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	<title>Vox Charta &#187; astro-ph</title>
	<atom:link href="http://voxcharta.org/category/astro-ph/feed/" rel="self" type="application/rss+xml" />
	<link>http://voxcharta.org</link>
	<description></description>
	<lastBuildDate>Thu, 23 Feb 2012 02:02:21 +0000</lastBuildDate>
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	<language>en</language>
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		<title>Evidence for top-heavy stellar initial mass functions with increasing density and decreasing metallicity</title>
		<link>http://voxcharta.org/2012/02/22/evidence-for-top-heavy-stellar-initial-mass-functions-with-increasing-density-and-decreasing-metallicity/</link>
		<comments>http://voxcharta.org/2012/02/22/evidence-for-top-heavy-stellar-initial-mass-functions-with-increasing-density-and-decreasing-metallicity/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 02:02:21 +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[arches]]></category>
		<category><![CDATA[chemical enrichment]]></category>
		<category><![CDATA[cloud core]]></category>
		<category><![CDATA[cluster formation]]></category>
		<category><![CDATA[dwarf galaxy]]></category>
		<category><![CDATA[expulsion]]></category>
		<category><![CDATA[fundamental plane]]></category>
		<category><![CDATA[galactic globular cluster]]></category>
		<category><![CDATA[high mass]]></category>
		<category><![CDATA[imf]]></category>
		<category><![CDATA[initial mass function]]></category>
		<category><![CDATA[mass radius]]></category>
		<category><![CDATA[NGC]]></category>
		<category><![CDATA[qualitative agreement]]></category>
		<category><![CDATA[radii]]></category>
		<category><![CDATA[residual gas]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[stellar mass]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/evidence-for-top-heavy-stellar-initial-mass-functions-with-increasing-density-and-decreasing-metallicity/</guid>
		<description><![CDATA[Residual-gas expulsion after cluster formation has recently been shown to leave an imprint in the low-mass present-day stellar mass function (PDMF) which allowed the estimation of birth conditions of some Galactic globular clusters (GCs) such as mass, radius and star formation efficiency. We show that in order to explain their characteristics (masses, radii, metallicity, PDMF) [...]]]></description>
			<content:encoded><![CDATA[<p>Residual-gas expulsion after cluster formation has recently been shown to leave an imprint in the low-mass present-day stellar mass function (PDMF) which allowed the estimation of birth conditions of some Galactic globular clusters (GCs) such as mass, radius and star formation efficiency. We show that in order to explain their characteristics (masses, radii, metallicity, PDMF) their stellar initial mass function (IMF) must have been top-heavy. It is found that the IMF is required to become more top-heavy the lower the cluster metallicity and the larger the pre-GC cloud-core density are. The deduced trends are in qualitative agreement with theoretical expectation. The results are consistent with estimates of the shape of the high-mass end of the IMF in the Arches cluster, Westerlund 1, R136 and NGC 3603, as well as with the IMF independently constrained for ultra-compact dwarf galaxies (UCDs). The latter suggests that GCs and UCDs might have formed along the same channel or that UCDs formed via mergers of GCs. A fundamental plane is found which describes the variation of the IMF with density and metallicity of the pre-GC cloud-cores simultaneously. The implications for the evolution of galaxies and chemical enrichment over cosmological times are expected to be major.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/evidence-for-top-heavy-stellar-initial-mass-functions-with-increasing-density-and-decreasing-metallicity/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Spatial variation in the fine-structure constant &#8212; new results from VLT/UVES</title>
		<link>http://voxcharta.org/2012/02/22/spatial-variation-in-the-fine-structure-constant-new-results-from-vltuves/</link>
		<comments>http://voxcharta.org/2012/02/22/spatial-variation-in-the-fine-structure-constant-new-results-from-vltuves/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 02:02:07 +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[absorption line spectra]]></category>
		<category><![CDATA[alpha alpha]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[clouds]]></category>
		<category><![CDATA[confidence level]]></category>
		<category><![CDATA[consistency]]></category>
		<category><![CDATA[deg]]></category>
		<category><![CDATA[delta alpha]]></category>
		<category><![CDATA[echelle spectrograph]]></category>
		<category><![CDATA[keck]]></category>
		<category><![CDATA[null model]]></category>
		<category><![CDATA[robustness]]></category>
		<category><![CDATA[sigma]]></category>
		<category><![CDATA[spatial variation]]></category>
		<category><![CDATA[statistical significance level]]></category>
		<category><![CDATA[subset]]></category>
		<category><![CDATA[systematic effects]]></category>
		<category><![CDATA[Telescope]]></category>
		<category><![CDATA[vlt]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/spatial-variation-in-the-fine-structure-constant-new-results-from-vltuves/</guid>
		<description><![CDATA[(abridged) We present a new analysis of a large sample of quasar absorption-line spectra obtained using UVES (the Ultraviolet and Visual Echelle Spectrograph) on the VLT (Very Large Telescope) in Chile. In the VLT sample (154 absorbers), we find evidence that alpha increases with increasing cosmological distance from Earth. However, as previously shown, the Keck [...]]]></description>
			<content:encoded><![CDATA[<p>(abridged) We present a new analysis of a large sample of quasar absorption-line spectra obtained using UVES (the Ultraviolet and Visual Echelle Spectrograph) on the VLT (Very Large Telescope) in Chile. In the VLT sample (154 absorbers), we find evidence that alpha increases with increasing cosmological distance from Earth. However, as previously shown, the Keck sample (141 absorbers) provided evidence for a smaller alpha in the distant absorption clouds. Upon combining the samples an apparent variation of alpha across the sky emerges which is well represented by an angular dipole model pointing in the direction RA=(17.3 +/- 1.0) hr, dec. = (-61 +/- 10) deg, with amplitude (0.97 +0.22/-0.20) x 10^(-5). The dipole model is required at the 4.1 sigma statistical significance level over a simple monopole model where alpha is the same across the sky (but possibly different to the current laboratory value). The data sets reveal a number of remarkable consistencies: various data cuts are consistent and there is consistency in the overlap region of the Keck and VLT samples. Assuming a dipole-only (i.e. no-monopole) model whose amplitude grows proportionally with `lookback-time distance&#8217; (r=ct, where t is the lookback time), the amplitude is (1.1 +/- 0.2) x 10^(-6) GLyr^(-1) and the model is significant at the 4.2 sigma confidence level over the null model [Delta alpha]/alpha = 0). We apply robustness checks and demonstrate that the dipole effect does not originate from a small subset of the absorbers or spectra. We present an analysis of systematic effects, and are unable to identify any single systematic effect which can emulate the observed variation in alpha.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/spatial-variation-in-the-fine-structure-constant-new-results-from-vltuves/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Relativistic Resonant Relations between Massive Black Hole Binary and Extreme Mass Ratio Inspiral</title>
		<link>http://voxcharta.org/2012/02/22/relativistic-resonant-relations-between-massive-black-hole-binary-and-extreme-mass-ratio-inspiral/</link>
		<comments>http://voxcharta.org/2012/02/22/relativistic-resonant-relations-between-massive-black-hole-binary-and-extreme-mass-ratio-inspiral/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 02:01:52 +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[approximation]]></category>
		<category><![CDATA[eccentricity]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[mass ratio]]></category>
		<category><![CDATA[massive black hole]]></category>
		<category><![CDATA[mbhb]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[radiation reaction]]></category>
		<category><![CDATA[relativistic effects]]></category>
		<category><![CDATA[resonance]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/relativistic-resonant-relations-between-massive-black-hole-binary-and-extreme-mass-ratio-inspiral/</guid>
		<description><![CDATA[One component of a massive black hole binary (MBHB) might capture a small third body, and then a hierarchical, inclined triple system would be formed. With the post-Newtonian approximation including radiation reaction, we analyzed the evolution of the triple initially with small eccentricities. We found that an essentially new resonant relation could arise in the [...]]]></description>
			<content:encoded><![CDATA[<p>One component of a massive black hole binary (MBHB) might capture a small third body, and then a hierarchical, inclined triple system would be formed. With the post-Newtonian approximation including radiation reaction, we analyzed the evolution of the triple initially with small eccentricities. We found that an essentially new resonant relation could arise in the triple system. Here relativistic effects are crucial. Relativistic resonances, including the new one, stably work even for an outer MBHB of comparable masses, and significantly change the orbit of the inner small body.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/relativistic-resonant-relations-between-massive-black-hole-binary-and-extreme-mass-ratio-inspiral/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Electron Capture Decay of 163-Ho to Measure the Electron Neutrino Mass with sub-eV Accuracy and Beyond [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/22/the-electron-capture-decay-of-163-ho-to-measure-the-electron-neutrino-mass-with-sub-ev-accuracy-and-beyond-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/22/the-electron-capture-decay-of-163-ho-to-measure-the-electron-neutrino-mass-with-sub-ev-accuracy-and-beyond-cross-listing/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 02:01:43 +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[accuracy]]></category>
		<category><![CDATA[decay]]></category>
		<category><![CDATA[electron neutrino]]></category>
		<category><![CDATA[roadmap]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/the-electron-capture-decay-of-163-ho-to-measure-the-electron-neutrino-mass-with-sub-ev-accuracy-and-beyond-cross-listing/</guid>
		<description><![CDATA[We have investigated the possibility of measuring the electron neutrino mass with sub-eV sensitivity by studying the electron capture decay of 163-Ho with cryogenic microcalorimeters. In this paper we will introduce an experiment&#8217;s concept, discuss the technical requirements, and identify a roadmap to reach a sensitivity of 0.1 eV and beyond.
