shown by our analyses. Small perturbations of the initially spherically symmetric accretion flow that is heated by the intermediate L_X quickly grow to form cold and dense clumps surrounded by overheated low density regions. The cold clumps continue their inward motion forming filamentary structures; while the hot infalling gas slows down because of buoyancy and can even start outflowing through the channels in between the filaments. We found that the ratio between the mass inflow rates of the cold and hot gas is a dynamical quantity depending on several factors: time, spatial location, and L_X; and ranges between 0 and 4. We briefly discuss astrophysical implications of such TI-driven fragmentation of accreting gas on the formation of clouds in narrow and broad line regions of AGN, the formation of stars, and the observed variability of the AGN luminiosity.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/multiphase-non-spherical-gas-accretion-onto-a-black-hole-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Light Dark Matter, Light Higgs and the Electroweak Phase Transition [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/light-dark-matter-light-higgs-and-the-electroweak-phase-transition-replacement-2/</link>
		<comments>http://voxcharta.org/2012/05/17/light-dark-matter-light-higgs-and-the-electroweak-phase-transition-replacement-2/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:34:26 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cogent]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[electroweak phase transition]]></category>
		<category><![CDATA[factories]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[lep]]></category>
		<category><![CDATA[light higgs]]></category>
		<category><![CDATA[minimal extension]]></category>
		<category><![CDATA[precision test]]></category>
		<category><![CDATA[scattering cross section]]></category>
		<category><![CDATA[standard model]]></category>
		<category><![CDATA[xenon]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/light-dark-matter-light-higgs-and-the-electroweak-phase-transition-replacement-2/</guid>
		<description><![CDATA[We propose a minimal extension of the Standard Model by two real singlet fields that could provide a good candidate for light Dark Matter, and give a strong first order electroweak phase transition. As a result, there are two CP even scalars; one is lighter than \sim 70 GeV, and the other one with mass [...]]]></description>
			<content:encoded><![CDATA[<p>We propose a minimal extension of the Standard Model by two real singlet fields that could provide a good candidate for light Dark Matter, and give a strong first order electroweak phase transition. As a result, there are two CP even scalars; one is lighter than \sim 70 GeV, and the other one with mass in the range of 280-400 GeV; and consistent with electroweak precision tests. We show that the light scalar mass can be as small as 25 GeV while still being consistent with the LEP data. The predicted dark matter scattering cross section is large enough to accommodate CoGeNT and can be probed by future XENON experiment. We also show that for dark matter mass around 2 GeV, the branching fraction of the process (B^+\rightarrowK^++2(DM)) can be accessible in SuperB factories.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/light-dark-matter-light-higgs-and-the-electroweak-phase-transition-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Approximate Bayesian Computation for Astronomical Model Analysis: A Case Study in Galaxy Demographics and Morphological Transformation at High Redshift [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/approximate-bayesian-computation-for-astronomical-model-analysis-a-case-study-in-galaxy-demographics-and-morphological-transformation-at-high-redshift-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/approximate-bayesian-computation-for-astronomical-model-analysis-a-case-study-in-galaxy-demographics-and-morphological-transformation-at-high-redshift-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:34:08 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abc analysis]]></category>
		<category><![CDATA[bayesian computation]]></category>
		<category><![CDATA[complex stochastic systems]]></category>
		<category><![CDATA[early universe]]></category>
		<category><![CDATA[input parameter]]></category>
		<category><![CDATA[latter condition]]></category>
		<category><![CDATA[markov chain monte]]></category>
		<category><![CDATA[markov chain monte carlo]]></category>
		<category><![CDATA[mcmc]]></category>
		<category><![CDATA[model analysis]]></category>
		<category><![CDATA[monte carlo simulation]]></category>
		<category><![CDATA[posterior probability]]></category>
		<category><![CDATA[probability density]]></category>
		<category><![CDATA[redshift galaxies]]></category>
		<category><![CDATA[statistical algorithm]]></category>
		<category><![CDATA[statistical inference]]></category>
		<category><![CDATA[stochastic model]]></category>
		<category><![CDATA[summary statistic]]></category>
		<category><![CDATA[target sequence]]></category>
		<category><![CDATA[tight constraints]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/approximate-bayesian-computation-for-astronomical-model-analysis-a-case-study-in-galaxy-demographics-and-morphological-transformation-at-high-redshift-replacement/</guid>