]]></description>
			<content:encoded><![CDATA[<p>We have investigated the possibility of measuring the electron neutrino mass with sub-eV sensitivity by studying the electron capture decay of 163-Ho with cryogenic microcalorimeters. In this paper we will introduce an experiment&#8217;s concept, discuss the technical requirements, and identify a roadmap to reach a sensitivity of 0.1 eV and beyond.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/the-electron-capture-decay-of-163-ho-to-measure-the-electron-neutrino-mass-with-sub-ev-accuracy-and-beyond-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Evolution of Group Galaxies from the First Red-Sequence Cluster Survey</title>
		<link>http://voxcharta.org/2012/02/22/evolution-of-group-galaxies-from-the-first-red-sequence-cluster-survey/</link>
		<comments>http://voxcharta.org/2012/02/22/evolution-of-group-galaxies-from-the-first-red-sequence-cluster-survey/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:59:57 +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[butcher]]></category>
		<category><![CDATA[cluster survey]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[dependence]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[galaxy group]]></category>
		<category><![CDATA[gradient]]></category>
		<category><![CDATA[group galaxies]]></category>
		<category><![CDATA[grp]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[massive galaxy]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[proxy]]></category>
		<category><![CDATA[radius]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[redshift range]]></category>
		<category><![CDATA[rgrp]]></category>
		<category><![CDATA[sigma 5]]></category>
		<category><![CDATA[stellar mass]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/evolution-of-group-galaxies-from-the-first-red-sequence-cluster-survey/</guid>
		<description><![CDATA[We study the evolution of the red galaxy fraction (f_red) in 905 galaxy groups with 0.15 &#60; z 2. In general, groups at lower redshifts exhibit larger f_red than those at higher redshifts, showing a group Butcher-Oemler effect. We investigate the evolution of f_red by examining its dependence on four parameters, which can be classified [...]]]></description>
			<content:encoded><![CDATA[<p>We study the evolution of the red galaxy fraction (f_red) in 905 galaxy groups with 0.15 &lt; z 2. In general, groups at lower redshifts exhibit larger f_red than those at higher redshifts, showing a group Butcher-Oemler effect. We investigate the evolution of f_red by examining its dependence on four parameters, which can be classified as one intrinsic and three environmental: galaxy stellar mass (M_*), total group stellar mass(M_{*,grp}, a proxy for group halo mass), normalized group-centric radius (r_grp), and local galaxy density (Sigma_5). We find that M_* is the dominant parameter such that there is a strong correlation between f_red and galaxy stellar mass. Furthermore, the dependence of f_red on the environmental parameters is also a strong function of M_*. Massive galaxies (M_* &gt; 10^11 M_sun) show little dependence of f_red on r_grp, M_{*,grp}, and Sigma_5 over the redshift range. The dependence of f_red on these parameters is primarily seen for galaxies with lower masses, especially for M_* &lt; 10^{10.6} M_{sun}. We observe an apparent `group down-sizing&#039; effect, in that galaxies in lower-mass halos, after controlling for galaxy stellar mass, have lower f_red. We find a dependence of \fred on both \rgrp and \SigmaF after the other parameters are controlled. At a fixed \rgrp, there is a significant dependence of f_red on Sigma_5, while r_grp gradients of f_red are seen for galaxies in similar Sigma_5 regions. This indicates &#8230;..</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/evolution-of-group-galaxies-from-the-first-red-sequence-cluster-survey/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The physics of the fundamental metallicity relation</title>
		<link>http://voxcharta.org/2012/02/22/the-physics-of-the-fundamental-metallicity-relation/</link>
		<comments>http://voxcharta.org/2012/02/22/the-physics-of-the-fundamental-metallicity-relation/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:59:39 +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[analytic model]]></category>
		<category><![CDATA[decreases]]></category>
		<category><![CDATA[efficiency]]></category>
		<category><![CDATA[element]]></category>
		<category><![CDATA[inflow]]></category>
		<category><![CDATA[intergalactic medium]]></category>
		<category><![CDATA[ism]]></category>
		<category><![CDATA[massive galaxy]]></category>
		<category><![CDATA[metal enrichment]]></category>
		<category><![CDATA[numerical simulation]]></category>
		<category><![CDATA[outflow]]></category>
		<category><![CDATA[physical processes]]></category>
		<category><![CDATA[physics]]></category>
		<category><![CDATA[sfr]]></category>
		<category><![CDATA[slope]]></category>
		<category><![CDATA[solar mass]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[stellar mass]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/the-physics-of-the-fundamental-metallicity-relation/</guid>
		<description><![CDATA[We present a simple, redshift-independent analytic model that explains the local Fundamental Metallicity Relation (FMR), taking into account the physical processes of star formation, inflow of metal-poor intergalactic medium (IGM) gas, and the outflow of metal rich interstellar medium (ISM) gas. We show that the physics of the FMR can be summarised as follows: for [...]]]></description>
			<content:encoded><![CDATA[<p>We present a simple, redshift-independent analytic model that explains the local Fundamental Metallicity Relation (FMR), taking into account the physical processes of star formation, inflow of metal-poor intergalactic medium (IGM) gas, and the outflow of metal rich interstellar medium (ISM) gas. We show that the physics of the FMR can be summarised as follows: for massive galaxies with stellar mass larger than 10^11 solar masses, ISM metal enrichment due to star formation is compensated by inflow of metal poor IGM gas, leading to a constant value of the gas metallicity with star formation rate (SFR); outflows are rendered negligible as a result of the large potential wells of these galaxies. On the other hand, as a result of their smaller SFR, less massive galaxies produce less heavy elements that are also more efficiently ejected due to their shallow potential wells; as a result, for a given stellar mass, the gas metallicity decreases with SFR. For such galaxies, the outflow efficiency determines both the slope, and the knee of the metallicity-SFR relation. The model is then successfully matched to results from numerical simulations including metal enrichment and feedback at higher redshifts.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/the-physics-of-the-fundamental-metallicity-relation/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Significance of tension for gravitating masses in Kaluza-Klein models [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/22/significance-of-tension-for-gravitating-masses-in-kaluza-klein-models-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/22/significance-of-tension-for-gravitating-masses-in-kaluza-klein-models-cross-listing/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:59:26 +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[astrophysical objects]]></category>
		<category><![CDATA[compact object]]></category>
		<category><![CDATA[equality]]></category>
		<category><![CDATA[equation of state]]></category>
		<category><![CDATA[external space]]></category>
		<category><![CDATA[internal space]]></category>
		<category><![CDATA[kaluza klein]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[Sun]]></category>
		<category><![CDATA[tension]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/significance-of-tension-for-gravitating-masses-in-kaluza-klein-models-cross-listing/</guid>
		<description><![CDATA[In this report, we consider the six-dimensional Kaluza-Klein models with spherical compactification of the internal space. Here, we investigate the case of bare gravitating compact objects with the dustlike equation of state $\hat p_0=0$ in the external (our) space and an arbitrary equation of state $\hat p_1=\Omega \hat \varepsilon$ in the internal space. These models [...]]]></description>
			<content:encoded><![CDATA[<p>In this report, we consider the six-dimensional Kaluza-Klein models with spherical compactification of the internal space. Here, we investigate the case of bare gravitating compact objects with the dustlike equation of state $\hat p_0=0$ in the external (our) space and an arbitrary equation of state $\hat p_1=\Omega \hat \varepsilon$ in the internal space. These models satisfy the classical gravitational tests. However, we show that gravitating masses acquire effective relativistic pressure in the external space. Such pressure contradicts the observations of compact astrophysical objects (e.g., the Sun). The equality $\Omega =-1/2$ (i.e. tension) is the only possibility to preserve the dustlike equation of state in the external space. Therefore, tension plays a crucial role for the considered models.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/significance-of-tension-for-gravitating-masses-in-kaluza-klein-models-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Measurement of Galactic Logarithmic Spiral Arm Pitch Angle Using Two-Dimensional Fast Fourier Transform Decomposition</title>
		<link>http://voxcharta.org/2012/02/22/measurement-of-galactic-logarithmic-spiral-arm-pitch-angle-using-two-dimensional-fast-fourier-transform-decomposition/</link>
		<comments>http://voxcharta.org/2012/02/22/measurement-of-galactic-logarithmic-spiral-arm-pitch-angle-using-two-dimensional-fast-fourier-transform-decomposition/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:58:45 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[angle]]></category>
		<category><![CDATA[classification scheme]]></category>
		<category><![CDATA[decomposition]]></category>
		<category><![CDATA[fourier transformation]]></category>
		<category><![CDATA[galaxy image]]></category>
		<category><![CDATA[genesis]]></category>
		<category><![CDATA[hubble classification]]></category>
		<category><![CDATA[image processing]]></category>
		<category><![CDATA[logarithmic spiral]]></category>
		<category><![CDATA[Measurement]]></category>
		<category><![CDATA[methodology]]></category>
		<category><![CDATA[morphological feature]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[pitch angle]]></category>
		<category><![CDATA[quotes]]></category>
		<category><![CDATA[robustness]]></category>
		<category><![CDATA[spiral arm]]></category>
		<category><![CDATA[spiral galaxy]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/measurement-of-galactic-logarithmic-spiral-arm-pitch-angle-using-two-dimensional-fast-fourier-transform-decomposition/</guid>
		<description><![CDATA[A logarithmic spiral is a prominent feature appearing in a majority of observed galaxies. This feature has long been associated with the traditional Hubble classification scheme, but historical quotes of pitch angle of spiral galaxies have been almost exclusively qualitative. We have developed a methodology, utilizing two-dimensional fast Fourier transformations of images of spiral galaxies, [...]]]></description>
			<content:encoded><![CDATA[<p>A logarithmic spiral is a prominent feature appearing in a majority of observed galaxies. This feature has long been associated with the traditional Hubble classification scheme, but historical quotes of pitch angle of spiral galaxies have been almost exclusively qualitative. We have developed a methodology, utilizing two-dimensional fast Fourier transformations of images of spiral galaxies, in order to isolate and measure the pitch angles of their spiral arms. Our technique provides a quantitative way to measure this morphological feature. This will allow comparison of spiral galaxy pitch angle to other galactic parameters and test spiral arm genesis theories. In this work, we detail our image processing and analysis of spiral galaxy images and discuss the robustness of our analysis techniques.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/measurement-of-galactic-logarithmic-spiral-arm-pitch-angle-using-two-dimensional-fast-fourier-transform-decomposition/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Contribution of TP-AGB and RHeB Stars to the Near-IR Luminosity of Local Galaxies: Implications for Stellar Mass Measurements of High Redshift Galaxies</title>
		<link>http://voxcharta.org/2012/02/22/the-contribution-of-tp-agb-and-rheb-stars-to-the-near-ir-luminosity-of-local-galaxies-implications-for-stellar-mass-measurements-of-high-redshift-galaxies/</link>
		<comments>http://voxcharta.org/2012/02/22/the-contribution-of-tp-agb-and-rheb-stars-to-the-near-ir-luminosity-of-local-galaxies-implications-for-stellar-mass-measurements-of-high-redshift-galaxies/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:58:26 +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[acs]]></category>
		<category><![CDATA[agb stars]]></category>
		<category><![CDATA[asymptotic giant branch]]></category>
		<category><![CDATA[discrepancy]]></category>
		<category><![CDATA[fluctuation]]></category>
		<category><![CDATA[gyr]]></category>
		<category><![CDATA[helium]]></category>
		<category><![CDATA[high spatial resolution]]></category>
		<category><![CDATA[ir luminosity]]></category>
		<category><![CDATA[mass measurement]]></category>
		<category><![CDATA[myr]]></category>
		<category><![CDATA[nearby galaxy]]></category>
		<category><![CDATA[observational result]]></category>
		<category><![CDATA[redshift galaxies]]></category>
		<category><![CDATA[rheb]]></category>
		<category><![CDATA[star formation history]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[timescale]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/the-contribution-of-tp-agb-and-rheb-stars-to-the-near-ir-luminosity-of-local-galaxies-implications-for-stellar-mass-measurements-of-high-redshift-galaxies/</guid>
		<description><![CDATA[Using high spatial resolution HST WFC3 and ACS imaging of resolved stellar populations, we constrain the contribution of thermally-pulsing asymptotic giant branch (TP-AGB) stars and red helium burning (RHeB) stars to the 1.6 um near-infrared (NIR) luminosities of 23 nearby galaxies. The TP-AGB phase contributes as much as 17% of the integrated F160W flux, even [...]]]></description>
			<content:encoded><![CDATA[<p>Using high spatial resolution HST WFC3 and ACS imaging of resolved stellar populations, we constrain the contribution of thermally-pulsing asymptotic giant branch (TP-AGB) stars and red helium burning (RHeB) stars to the 1.6 um near-infrared (NIR) luminosities of 23 nearby galaxies. The TP-AGB phase contributes as much as 17% of the integrated F160W flux, even when the red giant branch is well populated. The RHeB population contribution can match or even exceed the TP-AGB contribution, providing as much as 21% of the integrated F160W light. The NIR mass-to-light (M/L) ratio should therefore be expected to vary significantly due to fluctuations in the star formation rate over timescales from 25 Myr to several Gyr. We compare our observational results to predictions based on optically derived star formation histories and stellar population synthesis (SPS) models, including models based on the Padova isochrones (used in popular SPS programs). The SPS models generally reproduce the expected numbers of TP-AGB stars in the sample. The same SPS models, however, give a larger discrepancy in the F160W flux contribution from the TP-AGB stars, over-predicting the flux by a weighted mean factor of 2.3 +/-0.8. This larger offset is driven by the prediction of modest numbers of high luminosity TP-AGB stars at young (&lt;300 Myrs) ages. The best-fit SPS models simultaneously tend to under-predict the numbers and fluxes of stars on the RHeB sequence, typically by a factor of 2.0+/-0.6 for galaxies with significant numbers of RHeBs. Coincidentally, over-prediction of the TP-AGB and under-prediction of the RHeBs result in a NIR M/L ratio largely unchanged for a rapid star formation rate. However, the NIR-to-optical flux ratio of galaxies could be significantly smaller than AGB-rich models would predict, an outcome that has been observed in some intermediate redshift post-starburst galaxies. (Abridged)</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/the-contribution-of-tp-agb-and-rheb-stars-to-the-near-ir-luminosity-of-local-galaxies-implications-for-stellar-mass-measurements-of-high-redshift-galaxies/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>3-D radiative transfer in clumped hot star winds I. Influence of clumping on the resonance line formation</title>
		<link>http://voxcharta.org/2012/02/22/3-d-radiative-transfer-in-clumped-hot-star-winds-i-influence-of-clumping-on-the-resonance-line-formation/</link>
		<comments>http://voxcharta.org/2012/02/22/3-d-radiative-transfer-in-clumped-hot-star-winds-i-influence-of-clumping-on-the-resonance-line-formation/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:58:00 +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[correct mass]]></category>
		<category><![CDATA[hot star]]></category>
		<category><![CDATA[line formation]]></category>
		<category><![CDATA[line strength]]></category>
		<category><![CDATA[mass conservation]]></category>
		<category><![CDATA[mass loss rates]]></category>
		<category><![CDATA[model parameter]]></category>
		<category><![CDATA[number density]]></category>
		<category><![CDATA[radiative transfer calculations]]></category>
		<category><![CDATA[radiative transfer code]]></category>
		<category><![CDATA[representative model]]></category>
		<category><![CDATA[resonance line]]></category>
		<category><![CDATA[star winds]]></category>
		<category><![CDATA[stellar wind]]></category>
		<category><![CDATA[velocity field]]></category>
		<category><![CDATA[velocity gradient]]></category>
		<category><![CDATA[wind component]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/3-d-radiative-transfer-in-clumped-hot-star-winds-i-influence-of-clumping-on-the-resonance-line-formation/</guid>
		<description><![CDATA[The true mass-loss rates from massive stars are important for many branches of astrophysics. For the correct modeling of the resonance lines, which are among the key diagnostics of stellar mass-loss, the stellar wind clumping turned out to be very important. In order to incorporate clumping into radiative transfer calculation, 3-D models are required. Various [...]]]></description>
			<content:encoded><![CDATA[<p>The true mass-loss rates from massive stars are important for many branches of astrophysics. For the correct modeling of the resonance lines, which are among the key diagnostics of stellar mass-loss, the stellar wind clumping turned out to be very important. In order to incorporate clumping into radiative transfer calculation, 3-D models are required. Various properties of the clumps may have strong impact on the resonance line formation and, therefore, on the determination of empirical mass-loss rates. We incorporate the 3-D nature of the stellar wind clumping into radiative transfer calculations and investigate how different model parameters influence the resonance line formation. We develop a full 3-D Monte Carlo radiative transfer code for inhomogeneous expanding stellar winds. The number density of clumps follows the mass conservation. For the first time, realistic 3-D models that describe the dense as well as the tenuous wind components are used to model the formation of resonance lines in a clumped stellar wind. At the same time, non-monotonic velocity fields are accounted for. The 3-D density and velocity wind inhomogeneities show very strong impact on the resonance line formation. The different parameters describing the clumping and the velocity field results in different line strengths and profiles. We present a set of representative models for various sets of model parameters and investigate how the resonance lines are affected. Our 3-D models show that the line opacity is reduced for larger clump separation and for more shallow velocity gradients within the clumps. Our new model demonstrates that to obtain empirically correct mass-loss rates from the UV resonance lines, the wind clumping and its 3-D nature must be taken into account.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/3-d-radiative-transfer-in-clumped-hot-star-winds-i-influence-of-clumping-on-the-resonance-line-formation/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Identification of Ambient Molecular Clouds Associated with Galactic Supernova Remnant IC443</title>
		<link>http://voxcharta.org/2012/02/22/identification-of-ambient-molecular-clouds-associated-with-galactic-supernova-remnant-ic443/</link>
		<comments>http://voxcharta.org/2012/02/22/identification-of-ambient-molecular-clouds-associated-with-galactic-supernova-remnant-ic443/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:57:15 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bright clouds]]></category>
		<category><![CDATA[clump]]></category>
		<category><![CDATA[college radio astronomy]]></category>
		<category><![CDATA[core collapse]]></category>
		<category><![CDATA[dense core]]></category>
		<category><![CDATA[diffuse cloud]]></category>
		<category><![CDATA[hco]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[kinematic features]]></category>
		<category><![CDATA[molecular cloud]]></category>
		<category><![CDATA[nearby star]]></category>
		<category><![CDATA[physical relationship]]></category>
		<category><![CDATA[progenitor star]]></category>
		<category><![CDATA[radio astronomy observatory]]></category>
		<category><![CDATA[snr]]></category>
		<category><![CDATA[supernova evolution]]></category>
		<category><![CDATA[supernova remnant]]></category>
		<category><![CDATA[tracers]]></category>
		<category><![CDATA[velocity range]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/identification-of-ambient-molecular-clouds-associated-with-galactic-supernova-remnant-ic443/</guid>
		<description><![CDATA[The Galactic supernova remnant (SNR) IC443 is one of the most studied core-collapse SNRs for its interaction with molecular clouds. However, the ambient molecular clouds with which IC443 is interacting have not been thoroughly studied and remain poorly understood. Using Five College Radio Astronomy Observatory 14m telescope, we obtained fully sampled maps of ~ 1{\deg} [...]]]></description>
			<content:encoded><![CDATA[<p>The Galactic supernova remnant (SNR) IC443 is one of the most studied core-collapse SNRs for its interaction with molecular clouds. However, the ambient molecular clouds with which IC443 is interacting have not been thoroughly studied and remain poorly understood. Using Five College Radio Astronomy Observatory 14m telescope, we obtained fully sampled maps of ~ 1{\deg} \times 1{\deg} region toward IC443 in the 12CO J=1-0 and HCO+ J=1-0 lines. In addition to the previously known molecular clouds in the velocity range v_lsr = -6 to -1 km/s (-3 km/s clouds), our observations reveal two new ambient molecular cloud components: small (~ 1&#8242;) bright clouds in v_lsr = -8 to -3 km/s (SCs), and diffuse clouds in v_lsr = +3 to +10 km/s (+5 km/s clouds). Our data also reveal the detailed kinematics of the shocked molecular gas in IC443, however the focus of this paper is the physical relationship between the shocked clumps and the ambient cloud components. We find strong evidence that the SCs are associated with the shocked clumps. This is supported by the positional coincidence of the SCs with shocked clumps and other tracers of shocks. Furthermore, the kinematic features of some shocked clumps suggest that these are the ablated material from the SCs upon the impact of the SNR shock. The SCs are interpreted as dense cores of parental molecular clouds that survived the destruction by the pre-supernova evolution of the progenitor star or its nearby stars. We propose that the expanding SNR shock is now impacting some of the remaining cores and the gas is being ablated and accelerated producing the shocked molecular gas. The morphology of the +5 km/s clouds suggests an association with IC443. On the other hand, the -3 km/s clouds show no evidence for interaction.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/identification-of-ambient-molecular-clouds-associated-with-galactic-supernova-remnant-ic443/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Hi Environment of Counter-rotating Gas Hosts: Gas Accretion from Cold Gas Blobs</title>
		<link>http://voxcharta.org/2012/02/22/the-hi-environment-of-counter-rotating-gas-hosts-gas-accretion-from-cold-gas-blobs/</link>
		<comments>http://voxcharta.org/2012/02/22/the-hi-environment-of-counter-rotating-gas-hosts-gas-accretion-from-cold-gas-blobs/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:56:40 +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[cold gas]]></category>
		<category><![CDATA[companion]]></category>
		<category><![CDATA[comparable size]]></category>
		<category><![CDATA[dwarf]]></category>
		<category><![CDATA[dwarf galaxy]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[galaxy population]]></category>
		<category><![CDATA[hi gas]]></category>
		<category><![CDATA[incompleteness]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[morphology]]></category>
		<category><![CDATA[msun]]></category>
		<category><![CDATA[neighbour]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[stellar body]]></category>
		<category><![CDATA[synthesis imaging]]></category>
		<category><![CDATA[tidal interaction]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/the-hi-environment-of-counter-rotating-gas-hosts-gas-accretion-from-cold-gas-blobs/</guid>
		<description><![CDATA[We probe the HI properties and the gas environments of three early-type barred galaxies harbouring counter-rotating ionized gas, NGC 128, NGC 3203 and NGC 7332. Each system has one or more optically-identified galaxy, at a similar or as yet unknown redshift within a 50 kpc projected radius. Using HI synthesis imaging data, we investigate the [...]]]></description>
			<content:encoded><![CDATA[<p>We probe the HI properties and the gas environments of three early-type barred galaxies harbouring counter-rotating ionized gas, NGC 128, NGC 3203 and NGC 7332. Each system has one or more optically-identified galaxy, at a similar or as yet unknown redshift within a 50 kpc projected radius. Using HI synthesis imaging data, we investigate the hypothesis that the counter-rotating gas in these galaxies has been accreted from their neighbours. In NGC 128 and NGC 3203, we find 9.6e7 and 2.3e8 Msun of HI, respectively, covering almost the entire stellar bodies of dwarf companions that appear physically connected. Both the HI morphology and kinematics are suggestive of tidal interactions. In NGC 7332, we do not find any directly-associated HI. Instead, NGC 7339, a neighbour of a comparable size at about 10 kpc, is found with 8.9e8 Msun of HI gas. More recently in a single dish observation, however, another group discovered a large HI structure which seems to be an extension of NGC 7339&#8217;s HI disc and also covers NGC 7332. All these observations thus suggest that HI gas is being accreted in these three galaxies from their companions, which is likely responsible for the kinematically-decoupled gas component present in their central region. Considering the incompleteness of existing studies of the faint dwarf galaxy population both in the optical and in HI, accretion from cold gas blobs, presumably gas-rich dwarfs, is expected to occur even more frequently than what is inferred from such cases that have been observed to date.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/the-hi-environment-of-counter-rotating-gas-hosts-gas-accretion-from-cold-gas-blobs/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Multiple outflows from the luminous YSO IRAS 07422-2001</title>
		<link>http://voxcharta.org/2012/02/22/multiple-outflows-from-the-luminous-yso-iras-07422-2001/</link>
		<comments>http://voxcharta.org/2012/02/22/multiple-outflows-from-the-luminous-yso-iras-07422-2001/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:55:39 +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[angular resolution]]></category>
		<category><![CDATA[band image]]></category>
		<category><![CDATA[clump]]></category>
		<category><![CDATA[cluster candidates]]></category>
		<category><![CDATA[extinction]]></category>
		<category><![CDATA[ir wavelengths]]></category>
		<category><![CDATA[ira]]></category>
		<category><![CDATA[massive star cluster]]></category>
		<category><![CDATA[outflow]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[radiative transfer model]]></category>
		<category><![CDATA[spectral energy distribution]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[stellar object]]></category>
		<category><![CDATA[yso]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/multiple-outflows-from-the-luminous-yso-iras-07422-2001/</guid>
		<description><![CDATA[The luminous Young Stellar Object (YSO) IRAS 07422-2001 is studied in the infrared. We discover star forming activity in embedded clusters located in a cloud detected at mid-IR wavelengths in emission. Multiple outflows are discovered from these clusters in the H_2 ro-vibrational line at 2.122 micron. We detect at least six outflows from the cluster [...]]]></description>
			<content:encoded><![CDATA[<p>The luminous Young Stellar Object (YSO) IRAS 07422-2001 is studied in the infrared. We discover star forming activity in embedded clusters located in a cloud detected at mid-IR wavelengths in emission. Multiple outflows are discovered from these clusters in the H_2 ro-vibrational line at 2.122 micron. We detect at least six outflows from the cluster associated with the IRAS source and another outflow from a source located in a cluster detected ~2.7 arcmin NE of the IRAS source. Additional star formation is taking place in two other cluster candidates within the cloud. Three of the YSOs in the cluster associated with the IRAS source are detected at 11.2 micron at an angular resolution of ~0.8 arcsec. We have a tentative detection of a circumstellar disk in this cluster, seen as an extinction lane in the J and H-band images. The spectral energy distributions (SEDs) of the dominant YSOs in the cluster associated with the IRAS source and in the NE cluster are studied using radiative transfer models and the properties of the YSOs are estimated. The YSO associated with the IRAS source is probably in a very early Class I stage of formation. The source identified as the dominant YSO in the NE cluster appears to be older than the dominant YSO in the cluster associated with the IRAS source, but its observed flux seems to be contaminated by extra emission, which suggests the presence of a young source contributing to the SED at far-IR wavelengths. The star formation observed in the field of IRAS 07422-2001 supports the idea of hierarchical formation of massive star clusters and the growth of massive young stellar objects near the centres of multiple sub-clusters in a star forming clump through competitive accretion.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/multiple-outflows-from-the-luminous-yso-iras-07422-2001/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>First Science Observations with SOFIA/FORCAST: 6 TO 37 micron Imaging of Orion BN/KL</title>