		<description><![CDATA[&#8220;Approximate Bayesian Computation&#8221; (ABC) represents a powerful methodology for the analysis of complex stochastic systems for which the likelihood of the observed data under an arbitrary set of input parameters may be entirely intractable-the latter condition rendering useless the standard machinery of tractable likelihood-based, Bayesian statistical inference (e.g. conventional Markov Chain Monte Carlo simulation; MCMC). [...]]]></description>
			<content:encoded><![CDATA[<p>&#8220;Approximate Bayesian Computation&#8221; (ABC) represents a powerful methodology for the analysis of complex stochastic systems for which the likelihood of the observed data under an arbitrary set of input parameters may be entirely intractable-the latter condition rendering useless the standard machinery of tractable likelihood-based, Bayesian statistical inference (e.g. conventional Markov Chain Monte Carlo simulation; MCMC). In this article we demonstrate the potential of ABC for astronomical model analysis by application to a case study in the morphological transformation of high redshift galaxies. To this end we develop, first, a stochastic model for the competing processes of merging and secular evolution in the early Universe; and second, through an ABC-based comparison against the observed demographics of massive (M_gal &gt; 10^11 M_sun) galaxies (at 1.5 &lt; z &lt; 3) in the CANDELS/EGS dataset we derive posterior probability densities for the key parameters of this model. The &quot;Sequential Monte Carlo&quot; (SMC) implementation of ABC exhibited herein, featuring both a self-generating target sequence and self-refining MCMC kernel, is amongst the most efficient of contemporary approaches to this important statistical algorithm. We highlight as well through our chosen case study the value of careful summary statistic selection, and demonstrate two modern strategies for assessment and optimisation in this regard. Ultimately, our ABC analysis of the high redshift morphological mix returns tight constraints on the evolving merger rate in the early Universe and favours major merging (with disc survival or rapid reformation) over secular evolution as the mechanism most responsible for building up the first generation of bulges in early-type disks.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/approximate-bayesian-computation-for-astronomical-model-analysis-a-case-study-in-galaxy-demographics-and-morphological-transformation-at-high-redshift-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Shift of the Baryon Acoustic Oscillation Scale: A Simple Physical Picture [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/the-shift-of-the-baryon-acoustic-oscillation-scale-a-simple-physical-picture-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/the-shift-of-the-baryon-acoustic-oscillation-scale-a-simple-physical-picture-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:33:29 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[analytic expression]]></category>
		<category><![CDATA[bia]]></category>
		<category><![CDATA[correlation function]]></category>
		<category><![CDATA[fluctuation]]></category>
		<category><![CDATA[linear growth]]></category>
		<category><![CDATA[linear theory]]></category>
		<category><![CDATA[Measurement]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[next generation]]></category>
		<category><![CDATA[oscillation]]></category>
		<category><![CDATA[perturbation theory]]></category>
		<category><![CDATA[reconstruction]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[simulation result]]></category>
		<category><![CDATA[theory calculations]]></category>
		<category><![CDATA[tracers]]></category>
		<category><![CDATA[wavelength]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/the-shift-of-the-baryon-acoustic-oscillation-scale-a-simple-physical-picture-replacement/</guid>
		<description><![CDATA[A shift of the baryon acoustic oscillation (BAO) scale to smaller values than predicted by linear theory was observed in simulations. In this paper, we try to provide an intuitive physical understanding of why this shift occurs, explaining in more pedagogical detail earlier perturbation theory calculations. We find that the shift is mainly due to [...]]]></description>
			<content:encoded><![CDATA[<p>A shift of the baryon acoustic oscillation (BAO) scale to smaller values than predicted by linear theory was observed in simulations. In this paper, we try to provide an intuitive physical understanding of why this shift occurs, explaining in more pedagogical detail earlier perturbation theory calculations. We find that the shift is mainly due to the following physical effect. A measurement of the BAO scale is more sensitive to regions with long wavelength overdensities than underdensities, because (due to non-linear growth and bias) these overdense regions contain larger fluctuations and more tracers and hence contribute more to the total correlation function. In overdense regions the BAO scale shrinks because such regions locally behave as positively curved closed universes, and hence a smaller scale than predicted by linear theory is measured in the total correlation function. Other effects which also contribute to the shift are briefly discussed. We provide approximate analytic expressions for the non-linear shift including a brief discussion of biased tracers and explain why reconstruction should entirely reverse the shift. Our expressions and findings are in agreement with simulation results, and confirm that non-linear shifts should not be problematic for next-generation BAO measurements.