		<link>http://voxcharta.org/2012/02/22/first-science-observations-with-sofiaforcast-6-to-37-micron-imaging-of-orion-bnkl/</link>
		<comments>http://voxcharta.org/2012/02/22/first-science-observations-with-sofiaforcast-6-to-37-micron-imaging-of-orion-bnkl/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:55:12 +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[airborne telescope]]></category>
		<category><![CDATA[first science]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[high mass]]></category>
		<category><![CDATA[images]]></category>
		<category><![CDATA[intense investigation]]></category>
		<category><![CDATA[mass star]]></category>
		<category><![CDATA[micron]]></category>
		<category><![CDATA[orion nebula]]></category>
		<category><![CDATA[resolution observations]]></category>
		<category><![CDATA[science observations]]></category>
		<category><![CDATA[sofia]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[wavelength]]></category>
		<category><![CDATA[wavelength regime]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/first-science-observations-with-sofiaforcast-6-to-37-micron-imaging-of-orion-bnkl/</guid>
		<description><![CDATA[The BN/KL region of the Orion Nebula is the nearest region of high mass star formation in our galaxy. As such, it has been the subject of intense investigation at a variety of wavelengths, which have revealed it to be brightest in the infrared to sub-mm wavelength regime. Using the newly commissioned SOFIA airborne telescope [...]]]></description>
			<content:encoded><![CDATA[<p>The BN/KL region of the Orion Nebula is the nearest region of high mass star formation in our galaxy. As such, it has been the subject of intense investigation at a variety of wavelengths, which have revealed it to be brightest in the infrared to sub-mm wavelength regime. Using the newly commissioned SOFIA airborne telescope and its 5-40 micron camera FORCAST, images of the entire BN/KL complex have been acquired. The 31.5 and 37.1 micron images represent the highest resolution observations (31.5 microns, and that this distinction goes instead to the source IRc4. It was determined from these images and derived dust color temperature maps that IRc4 is also likely to be self-luminous. A new source of emission has also been identified at wavelengths &gt;31.5 microns that coincides with the northeastern outflow lobe from the protostellar disk associated with radio source I.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/first-science-observations-with-sofiaforcast-6-to-37-micron-imaging-of-orion-bnkl/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Characterizing the nature of Fossil Groups with XMM</title>
		<link>http://voxcharta.org/2012/02/22/characterizing-the-nature-of-fossil-groups-with-xmm/</link>
		<comments>http://voxcharta.org/2012/02/22/characterizing-the-nature-of-fossil-groups-with-xmm/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:54:41 +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[AGN]]></category>
		<category><![CDATA[Chandra]]></category>
		<category><![CDATA[cosmological simulations]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[ellipticals]]></category>
		<category><![CDATA[faint galaxy]]></category>
		<category><![CDATA[fgs]]></category>
		<category><![CDATA[fossil]]></category>
		<category><![CDATA[fossil group]]></category>
		<category><![CDATA[gap]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[rass data]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[ray sources]]></category>
		<category><![CDATA[sdss data]]></category>
		<category><![CDATA[similarity]]></category>
		<category><![CDATA[velocity distribution]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xmm]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/characterizing-the-nature-of-fossil-groups-with-xmm/</guid>
		<description><![CDATA[We present an X-ray follow-up, based on XMM plus Chandra, of six Fossil Group (FG) candidates identified in our previous work using SDSS and RASS data. Four candidates (out of six) exhibit extended X-ray emission, confirming them as true FGs. For the other two groups, the RASS emission has its origin as either an optically [...]]]></description>
			<content:encoded><![CDATA[<p>We present an X-ray follow-up, based on XMM plus Chandra, of six Fossil Group (FG) candidates identified in our previous work using SDSS and RASS data. Four candidates (out of six) exhibit extended X-ray emission, confirming them as true FGs. For the other two groups, the RASS emission has its origin as either an optically dull/X-ray bright AGN, or the blending of distinct X-ray sources. Using SDSS-DR7 data, we confirm, for all groups, the presence of an r-band magnitude gap between the seed elliptical and the second-rank galaxy. However, the gap value depends, up to 0.5mag, on how one estimates the seed galaxy total flux, which is greatly underestimated when using SDSS (relative to Sersic) magnitudes. This implies that many FGs may be actually missed when using SDSS data, a fact that should be carefully taken into account when comparing the observed number densities of FGs to the expectations from cosmological simulations. The similarity in the properties of seed&#8211;FG and non-fossil ellipticals, found in our previous study, extends to the sample of X-ray confirmed FGs, indicating that bright ellipticals in FGs do not represent a distinct population of galaxies. For one system, we also find that the velocity distribution of faint galaxies is bimodal, possibly showing that the system formed through the merging of two groups. This undermines the idea that all selected FGs form a population of true fossils.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/characterizing-the-nature-of-fossil-groups-with-xmm/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Crossing Statistic: Bayesian interpretation, model selection and resolving dark energy parametrization problem</title>
		<link>http://voxcharta.org/2012/02/22/crossing-statistic-bayesian-interpretation-model-selection-and-resolving-dark-energy-parametrization-problem/</link>
		<comments>http://voxcharta.org/2012/02/22/crossing-statistic-bayesian-interpretation-model-selection-and-resolving-dark-energy-parametrization-problem/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:54:26 +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[cosmological model]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[dispersion]]></category>
		<category><![CDATA[equation of state]]></category>
		<category><![CDATA[Hubble]]></category>
		<category><![CDATA[model of the universe]]></category>
		<category><![CDATA[model selection]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[priors]]></category>
		<category><![CDATA[quantities]]></category>
		<category><![CDATA[statistic]]></category>
		<category><![CDATA[uncertainty]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/crossing-statistic-bayesian-interpretation-model-selection-and-resolving-dark-energy-parametrization-problem/</guid>
		<description><![CDATA[By introducing Crossing functions and hyper-parameters I show that the Bayesian interpretation of the Crossing Statistics [1] can be used trivially for the purpose of model selection among cosmological models. In this approach to falsify a cosmological model there is no need to compare it with other models or assume any particular form of parametrization [...]]]></description>
			<content:encoded><![CDATA[<p>By introducing Crossing functions and hyper-parameters I show that the Bayesian interpretation of the Crossing Statistics [1] can be used trivially for the purpose of model selection among cosmological models. In this approach to falsify a cosmological model there is no need to compare it with other models or assume any particular form of parametrization for the cosmological quantities like luminosity distance, Hubble parameter or equation of state of dark energy. Instead, hyper-parameters of Crossing functions perform as discriminators between correct and wrong models. Using this approach one can falsify any assumed cosmological model without putting priors on the underlying actual model of the universe and its parameters, hence the issue of dark energy parametrization is resolved. It will be also shown that the sensitivity of the method to the intrinsic dispersion of the data is small that is another important characteristic of the method in testing cosmological models dealing with data with high uncertainties.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/crossing-statistic-bayesian-interpretation-model-selection-and-resolving-dark-energy-parametrization-problem/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Transition Radiation from the Neutrino-Photon Interaction in Matter [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/22/transition-radiation-from-the-neutrino-photon-interaction-in-matter-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/22/transition-radiation-from-the-neutrino-photon-interaction-in-matter-cross-listing/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:54:16 +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[dipole moment]]></category>
		<category><![CDATA[electromagnetic interaction]]></category>
		<category><![CDATA[indices of refraction]]></category>
		<category><![CDATA[phenomena]]></category>
		<category><![CDATA[photon interaction]]></category>
		<category><![CDATA[standard model]]></category>
		<category><![CDATA[transition radiation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/transition-radiation-from-the-neutrino-photon-interaction-in-matter-cross-listing/</guid>
		<description><![CDATA[We show that, because of their effective electromagnetic interaction in matter, transition radiation is emitted whenever neutrinos goes across the boundary between two media with different indices of refraction. This effect occurs in the context of the standard model and does not depend on any exotic neutrino property. We examine such a phenomena and compare [...]]]></description>
			<content:encoded><![CDATA[<p>We show that, because of their effective electromagnetic interaction in matter, transition radiation is emitted whenever neutrinos goes across the boundary between two media with different indices of refraction. This effect occurs in the context of the standard model and does not depend on any exotic neutrino property. We examine such a phenomena and compare it with the transition radiation of a neutrino endowed with an intrinsic dipole moment.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/transition-radiation-from-the-neutrino-photon-interaction-in-matter-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Proposed Quadruple System SZ Herculis: Revised LITE Model and Orbital Stability Study</title>
		<link>http://voxcharta.org/2012/02/22/the-proposed-quadruple-system-sz-herculis-revised-lite-model-and-orbital-stability-study/</link>
		<comments>http://voxcharta.org/2012/02/22/the-proposed-quadruple-system-sz-herculis-revised-lite-model-and-orbital-stability-study/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:54:02 +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[companion]]></category>
		<category><![CDATA[detached binary system]]></category>
		<category><![CDATA[dynamical instability]]></category>
		<category><![CDATA[eccentric orbit]]></category>
		<category><![CDATA[herculis]]></category>
		<category><![CDATA[light travel time]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[model parameter]]></category>
		<category><![CDATA[monte carlo approach]]></category>
		<category><![CDATA[orbital element]]></category>
		<category><![CDATA[orbital resonance]]></category>
		<category><![CDATA[orbital stability]]></category>
		<category><![CDATA[parameter space]]></category>
		<category><![CDATA[proposed system]]></category>
		<category><![CDATA[stability study]]></category>
		<category><![CDATA[time effect]]></category>
		<category><![CDATA[time model]]></category>
		<category><![CDATA[timing observations]]></category>
		<category><![CDATA[timing variations]]></category>
		<category><![CDATA[true nature]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/the-proposed-quadruple-system-sz-herculis-revised-lite-model-and-orbital-stability-study/</guid>
		<description><![CDATA[In a recent study, Lee et al. presented new photometric follow-up timing observations of the semi-detached binary system SZ Herculis and proposed the existence of two hierarchical cirumbinary companions. Based on the light-travel time effect, the two low-mass M-dwarf companions are found to orbit the binary pair on moderate to high eccentric orbits. The derived [...]]]></description>
			<content:encoded><![CDATA[<p>In a recent study, Lee et al. presented new photometric follow-up timing observations of the semi-detached binary system SZ Herculis and proposed the existence of two hierarchical cirumbinary companions. Based on the light-travel time effect, the two low-mass M-dwarf companions are found to orbit the binary pair on moderate to high eccentric orbits. The derived periods of these two companions are close to a 2:1 mean-motion orbital resonance. We have studied the stability of the system using the osculating orbital elements as presented by Lee et al. Results indicate an orbit-crossing architecture exhibiting short-term dynamical instabilities leading to the escape of one of the proposed companions. We have examined the system&#8217;s underlying model parameter-space by following a Monte Carlo approach and found an improved fit to the timing data. A study of the stability of our best-fitting orbits also indicates that the proposed system is generally unstable. If the observed anomalous timing variations of the binary period is due to additional circumbinary companions, then the resulting system should exhibit a long-term stable orbital configuration much different from the orbits suggested by Lee et al. We, therefore, suggest that based on Newtonian-dynamical considerations, the proposed quadruple system cannot exist. To uncover the true nature of the observed period variations of this system, we recommend future photometric follow-up observations that could further constrain eclipse-timing variations and/or refine light-travel time models.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/the-proposed-quadruple-system-sz-herculis-revised-lite-model-and-orbital-stability-study/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Origin of the EUV Late Phase: A Case Study of the C8.8 Flare on 2010 May 5</title>
		<link>http://voxcharta.org/2012/02/22/the-origin-of-the-euv-late-phase-a-case-study-of-the-c8-8-flare-on-2010-may-5/</link>
		<comments>http://voxcharta.org/2012/02/22/the-origin-of-the-euv-late-phase-a-case-study-of-the-c8-8-flare-on-2010-may-5/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:53:47 +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[case study]]></category>
		<category><![CDATA[coronal]]></category>
		<category><![CDATA[enhancement]]></category>
		<category><![CDATA[eve]]></category>
		<category><![CDATA[flare]]></category>
		<category><![CDATA[images]]></category>
		<category><![CDATA[launch]]></category>
		<category><![CDATA[nasa]]></category>
		<category><![CDATA[observatory]]></category>
		<category><![CDATA[physical model]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[secondary emission]]></category>
		<category><![CDATA[soft x]]></category>
		<category><![CDATA[subset]]></category>
		<category><![CDATA[thermal evolution]]></category>
		<category><![CDATA[variability]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/the-origin-of-the-euv-late-phase-a-case-study-of-the-c8-8-flare-on-2010-may-5/</guid>
		<description><![CDATA[Since the launch of NASA&#8217;s Solar Dynamics Observatory on 2010 February 11, the Extreme ultraviolet Variability Experiment (EVE) has observed numerous flares. One interesting feature observed by EVE is that a subset of flares exhibit an additional enhancement of the 2-3 million K emission several hours after the flare&#8217;s soft X-ray emission. From the Atmospheric [...]]]></description>
			<content:encoded><![CDATA[<p>Since the launch of NASA&#8217;s Solar Dynamics Observatory on 2010 February 11, the Extreme ultraviolet Variability Experiment (EVE) has observed numerous flares. One interesting feature observed by EVE is that a subset of flares exhibit an additional enhancement of the 2-3 million K emission several hours after the flare&#8217;s soft X-ray emission. From the Atmospheric Imaging Assembly (AIA) images, we observe that this secondary emission, dubbed the EUV late phase, occurs in the same active region as the flare but not in the same coronal loops. Here, we examine the C8.8 flare that occurred on 2010 May 5 as a case study of EUV late phase flares. In addition to presenting detailed observations from both AIA and EVE, we develop a physical model of this flare and test it using the Enthalpy Based Thermal Evolution of Loops (EBTEL) model.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/the-origin-of-the-euv-late-phase-a-case-study-of-the-c8-8-flare-on-2010-may-5/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Unusual Temporal and Spectral Evolution of the Type IIn Supernova 2011ht</title>
		<link>http://voxcharta.org/2012/02/22/the-unusual-temporal-and-spectral-evolution-of-the-type-iin-supernova-2011ht/</link>
		<comments>http://voxcharta.org/2012/02/22/the-unusual-temporal-and-spectral-evolution-of-the-type-iin-supernova-2011ht/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:53:09 +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[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absolute magnitude]]></category>
		<category><![CDATA[absorption line]]></category>
		<category><![CDATA[ergs]]></category>
		<category><![CDATA[impostor]]></category>
		<category><![CDATA[light curve]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[magnitude increase]]></category>
		<category><![CDATA[optical spectra]]></category>
		<category><![CDATA[peculiar type]]></category>
		<category><![CDATA[photometric]]></category>
		<category><![CDATA[ray observations]]></category>
		<category><![CDATA[siii]]></category>
		<category><![CDATA[spectral evolution]]></category>
		<category><![CDATA[spectroscopic observation]]></category>
		<category><![CDATA[type iin]]></category>
		<category><![CDATA[uv observations]]></category>
		<category><![CDATA[uv spectra]]></category>
		<category><![CDATA[v band]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/the-unusual-temporal-and-spectral-evolution-of-the-type-iin-supernova-2011ht/</guid>
		<description><![CDATA[We present very early UV to optical photometric and spectroscopic observations of the peculiar Type IIn supernova (SN) 2011ht in UGC 5460. The UV observations of the rise to peak are only the second ever recorded for a Type IIn SN and are by far the most complete. The SN, first classified as a SN [...]]]></description>
			<content:encoded><![CDATA[<p>We present very early UV to optical photometric and spectroscopic observations of the peculiar Type IIn supernova (SN) 2011ht in UGC 5460. The UV observations of the rise to peak are only the second ever recorded for a Type IIn SN and are by far the most complete. The SN, first classified as a SN impostor, slowly rose to a peak of M_V \sim -17 in \sim55 days. In contrast to the \sim2 magnitude increase in the v-band light curve from the first observation until peak, the UV flux increased by &gt;7 magnitudes. The optical spectra are dominated by strong, Balmer emission with narrow peaks (FWHM\sim600 km/s), very broad asymmetric wings (FWHM\sim4200 km/s), and blue shifted absorption (\sim300 km/s) superposed on a strong blue continuum. The UV spectra are dominated by FeII, MgII, SiII, and SiIII absorption lines broadened by \sim1500 km/s. Merged X-ray observations reveal a L_(0.2-10)=(1.0+/-0.2)x10^(39) erg/s. Some properties of SN 2011ht are similar to SN impostors, while others are comparable to Type IIn SNe. Early spectra showed features typical of luminous blue variables at maximum and during giant eruptions. However, the broad emission profiles coupled with the strong UV flux have not been observed in previous SN impostors. The absolute magnitude and energetics (~2.5&#215;10^(49) ergs in the first 112 days) are reminiscent of normal Type IIn SN, but the spectra are of a dense wind. We suggest that the mechanism for creating this unusual profile could be a shock interacting with a shell of material that was ejected a year before the discovery of the SN.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/the-unusual-temporal-and-spectral-evolution-of-the-type-iin-supernova-2011ht/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Absolute dimensions of solar-type eclipsing binaries. EF Aquarii: a G0 test for stellar evolution models</title>
		<link>http://voxcharta.org/2012/02/22/absolute-dimensions-of-solar-type-eclipsing-binaries-ef-aquarii-a-g0-test-for-stellar-evolution-models/</link>
		<comments>http://voxcharta.org/2012/02/22/absolute-dimensions-of-solar-type-eclipsing-binaries-ef-aquarii-a-g0-test-for-stellar-evolution-models/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:52:41 +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[aqr]]></category>
		<category><![CDATA[automatic telescope]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[energy transport]]></category>
		<category><![CDATA[evolutionary model]]></category>
		<category><![CDATA[formalism]]></category>
		<category><![CDATA[isochrone]]></category>
		<category><![CDATA[la palma]]></category>
		<category><![CDATA[length parameter]]></category>
		<category><![CDATA[magnetic activity]]></category>
		<category><![CDATA[metallicity]]></category>
		<category><![CDATA[photometry]]></category>
		<category><![CDATA[radial velocity]]></category>
		<category><![CDATA[radii]]></category>
		<category><![CDATA[star spot]]></category>
		<category><![CDATA[stellar evolution models]]></category>
		<category><![CDATA[theoretical evolution]]></category>
		<category><![CDATA[velocity curves]]></category>
		<category><![CDATA[victoria regina]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/absolute-dimensions-of-solar-type-eclipsing-binaries-ef-aquarii-a-g0-test-for-stellar-evolution-models/</guid>
		<description><![CDATA[Recent studies have shown that stellar chromospheric activity, and its effect on convective energy transport in the envelope, is most likely the cause of significant radius and temperature discrepancies between theoretical evolution models and observations. We aim to determine absolute dimensions and abundances for the solar-type detached eclipsing binary EF Aqr, and to perform a [...]]]></description>
			<content:encoded><![CDATA[<p>Recent studies have shown that stellar chromospheric activity, and its effect on convective energy transport in the envelope, is most likely the cause of significant radius and temperature discrepancies between theoretical evolution models and observations. We aim to determine absolute dimensions and abundances for the solar-type detached eclipsing binary EF Aqr, and to perform a detailed comparison with results from recent stellar evolutionary models. uvby-beta standard photometry was obtained with the Stromgren Automatic Telescope. The broadening function formalism was applied on spectra observed with HERMES at the Mercator telescope in La Palma, to obtain radial velocity curves. Masses and radii with a precision of 0.6% and 1.0% respectively have been established for both components of EF Aqr. The active 0.956 M_sol secondary shows star spots and strong Ca II H and K emission lines. The 1.224 M_sol primary shows signs of activity as well, but at a lower level. An [Fe/H] abundance of 0.00+-0.10 is derived with similar abundances for Si, Ca, Sc, Ti, V, Cr, Co, and Ni. Solar calibrated evolutionary models such as Yonsei-Yale, Victoria-Regina and BaSTI isochrones and evolutionary tracks are unable to reproduce EF Aqr, especially for the secondary, which is 9% larger and 400 K cooler than predicted. Models adopting significantly lower mixing length parameters l/H_p remove these discrepancies, as seen in other solar type binaries. For the observed metallicity, Granada models with a mixing length of l/H_p=1.30 (primary) and 1.05 (secondary) reproduce both components at a common age of 1.5+-0.6 Gyr. Observations of EF Aqr suggests that magnetic activity, and its effect on envelope convection, is likely to be the cause of discrepancies in both radius and temperature, which can be removed by adjusting the mixing length parameter of the models downwards.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/absolute-dimensions-of-solar-type-eclipsing-binaries-ef-aquarii-a-g0-test-for-stellar-evolution-models/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Effect of a Weak Electromagnetic Field on Particle Acceleration by a Rotating Black Hole [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/22/effect-of-a-weak-electromagnetic-field-on-particle-acceleration-by-a-rotating-black-hole-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/22/effect-of-a-weak-electromagnetic-field-on-particle-acceleration-by-a-rotating-black-hole-cross-listing/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:52:28 +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[capability]]></category>
		<category><![CDATA[center of mass]]></category>
		<category><![CDATA[circular orbit]]></category>
		<category><![CDATA[electromagnetic field]]></category>
		<category><![CDATA[finite energy]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[horizon]]></category>
		<category><![CDATA[isco]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[particle acceleration]]></category>
		<category><![CDATA[particle accelerator]]></category>
		<category><![CDATA[particle collision]]></category>
		<category><![CDATA[phys rev d]]></category>
		<category><![CDATA[plunge]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/effect-of-a-weak-electromagnetic-field-on-particle-acceleration-by-a-rotating-black-hole-cross-listing/</guid>
		<description><![CDATA[We study high energy charged particle collisions near the horizon in an electromagnetic field around a rotating black hole and reveal the condition of the fine-tuning to obtain arbitrarily large center-of-mass (CM) energy. We demonstrate that the CM energy can be arbitrarily large as the uniformly magnetized rotating black hole arbitrarily approaches maximal rotation under [...]]]></description>
			<content:encoded><![CDATA[<p>We study high energy charged particle collisions near the horizon in an electromagnetic field around a rotating black hole and reveal the condition of the fine-tuning to obtain arbitrarily large center-of-mass (CM) energy. We demonstrate that the CM energy can be arbitrarily large as the uniformly magnetized rotating black hole arbitrarily approaches maximal rotation under the situation that a charged particle plunges from the innermost stable circular orbit (ISCO) and collides with another particle near the horizon. Recently, Frolov [Phys. Rev. D 85, 024020 (2012)] proposed that the CM energy can be arbitrarily high if the magnetic field is arbitrarily strong, when a particle collides with a charged particle orbiting the ISCO with finite energy near the horizon of a uniformly magnetized Schwarzschild black hole. We show that the charged particle orbiting the ISCO around a spinning black hole needs arbitrarily high energy in the strong field limit. This suggests that Frolov&#8217;s process is unstable against the black hole spin. Nevertheless, we see that magnetic fields may substantially promote the capability of rotating black holes as particle accelerators in astrophysical situations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/effect-of-a-weak-electromagnetic-field-on-particle-acceleration-by-a-rotating-black-hole-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Pisa Stellar Evolution Data Base for low-mass stars</title>
		<link>http://voxcharta.org/2012/02/22/the-pisa-stellar-evolution-data-base-for-low-mass-stars/</link>
		<comments>http://voxcharta.org/2012/02/22/the-pisa-stellar-evolution-data-base-for-low-mass-stars/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:52:10 +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 model]]></category>
		<category><![CDATA[chemical composition]]></category>
		<category><![CDATA[chemical inputs]]></category>
		<category><![CDATA[evolutionary model]]></category>
		<category><![CDATA[galactic globular cluster]]></category>
		<category><![CDATA[gyr]]></category>
		<category><![CDATA[helium content]]></category>
		<category><![CDATA[initial mass]]></category>
		<category><![CDATA[isochrone]]></category>
		<category><![CDATA[msun]]></category>
		<category><![CDATA[nuclear reaction rates]]></category>
		<category><![CDATA[observational result]]></category>
		<category><![CDATA[opacity]]></category>
		<category><![CDATA[realistic atmosphere]]></category>
		<category><![CDATA[stellar cluster]]></category>
		<category><![CDATA[stellar evolution]]></category>
		<category><![CDATA[stellar model]]></category>
		<category><![CDATA[theoretical interpretation]]></category>
		<category><![CDATA[web model]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/the-pisa-stellar-evolution-data-base-for-low-mass-stars/</guid>
		<description><![CDATA[The last decade showed an impressive observational effort from the photometric and spectroscopic point of view for ancient stellar clusters in our Galaxy and beyond. The theoretical interpretation of these new observational results requires updated evolutionary models and isochrones spanning a wide range of chemical composition. With this aim we built the new &#8220;Pisa Stellar [...]]]></description>