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/the-shift-of-the-baryon-acoustic-oscillation-scale-a-simple-physical-picture-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Particle-in-cell simulations of particle energization from low Mach number fast mode shocks [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/particle-in-cell-simulations-of-particle-energization-from-low-mach-number-fast-mode-shocks-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/particle-in-cell-simulations-of-particle-energization-from-low-mach-number-fast-mode-shocks-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:33:19 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[boundary method]]></category>
		<category><![CDATA[cell pic]]></category>
		<category><![CDATA[cell simulation]]></category>
		<category><![CDATA[dimensional particle]]></category>
		<category><![CDATA[electron distribution]]></category>
		<category><![CDATA[electron mass]]></category>
		<category><![CDATA[initial generation]]></category>
		<category><![CDATA[mach number]]></category>
		<category><![CDATA[magnetic pressure]]></category>
		<category><![CDATA[microphysics]]></category>
		<category><![CDATA[moving wall]]></category>
		<category><![CDATA[pic simulations]]></category>
		<category><![CDATA[plasma turbulence]]></category>
		<category><![CDATA[shock formation]]></category>
		<category><![CDATA[shock speed]]></category>
		<category><![CDATA[shock transition]]></category>
		<category><![CDATA[simulation result]]></category>
		<category><![CDATA[simulation time]]></category>
		<category><![CDATA[solar flare]]></category>
		<category><![CDATA[transition region]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/particle-in-cell-simulations-of-particle-energization-from-low-mach-number-fast-mode-shocks-replacement/</guid>
		<description><![CDATA[Astrophysical shocks are often studied in the high Mach number limit but weakly compressive fast shocks can occur in magnetic reconnection outflows and are considered to be a site of particle energization in solar flares. Here we study the microphysics of such perpendicular, low Mach number collisionless shocks using two-dimensional particle-in-cell (PIC) simulations with a [...]]]></description>
			<content:encoded><![CDATA[<p>Astrophysical shocks are often studied in the high Mach number limit but weakly compressive fast shocks can occur in magnetic reconnection outflows and are considered to be a site of particle energization in solar flares. Here we study the microphysics of such perpendicular, low Mach number collisionless shocks using two-dimensional particle-in-cell (PIC) simulations with a reduced ion/electron mass ratio and employ a moving wall boundary method for initial generation of the shock. This moving wall method allows for more control of the shock speed, smaller simulation box sizes, and longer simulation times than the commonly used fixed wall, reflection method of shock formation. Our results, which are independent of the shock formation method, reveal the prevalence shock drift acceleration (SDA) of both electron and ions in a purely perpendicular shock with Alfv\&#8217;en Mach number $M_A=6.8$ and ratio of thermal to magnetic pressure $\beta=8$. We determine the respective minimum energies required for electrons and ions to incur SDA. We derive a theoretical electron distribution via SDA that compares to the simulation results. We also show that a modified two-stream instability due to the incoming and reflecting ions in the shock transition region acts as the mechanism to generate collisionless plasma turbulence that sustains the shock.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/particle-in-cell-simulations-of-particle-energization-from-low-mach-number-fast-mode-shocks-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Very small-scale clustering of quasars from a complete quasar lens survey [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/very-small-scale-clustering-of-quasars-from-a-complete-quasar-lens-survey-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/very-small-scale-clustering-of-quasars-from-a-complete-quasar-lens-survey-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:33:10 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[correlation function]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[lens survey]]></category>
		<category><![CDATA[quasar]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/very-small-scale-clustering-of-quasars-from-a-complete-quasar-lens-survey-replacement/</guid>
		<description><![CDATA[We measure the small-scale (comoving separation 10 kpc/h &#60; r_p &#60; 200 kpc/h) two-point correlation function of quasars using a sample of 26 spectroscopically confirmed binary quasars at 0.6&#60;z 30), which may be suggestive of enhanced quasar activities by direct interactions.