			<content:encoded><![CDATA[<p>The last decade showed an impressive observational effort from the photometric and spectroscopic point of view for ancient stellar clusters in our Galaxy and beyond. The theoretical interpretation of these new observational results requires updated evolutionary models and isochrones spanning a wide range of chemical composition. With this aim we built the new &#8220;Pisa Stellar Evolution Database&#8221; of stellar models and isochrones by adopting a well-tested evolutionary code (FRANEC) implemented with updated physical and chemical inputs. In particular, our code adopts realistic atmosphere models and an updated equation of state, nuclear reaction rates and opacities calculated with recent solar elements mixture. A total of 32646 models have been computed in the range of initial masses 0.30 &#8211; 1.10 Msun for a grid of 216 chemical compositions with the fractional metal abundance in mass, Z, ranging from 0.0001 to 0.01, and the original helium content, Y, from 0.25 to 0.42. Models were computed for both solar-scaled and alpha-enhanced abundances with different external convection efficiencies. Correspondingly, 9720 isochrones were computed in the age range 8 &#8211; 15 Gyr, in time steps of 0.5 Gyr. The whole database is available to the scientific community on the web. Models and isochrones were compared with recent calculations available in the literature and with the color-magnitude diagram of selected Galactic globular clusters. The dependence of relevant evolutionary quantities on the chemical composition and convection efficiency were analyzed in a quantitative statistical way and analytical formulations were made available for reader&#8217;s convenience.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/the-pisa-stellar-evolution-data-base-for-low-mass-stars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Sympathetic Partial and Full Filament Eruptions Observed in One Solar Breakout Event</title>
		<link>http://voxcharta.org/2012/02/22/sympathetic-partial-and-full-filament-eruptions-observed-in-one-solar-breakout-event/</link>
		<comments>http://voxcharta.org/2012/02/22/sympathetic-partial-and-full-filament-eruptions-observed-in-one-solar-breakout-event/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:51:54 +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[antiparallel]]></category>
		<category><![CDATA[coronal mass ejection]]></category>
		<category><![CDATA[extrapolation]]></category>
		<category><![CDATA[filament]]></category>
		<category><![CDATA[implosion]]></category>
		<category><![CDATA[lateral lobes]]></category>
		<category><![CDATA[linkage]]></category>
		<category><![CDATA[low temperature]]></category>
		<category><![CDATA[mechanisms]]></category>
		<category><![CDATA[middle lobe]]></category>
		<category><![CDATA[null point]]></category>
		<category><![CDATA[reconnection]]></category>
		<category><![CDATA[rope]]></category>
		<category><![CDATA[solar eruption]]></category>
		<category><![CDATA[source region]]></category>
		<category><![CDATA[temperature lines]]></category>
		<category><![CDATA[topology]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/sympathetic-partial-and-full-filament-eruptions-observed-in-one-solar-breakout-event/</guid>
		<description><![CDATA[We report two sympathetic solar eruptions, including a partial and a full flux rope eruption in a quadrupolar magnetic region, where a large and a small filament resided above the middle and the east neutral lines respectively. The large filament first rose slowly at a speed of 8 km/s for 23 minutes and then it [...]]]></description>
			<content:encoded><![CDATA[<p>We report two sympathetic solar eruptions, including a partial and a full flux rope eruption in a quadrupolar magnetic region, where a large and a small filament resided above the middle and the east neutral lines respectively. The large filament first rose slowly at a speed of 8 km/s for 23 minutes and then it was accelerated to 102 km/s. Finally, this filament erupted successfully and caused a coronal mass ejection. During the slow rising phase, various evidence for breakout-like external reconnection has been identified at high and low temperature lines. The eruption of the small filament started around the end of the large filament&#8217;s slow rising. This filament erupted partially and no associating coronal mass ejection could be detected. Based on a potential field extrapolation, we find that the topology of the three-dimensional coronal field above the source region is composed of three low-lying lobes and a large overlying flux system, and a null point located between the middle lobe and the overlying antiparallel flux system. We propose a possible mechanism within the framework of the magnetic breakout model to interpret the sympathetic filament eruptions, in which the magnetic implosion mechanism is thought to be a possible linkage between the sympathetic eruptions, and the external reconnection at the null point transfers field lines from the middle lobe to the lateral lobes and thereby leads to the full (partial) eruption of the observed large (small) filament. Other possible mechanisms are also discussed briefly. We conclude that the structural properties of coronal fields are important for producing sympathetic eruptions.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/sympathetic-partial-and-full-filament-eruptions-observed-in-one-solar-breakout-event/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Evolutionary synthesis models as a tool and guide towards the first galaxies</title>
		<link>http://voxcharta.org/2012/02/22/evolutionary-synthesis-models-as-a-tool-and-guide-towards-the-first-galaxies/</link>
		<comments>http://voxcharta.org/2012/02/22/evolutionary-synthesis-models-as-a-tool-and-guide-towards-the-first-galaxies/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:51:11 +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[continuum emission]]></category>
		<category><![CDATA[dependence]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[evolutionary synthesis models]]></category>
		<category><![CDATA[fundamental tool]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[galaxy formation]]></category>
		<category><![CDATA[imf]]></category>
		<category><![CDATA[ism]]></category>
		<category><![CDATA[line strength]]></category>
		<category><![CDATA[nearby universe]]></category>
		<category><![CDATA[observational signature]]></category>
		<category><![CDATA[optical domain]]></category>
		<category><![CDATA[quantities]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[star formation history]]></category>
		<category><![CDATA[stellar atmosphere]]></category>
		<category><![CDATA[stellar evolution]]></category>
		<category><![CDATA[stellar population]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/evolutionary-synthesis-models-as-a-tool-and-guide-towards-the-first-galaxies/</guid>
		<description><![CDATA[We summarize the principles and fundamental ingredients of evolutionary synthesis models, which are stellar evolution, stellar atmospheres, the IMF, star-formation histories, nebular emission, and also attenuation from the ISM and IGM. The chapter focusses in particular on issues of importance for predictions of metal-poor and Population III dominated galaxies.   We review recent predictions [...]]]></description>
			<content:encoded><![CDATA[<p>We summarize the principles and fundamental ingredients of evolutionary synthesis models, which are stellar evolution, stellar atmospheres, the IMF, star-formation histories, nebular emission, and also attenuation from the ISM and IGM. The chapter focusses in particular on issues of importance for predictions of metal-poor and Population III dominated galaxies.   We review recent predictions for the main physical properties and related observables of star-forming galaxies based on up-to-date inputs. The predicted metallicity dependence of these quantities and their physical causes are discussed. The predicted observables include in particular the restframe UV-to-optical domain with continuum emission from stars and the ionized ISM, as well as emission lines from H, He, and metals.   Based on these predictions we summarize the main observational signatures (emission line strengths, colors etc.), which can be used to distinguish &#8220;normal&#8221; stellar populations from very metal-poor objects or even Pop III.   Evolutionary synthesis models provide an important and fundamental tool for studies of galaxy formation and evolution, from the nearby Universe back to first galaxies. They are used in many applications to interpret existing observations, to predict and guide future missions/instruments, and to allow direct comparisons between state-of-the-art galaxy simulations and observations.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Joint spectral-timing modelling of the hard lags in GX 339-4: constraints on reflection models</title>
		<link>http://voxcharta.org/2012/02/22/joint-spectral-timing-modelling-of-the-hard-lags-in-gx-339-4-constraints-on-reflection-models/</link>
		<comments>http://voxcharta.org/2012/02/22/joint-spectral-timing-modelling-of-the-hard-lags-in-gx-339-4-constraints-on-reflection-models/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:50:44 +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 disc]]></category>
		<category><![CDATA[alpha emission]]></category>
		<category><![CDATA[dependent response]]></category>
		<category><![CDATA[energy spectrum]]></category>
		<category><![CDATA[frequency dependence]]></category>
		<category><![CDATA[lags]]></category>
		<category><![CDATA[propagation effects]]></category>
		<category><![CDATA[radii]]></category>
		<category><![CDATA[ray binaries]]></category>
		<category><![CDATA[reflection model]]></category>
		<category><![CDATA[response function]]></category>
		<category><![CDATA[solid angle]]></category>
		<category><![CDATA[spectral data]]></category>
		<category><![CDATA[spectral variations]]></category>
		<category><![CDATA[time delay]]></category>
		<category><![CDATA[time lag]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xmm newton]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/joint-spectral-timing-modelling-of-the-hard-lags-in-gx-339-4-constraints-on-reflection-models/</guid>
		<description><![CDATA[The X-ray variations of hard state black hole X-ray binaries above 2 keV show &#8216;hard lags&#8217;, in that the variations at harder energies follow variations at softer energies, with a time-lag \tau depending on frequency \nu approximately as \tau \propto \nu^{-0.7}. Several models have so far been proposed to explain this time delay, including fluctuations [...]]]></description>
			<content:encoded><![CDATA[<p>The X-ray variations of hard state black hole X-ray binaries above 2 keV show &#8216;hard lags&#8217;, in that the variations at harder energies follow variations at softer energies, with a time-lag \tau depending on frequency \nu approximately as \tau \propto \nu^{-0.7}. Several models have so far been proposed to explain this time delay, including fluctuations propagating through an accretion flow, spectral variations during coronal flares, Comptonisation in the extended hot corona or a jet, or time-delays due to large-scale reflection from the accretion disc. In principle these models can be used to predict the shape of the energy spectrum as well as the frequency-dependence of the time-lags, through the construction of energy-dependent response functions which map the emission as a function of time-delay in the system. Here we use this approach to test a simple reflection model for the frequency-dependent lags seen in the hard state of GX 339-4, by simultaneously fitting the model to the frequency-dependent lags and energy spectrum measured by XMM-Newton in 2004 and 2009. Our model cannot simultaneously fit both the lag and spectral data, since the relatively large lags require an extremely flared disc which subtends a large solid angle to the continuum at large radii, in disagreement with the observed Fe K\alpha emission. Therefore, we consider it more likely that the lags &gt; 2 keV are caused by propagation effects in the accretion flow, possibly related to the accretion disc fluctuations which have been observed previously.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/joint-spectral-timing-modelling-of-the-hard-lags-in-gx-339-4-constraints-on-reflection-models/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Space Astronomy for the mid-21st Century: Robotically Maintained Space Telescopes</title>
		<link>http://voxcharta.org/2012/02/22/space-astronomy-for-the-mid-21st-century-robotically-maintained-space-telescopes/</link>
		<comments>http://voxcharta.org/2012/02/22/space-astronomy-for-the-mid-21st-century-robotically-maintained-space-telescopes/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:49:48 +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[21st century]]></category>
		<category><![CDATA[astronomical telescope]]></category>
		<category><![CDATA[autonomy]]></category>
		<category><![CDATA[capability]]></category>
		<category><![CDATA[decade]]></category>
		<category><![CDATA[lifetime]]></category>
		<category><![CDATA[mirror]]></category>
		<category><![CDATA[operational budget]]></category>
		<category><![CDATA[prerequisite]]></category>
		<category><![CDATA[robotic missions]]></category>
		<category><![CDATA[running costs]]></category>
		<category><![CDATA[scientific instrument]]></category>
		<category><![CDATA[space astronomy]]></category>
		<category><![CDATA[space telescope]]></category>
		<category><![CDATA[spacecraft components]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/space-astronomy-for-the-mid-21st-century-robotically-maintained-space-telescopes/</guid>
		<description><![CDATA[The historical development of ground based astronomical telescopes leads us to expect that space-based astronomical telescopes will need to be operational for many decades. The exchange of scientific instruments in space will be a prerequisite for the long lasting scientific success of such missions. Operationally, the possibility to repair or replace key spacecraft components in [...]]]></description>
			<content:encoded><![CDATA[<p>The historical development of ground based astronomical telescopes leads us to expect that space-based astronomical telescopes will need to be operational for many decades. The exchange of scientific instruments in space will be a prerequisite for the long lasting scientific success of such missions. Operationally, the possibility to repair or replace key spacecraft components in space will be mandatory. We argue that these requirements can be fulfilled with robotic missions and see the development of the required engineering as the main challenge. Ground based operations, scientifically and technically, will require a low operational budget of the running costs. These can be achieved through enhanced autonomy of the spacecraft and mission independent concepts for the support of the software. This concept can be applied to areas where the mirror capabilities do not constrain the lifetime of the mission.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/space-astronomy-for-the-mid-21st-century-robotically-maintained-space-telescopes/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Jovian Early Bombardment: planetesimal erosion in the inner asteroid belt</title>