]]></description>
			<content:encoded><![CDATA[<p>We measure the small-scale (comoving separation 10 kpc/h &lt; r_p &lt; 200 kpc/h) two-point correlation function of quasars using a sample of 26 spectroscopically confirmed binary quasars at 0.6&lt;z 30), which may be suggestive of enhanced quasar activities by direct interactions.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/very-small-scale-clustering-of-quasars-from-a-complete-quasar-lens-survey-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Gauge-invariant variables in general-relativistic perturbations: globalization and zero-mode problem [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/gauge-invariant-variables-in-general-relativistic-perturbations-globalization-and-zero-mode-problem-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/gauge-invariant-variables-in-general-relativistic-perturbations-globalization-and-zero-mode-problem-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:32:59 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[decomposition]]></category>
		<category><![CDATA[global sense]]></category>
		<category><![CDATA[globalization]]></category>
		<category><![CDATA[metric perturbations]]></category>
		<category><![CDATA[perturbation theory]]></category>
		<category><![CDATA[proof]]></category>
		<category><![CDATA[spacetime]]></category>
		<category><![CDATA[variables]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/gauge-invariant-variables-in-general-relativistic-perturbations-globalization-and-zero-mode-problem-replacement/</guid>
		<description><![CDATA[An outline of a proof of the local decomposition of linear metric perturbations into gauge-invariant and gauge-variant parts on an arbitrary background spacetime is briefly explained. We explicitly construct the gauge-invariant and gauge-variant parts of the linear metric perturbations based on some assumptions. We also point out the zero-mode problem is an essential problem to [...]]]></description>
			<content:encoded><![CDATA[<p>An outline of a proof of the local decomposition of linear metric perturbations into gauge-invariant and gauge-variant parts on an arbitrary background spacetime is briefly explained. We explicitly construct the gauge-invariant and gauge-variant parts of the linear metric perturbations based on some assumptions. We also point out the zero-mode problem is an essential problem to globalize of this decomposition of linear metric perturbations. The resolution of this zero-mode problem implies the possibility of the development of the higher-order gauge-invariant perturbation theory on an arbitrary background spacetime in a global sense.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/gauge-invariant-variables-in-general-relativistic-perturbations-globalization-and-zero-mode-problem-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Dark matter origin of the gamma ray emission from the galactic center observed by HESS [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/dark-matter-origin-of-the-gamma-ray-emission-from-the-galactic-center-observed-by-hess-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/dark-matter-origin-of-the-gamma-ray-emission-from-the-galactic-center-observed-by-hess-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:32:37 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[annihilation]]></category>
		<category><![CDATA[array]]></category>
		<category><![CDATA[cherenkov telescopes]]></category>
		<category><![CDATA[contraction]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[enhancement]]></category>
		<category><![CDATA[Fermi]]></category>
		<category><![CDATA[galactic center]]></category>
		<category><![CDATA[gamma ray emission]]></category>
		<category><![CDATA[hes]]></category>
		<category><![CDATA[morphology]]></category>
		<category><![CDATA[parsec]]></category>
		<category><![CDATA[photon]]></category>
		<category><![CDATA[profile]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[spectrum]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/dark-matter-origin-of-the-gamma-ray-emission-from-the-galactic-center-observed-by-hess-replacement/</guid>
		<description><![CDATA[We show that the gamma ray spectrum observed with the HESS array of Cherenkov telescopes coming from the Galactic Center (GC) region and identified with the source HESS J1745-290, is well fitted by the secondary photons coming from dark matter (DM) annihilation over a diffuse power-law background. The amount of photons and morphology of the [...]]]></description>
			<content:encoded><![CDATA[<p>We show that the gamma ray spectrum observed with the HESS array of Cherenkov telescopes coming from the Galactic Center (GC) region and identified with the source HESS J1745-290, is well fitted by the secondary photons coming from dark matter (DM) annihilation over a diffuse power-law background. The amount of photons and morphology of the signal localized within a region of few parsecs, require compressed DM profiles as those resulting from baryonic contraction, which offer $\sim 10^3$ enhancements in the signal over DM alone simulations. The fitted background from HESS data is consistent with recent Fermi-LAT observations of the same region.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/dark-matter-origin-of-the-gamma-ray-emission-from-the-galactic-center-observed-by-hess-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
	</channel>
</rss>