		<link>http://voxcharta.org/2012/02/22/jovian-early-bombardment-planetesimal-erosion-in-the-inner-asteroid-belt/</link>
		<comments>http://voxcharta.org/2012/02/22/jovian-early-bombardment-planetesimal-erosion-in-the-inner-asteroid-belt/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:49:34 +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[asteroid belt]]></category>
		<category><![CDATA[asteroids]]></category>
		<category><![CDATA[bombardment]]></category>
		<category><![CDATA[collisional evolution]]></category>
		<category><![CDATA[disruption]]></category>
		<category><![CDATA[erosion]]></category>
		<category><![CDATA[frequency distribution]]></category>
		<category><![CDATA[giant planet]]></category>
		<category><![CDATA[history of the solar system]]></category>
		<category><![CDATA[initial size]]></category>
		<category><![CDATA[intense period]]></category>
		<category><![CDATA[jupiter]]></category>
		<category><![CDATA[physical characteristics]]></category>
		<category><![CDATA[planetesimal]]></category>
		<category><![CDATA[present day]]></category>
		<category><![CDATA[progenitor]]></category>
		<category><![CDATA[solar nebula]]></category>
		<category><![CDATA[threshold size]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/jovian-early-bombardment-planetesimal-erosion-in-the-inner-asteroid-belt/</guid>
		<description><![CDATA[The asteroid belt is an open window on the history of the Solar System, as it preserves records of both its formation process and its secular evolution. The progenitors of the present-day asteroids formed in the Solar Nebula almost contemporary to the giant planets. The actual process producing the first generation of asteroids is uncertain, [...]]]></description>
			<content:encoded><![CDATA[<p>The asteroid belt is an open window on the history of the Solar System, as it preserves records of both its formation process and its secular evolution. The progenitors of the present-day asteroids formed in the Solar Nebula almost contemporary to the giant planets. The actual process producing the first generation of asteroids is uncertain, strongly depending on the physical characteristics of the Solar Nebula, and the different scenarios produce very diverse initial size-frequency distributions. In this work we investigate the implications of the formation of Jupiter, plausibly the first giant planet to form, on the evolution of the primordial asteroid belt. The formation of Jupiter triggered a short but intense period of primordial bombardment, previously unaccounted for, which caused an early phase of enhanced collisional evolution in the asteroid belt. Our results indicate that this Jovian Early Bombardment caused the erosion or the disruption of bodies smaller than a threshold size, which strongly depends on the size-frequency distribution of the primordial planetesimals. If the asteroid belt was dominated by planetesimals less than 100 km in diameter, the primordial bombardment would have caused the erosion of bodies smaller than 200 km in diameter. If the asteroid belt was instead dominated by larger planetesimals, the bombardment would have resulted in the destruction of bodies as big as 500 km.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
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		<item>
		<title>Cosmological models with fluid matter undergoing velocity diffusion [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/22/cosmological-models-with-fluid-matter-undergoing-velocity-diffusion-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/22/cosmological-models-with-fluid-matter-undergoing-velocity-diffusion-cross-listing/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:49:20 +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[cosmological model]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[diffusion]]></category>
		<category><![CDATA[dynamical properties]]></category>
		<category><![CDATA[einstein equation]]></category>
		<category><![CDATA[fluid particles]]></category>
		<category><![CDATA[friction]]></category>
		<category><![CDATA[general relativity]]></category>
		<category><![CDATA[hypothesis]]></category>
		<category><![CDATA[left hand side]]></category>
		<category><![CDATA[scalar field]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/cosmological-models-with-fluid-matter-undergoing-velocity-diffusion-cross-listing/</guid>
		<description><![CDATA[A new type of fluid matter model in general relativity is introduced, in which the fluid particles are subject to velocity diffusion without friction. In order to compensate for the energy lost by the fluid particles due to diffusion, a cosmological scalar field term is added to the left hand side of the Einstein equations. [...]]]></description>
			<content:encoded><![CDATA[<p>A new type of fluid matter model in general relativity is introduced, in which the fluid particles are subject to velocity diffusion without friction. In order to compensate for the energy lost by the fluid particles due to diffusion, a cosmological scalar field term is added to the left hand side of the Einstein equations. This hypothesis promotes diffusion to a new mechanism for accelerated expansion in cosmology. It is shown that diffusion alters not only quantitatively, but also qualitatively the global dynamical properties of the standard cosmological models.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/cosmological-models-with-fluid-matter-undergoing-velocity-diffusion-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Non-Gaussian isocurvature perturbations in dark radiation</title>
		<link>http://voxcharta.org/2012/02/22/non-gaussian-isocurvature-perturbations-in-dark-radiation/</link>
		<comments>http://voxcharta.org/2012/02/22/non-gaussian-isocurvature-perturbations-in-dark-radiation/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:49:05 +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[asymmetry]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[curvature]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[expression]]></category>
		<category><![CDATA[fisher]]></category>
		<category><![CDATA[matrix analysis]]></category>
		<category><![CDATA[mixture]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[neutrino]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[particle physics]]></category>
		<category><![CDATA[perturbation]]></category>
		<category><![CDATA[radiation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/non-gaussian-isocurvature-perturbations-in-dark-radiation/</guid>
		<description><![CDATA[We study non-Gaussian properties of the isocurvature perturbations in the dark radiation, which consists of the active neutrinos and extra light species, if exist. We first derive expressions for the bispectra of primordial perturbations which are mixtures of curvature and dark radiation isocurvature perturbations. We also discuss CMB bispectra produced in our model and forecast [...]]]></description>
			<content:encoded><![CDATA[<p>We study non-Gaussian properties of the isocurvature perturbations in the dark radiation, which consists of the active neutrinos and extra light species, if exist. We first derive expressions for the bispectra of primordial perturbations which are mixtures of curvature and dark radiation isocurvature perturbations. We also discuss CMB bispectra produced in our model and forecast CMB constraints on the nonlinearity parameters based on the Fisher matrix analysis. Some concrete particle physics motivated models are presented in which large isocurvature perturbations in extra light species and/or the neutrino density isocurvature perturbations as well as their non-Gaussianities may be generated. Thus detections of non-Gaussianity in the dark radiation isocurvature perturbation will give us an opportunity to identify the origin of extra light species and lepton asymmetry.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/non-gaussian-isocurvature-perturbations-in-dark-radiation/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Black hole perturbation in the most general scalar-tensor theory with second-order field equations I: the odd-parity sector [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/22/black-hole-perturbation-in-the-most-general-scalar-tensor-theory-with-second-order-field-equations-i-the-odd-parity-sector-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/22/black-hole-perturbation-in-the-most-general-scalar-tensor-theory-with-second-order-field-equations-i-the-odd-parity-sector-cross-listing/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:48:42 +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[black hole]]></category>
		<category><![CDATA[brans]]></category>
		<category><![CDATA[degree of freedom]]></category>
		<category><![CDATA[dicke]]></category>
		<category><![CDATA[field equation]]></category>
		<category><![CDATA[general relativity]]></category>
		<category><![CDATA[ghost]]></category>
		<category><![CDATA[gradient]]></category>
		<category><![CDATA[gravity]]></category>
		<category><![CDATA[odd parity]]></category>
		<category><![CDATA[perturbation]]></category>
		<category><![CDATA[spherically symmetric solution]]></category>
		<category><![CDATA[theory models]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/black-hole-perturbation-in-the-most-general-scalar-tensor-theory-with-second-order-field-equations-i-the-odd-parity-sector-cross-listing/</guid>
		<description><![CDATA[We perform a fully relativistic analysis of odd-type linear perturbations around a static and spherically symmetric solution in the most general scalar-tensor theory with second-order field equations. It is shown that, as in the case of general relativity, the quadratic action for the perturbations reduces to the one having only a single dynamical variable, from [...]]]></description>
			<content:encoded><![CDATA[<p>We perform a fully relativistic analysis of odd-type linear perturbations around a static and spherically symmetric solution in the most general scalar-tensor theory with second-order field equations. It is shown that, as in the case of general relativity, the quadratic action for the perturbations reduces to the one having only a single dynamical variable, from which concise formulas for no-ghost and no-gradient instability conditions are derived. Our result is applicable to all the theories of gravity with an extra scalar degree of freedom. We demonstrate how the generic formulas can be applied to some particular examples such as the Brans-Dicke theory, $f(R)$ models, and Galileon gravity.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/black-hole-perturbation-in-the-most-general-scalar-tensor-theory-with-second-order-field-equations-i-the-odd-parity-sector-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Fast calculation of the Fisher matrix for Cosmic Microwave Background experiments</title>
		<link>http://voxcharta.org/2012/02/22/fast-calculation-of-the-fisher-matrix-for-cosmic-microwave-background-experiments/</link>
		<comments>http://voxcharta.org/2012/02/22/fast-calculation-of-the-fisher-matrix-for-cosmic-microwave-background-experiments/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:48:15 +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[approximation]]></category>
		<category><![CDATA[art surveys]]></category>
		<category><![CDATA[background experiments]]></category>
		<category><![CDATA[cmb data]]></category>
		<category><![CDATA[cmb experiments]]></category>
		<category><![CDATA[coefficients]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[cosmic microwave background]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[exact calculation]]></category>
		<category><![CDATA[fisher]]></category>
		<category><![CDATA[fundamental quantity]]></category>
		<category><![CDATA[information matrix]]></category>
		<category><![CDATA[max 3]]></category>
		<category><![CDATA[noise covariance]]></category>
		<category><![CDATA[optimal power]]></category>
		<category><![CDATA[power spectrum estimation]]></category>
		<category><![CDATA[radiation power]]></category>
		<category><![CDATA[sky coverage]]></category>
		<category><![CDATA[symmetry]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/fast-calculation-of-the-fisher-matrix-for-cosmic-microwave-background-experiments/</guid>
		<description><![CDATA[The Fisher information matrix of the cosmic microwave background (CMB) radiation power spectrum coefficients is a fundamental quantity that specifies the information content of a CMB experiment. In the most general case, its exact calculation scales with the third power of the number of data points N and is therefore computationally prohibitive for state-of-the-art surveys. [...]]]></description>
			<content:encoded><![CDATA[<p>The Fisher information matrix of the cosmic microwave background (CMB) radiation power spectrum coefficients is a fundamental quantity that specifies the information content of a CMB experiment. In the most general case, its exact calculation scales with the third power of the number of data points N and is therefore computationally prohibitive for state-of-the-art surveys. In this letter, we show how to compute the Fisher matrix in only O(N^2 log N) operations for a very large class of CMB experiments without special symmetries, as long as the inverse noise covariance matrix can be applied to a data vector in time O(l_max^3 log l_max}. This is true to a good approximation for all CMB data sets taken so far. The method takes into account common systematics such as arbitrary sky coverage and realistic noise correlations. As a consequence, optimal quadratic power spectrum estimation also becomes feasible in O(N^2 log N) operations for this large class of experiments. We discuss the relevance of our findings to other areas of cosmology where optimal power spectrum estimation plays a role.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/fast-calculation-of-the-fisher-matrix-for-cosmic-microwave-background-experiments/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Double Compact Objects I: The Significance Of The Common Envelope On Merger Rates</title>
		<link>http://voxcharta.org/2012/02/22/double-compact-objects-i-the-significance-of-the-common-envelope-on-merger-rates/</link>
		<comments>http://voxcharta.org/2012/02/22/double-compact-objects-i-the-significance-of-the-common-envelope-on-merger-rates/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:47:58 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[binary evolution]]></category>
		<category><![CDATA[binding energy]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[compact object]]></category>
		<category><![CDATA[dco]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[hole mass]]></category>
		<category><![CDATA[last decade]]></category>
		<category><![CDATA[mass distribution]]></category>
		<category><![CDATA[mass gap]]></category>
		<category><![CDATA[mass loss rates]]></category>
		<category><![CDATA[metallicity]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[orders of magnitude]]></category>
		<category><![CDATA[realistic treatment]]></category>
		<category><![CDATA[sensitivity curves]]></category>
		<category><![CDATA[signal waveforms]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[theoretical development]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/double-compact-objects-i-the-significance-of-the-common-envelope-on-merger-rates/</guid>
		<description><![CDATA[The development of gravitational wave observatories (Advanced LIGO/Virgo, Einstein Telescope) is proceeding apace, and the direct detection of gravitational waves should be imminent. The last decade of observational and theoretical developments in stellar and binary evolution provides us with improvements to the predictions from populations synthesis models. Among the most important revisions in the formation [...]]]></description>
			<content:encoded><![CDATA[<p>The development of gravitational wave observatories (Advanced LIGO/Virgo, Einstein Telescope) is proceeding apace, and the direct detection of gravitational waves should be imminent. The last decade of observational and theoretical developments in stellar and binary evolution provides us with improvements to the predictions from populations synthesis models. Among the most important revisions in the formation and evolution of double compact objects are: updated wind mass loss rates (allowing for stellar mass black holes up to 80 Msun), a realistic treatment of the common envelope phase (that can affect merger rates by 2&#8211;3 orders of magnitude), and a qualitatively new neutron star/black hole mass distribution (consistent with the observed &#8220;mass gap&#8221;). We present a parameter study with these major physical updates included, focusing on the most important factors that set the DCO merger rates. A few of our more interesting findings are: the binding energy of the envelope and our description of natal kicks from supernovae play an important role in determining the formation and merger rate of DCOs. Also, models incorporating delayed (SASI) supernovae do not agree with the observed NS/BH &#8220;mass gap&#8221;, in accordance with our previous work. And, finally, we find enhanced rates for BH-BH mergers as compared to previous estimates, with an expectation of ~100 such mergers per year in Advanced LIGO/Virgo detectors (although this rate is sensitive to factors, such as the natal kick distribution). This is the first in a series of three papers. The second paper will study the merger rates of double compact objects as a function of cosmological redshift, star formation rate, and metallicity. In the third paper we will present the detection rates for future gravitational wave observatories, using up-to-date signal waveforms and sensitivity curves. (abridged)</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/double-compact-objects-i-the-significance-of-the-common-envelope-on-merger-rates/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>True CMB Power Spectrum Estimation</title>
		<link>http://voxcharta.org/2012/02/22/true-cmb-power-spectrum-estimation/</link>
		<comments>http://voxcharta.org/2012/02/22/true-cmb-power-spectrum-estimation/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:47:45 +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 power spectrum]]></category>
		<category><![CDATA[cmb power spectrum]]></category>
		<category><![CDATA[coefficients]]></category>
		<category><![CDATA[cosmic microwave background]]></category>
		<category><![CDATA[cosmological parameters]]></category>
		<category><![CDATA[dct]]></category>
		<category><![CDATA[dictionary]]></category>
		<category><![CDATA[map]]></category>
		<category><![CDATA[monte carlo simulation]]></category>
		<category><![CDATA[perturbation]]></category>
		<category><![CDATA[power spectra]]></category>
		<category><![CDATA[power spectrum estimation]]></category>
		<category><![CDATA[realization]]></category>
		<category><![CDATA[sky]]></category>
		<category><![CDATA[sparsity]]></category>
		<category><![CDATA[statistical information]]></category>
		<category><![CDATA[theoretical power]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/true-cmb-power-spectrum-estimation/</guid>
		<description><![CDATA[The cosmic microwave background (CMB) power spectrum is a powerful cosmological probe as it entails almost all the statistical information of the CMB perturbations. Having access to only one sky, the CMB power spectrum measured by our experiments is only a realization of the true underlying angular power spectrum. In this paper we aim to [...]]]></description>
			<content:encoded><![CDATA[<p>The cosmic microwave background (CMB) power spectrum is a powerful cosmological probe as it entails almost all the statistical information of the CMB perturbations. Having access to only one sky, the CMB power spectrum measured by our experiments is only a realization of the true underlying angular power spectrum. In this paper we aim to recover the true underlying CMB power spectrum from the one realization that we have without a need to know the cosmological parameters. The sparsity of the CMB power spectrum is first investigated in two dictionaries; Discrete Cosine Transform (DCT) and Wavelet Transform (WT). The CMB power spectrum can be recovered with only a few percentage of the coefficients in both of these dictionaries and hence is very compressible in these dictionaries. We study the performance of these dictionaries in smoothing a set of simulated power spectra. Based on this, we develop a technique that estimates the true underlying CMB power spectrum from data, i.e. without a need to know the cosmological parameters. This smooth estimated spectrum can be used to simulate CMB maps with similar properties to the true CMB simulations with the correct cosmological parameters. This allows us to make Monte Carlo simulations in a given project, without having to know the cosmological parameters. The developed IDL code, TOUSI, for Theoretical pOwer spectrUm using Sparse estImation, will be released with the next version of ISAP.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/true-cmb-power-spectrum-estimation/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The fight for accretion: discovery of intermittent mass transfer in BB Doradus in the low state</title>
		<link>http://voxcharta.org/2012/02/22/the-fight-for-accretion-discovery-of-intermittent-mass-transfer-in-bb-doradus-in-the-low-state/</link>
		<comments>http://voxcharta.org/2012/02/22/the-fight-for-accretion-discovery-of-intermittent-mass-transfer-in-bb-doradus-in-the-low-state/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:47:24 +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[accretion disc]]></category>
		<category><![CDATA[alpha emission]]></category>
		<category><![CDATA[balmer series]]></category>
		<category><![CDATA[cataclysmic variables]]></category>
		<category><![CDATA[doradus]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[line profile]]></category>
		<category><![CDATA[mass transfer]]></category>
		<category><![CDATA[optical spectroscopy]]></category>
		<category><![CDATA[optical spectrum]]></category>
		<category><![CDATA[orbital period]]></category>
		<category><![CDATA[outer edge]]></category>
		<category><![CDATA[quiescence]]></category>
		<category><![CDATA[radial velocity]]></category>
		<category><![CDATA[remnant]]></category>
		<category><![CDATA[secondary star]]></category>
		<category><![CDATA[teff]]></category>
		<category><![CDATA[timescale]]></category>
		<category><![CDATA[velocity curve]]></category>
		<category><![CDATA[white dwarf]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/the-fight-for-accretion-discovery-of-intermittent-mass-transfer-in-bb-doradus-in-the-low-state/</guid>
		<description><![CDATA[Our long-term photometric monitoring of southern nova-like cataclysmic variables with the 1.3-m SMARTS telescope found BB Doradus fading from V ~ 14.3 towards a deep low state at V ~ 19.3 in April 2008. Here we present time-resolved optical spectroscopy of BB Dor in this faint state in 2009. The optical spectrum in quiescence is [...]]]></description>
			<content:encoded><![CDATA[<p>Our long-term photometric monitoring of southern nova-like cataclysmic variables with the 1.3-m SMARTS telescope found BB Doradus fading from V ~ 14.3 towards a deep low state at V ~ 19.3 in April 2008. Here we present time-resolved optical spectroscopy of BB Dor in this faint state in 2009. The optical spectrum in quiescence is a composite of a hot white dwarf with Teff = 30000 +- 5000 K and a M3-4 secondary star with narrow emission lines (mainly of the Balmer series and HeI) superposed. We associate these narrow profiles with an origin on the donor star. Analysis of the radial velocity curve of the H-alpha emission from the donor star allowed the measurement of an orbital period of 0.154095 +- 0.000003 d (3.69828 +- 0.00007 h), different from all previous estimates. We detected episodic accretion events which veiled the spectra of both stars and radically changed the line profiles within a timescale of tens of minutes. This shows that accretion is not completely quenched in the low state. During these accretion episodes the line wings are stronger and their radial velocity curve is delayed by ~ 0.2 cycle, similar to that observed in SW Sex and AM Her stars in the high state, with respect to the motion of the white dwarf. Two scenarios are proposed to explain the extra emission: impact of the material on the outer edge of a cold, remnant accretion disc, or the combined action of a moderately magnetic white dwarf (B1 &lt;~ 5 MG) and the magnetic activity of the donor star.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/the-fight-for-accretion-discovery-of-intermittent-mass-transfer-in-bb-doradus-in-the-low-state/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Multimodality in galaxy clusters from SDSS DR8: substructure and velocity distribution</title>
		<link>http://voxcharta.org/2012/02/22/multimodality-in-galaxy-clusters-from-sdss-dr8-substructure-and-velocity-distribution/</link>
		<comments>http://voxcharta.org/2012/02/22/multimodality-in-galaxy-clusters-from-sdss-dr8-substructure-and-velocity-distribution/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:47:10 +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[3d 2d]]></category>
		<category><![CDATA[cluster galaxy]]></category>
		<category><![CDATA[delimited]]></category>
		<category><![CDATA[dressler]]></category>
		<category><![CDATA[ds test]]></category>
		<category><![CDATA[galaxy cluster]]></category>
		<category><![CDATA[median value]]></category>
		<category><![CDATA[member galaxies]]></category>
		<category><![CDATA[multimodality]]></category>
		<category><![CDATA[peculiar velocity]]></category>
		<category><![CDATA[physical parameter]]></category>
		<category><![CDATA[principal component analysis]]></category>
		<category><![CDATA[rms]]></category>
		<category><![CDATA[rms velocity]]></category>
		<category><![CDATA[sdss]]></category>
		<category><![CDATA[shapiro wilk]]></category>
		<category><![CDATA[sky distribution]]></category>
		<category><![CDATA[substructure]]></category>
		<category><![CDATA[velocity distribution]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/multimodality-in-galaxy-clusters-from-sdss-dr8-substructure-and-velocity-distribution/</guid>
		<description><![CDATA[We search for the presence of substructure, a non-Gaussian, asymmetrical velocity distribution of galaxies, and large peculiar velocities of the main galaxies in galaxy clusters with at least 50 member galaxies, drawn from the SDSS DR8. We employ a number of 3D, 2D, and 1D tests to analyse the distribution of galaxies in clusters: 3D [...]]]></description>
			<content:encoded><![CDATA[<p>We search for the presence of substructure, a non-Gaussian, asymmetrical velocity distribution of galaxies, and large peculiar velocities of the main galaxies in galaxy clusters with at least 50 member galaxies, drawn from the SDSS DR8. We employ a number of 3D, 2D, and 1D tests to analyse the distribution of galaxies in clusters: 3D normal mixture modelling, the Dressler-Shectman test, the Anderson-Darling and Shapiro-Wilk tests and others. We find the peculiar velocities of the main galaxies, and use principal component analysis to characterise our results. More than 80% of the clusters in our sample have substructure according to 3D normal mixture modelling, the Dressler-Shectman (DS) test shows substructure in about 70% of the clusters. The median value of the peculiar velocities of the main galaxies in clusters is 206 km/s (41% of the rms velocity). The velocities of galaxies in more than 20% of the clusters show significant non-Gaussianity. While multidimensional normal mixture modelling is more sensitive than the DS test in resolving substructure in the sky distribution of cluster galaxies, the DS test determines better substructure expressed as tails in the velocity distribution of galaxies. Richer, larger, and more luminous clusters have larger amount of substructure and larger (compared to the rms velocity) peculiar velocities of the main galaxies. Principal component analysis of both the substructure indicators and the physical parameters of clusters shows that galaxy clusters are complicated objects, the properties of which cannot be explained with a small number of parameters or delimited by one single test. The presence of substructure, the non-Gaussian velocity distributions, as well as the large peculiar velocities of the main galaxies, shows that most of the clusters in our sample are dynamically young.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/multimodality-in-galaxy-clusters-from-sdss-dr8-substructure-and-velocity-distribution/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A Note on the Variability of V538 Cassiopeiae</title>
		<link>http://voxcharta.org/2012/02/22/a-note-on-the-variability-of-v538-cassiopeiae/</link>
		<comments>http://voxcharta.org/2012/02/22/a-note-on-the-variability-of-v538-cassiopeiae/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:47:00 +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[bright star]]></category>
		<category><![CDATA[ccd observations]]></category>
		<category><![CDATA[variability]]></category>
		<category><![CDATA[variation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/a-note-on-the-variability-of-v538-cassiopeiae/</guid>
		<description><![CDATA[CCD observations of V538 Cas have been made on nine nights during three weeks using the AAVSO Bright Star Monitor. No significant variations were found.
]]></description>
			<content:encoded><![CDATA[<p>CCD observations of V538 Cas have been made on nine nights during three weeks using the AAVSO Bright Star Monitor. No significant variations were found.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/a-note-on-the-variability-of-v538-cassiopeiae/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Sun in Hidden Photons [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/22/the-sun-in-hidden-photons-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/22/the-sun-in-hidden-photons-cross-listing/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:45:32 +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[cosmic microwave background]]></category>
		<category><![CDATA[estimates]]></category>
		<category><![CDATA[large scale]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[photon]]></category>
		<category><![CDATA[photosphere]]></category>
		<category><![CDATA[probes]]></category>
		<category><![CDATA[scale structure]]></category>
		<category><![CDATA[scenarios]]></category>
		<category><![CDATA[string theory]]></category>
		<category><![CDATA[Sun]]></category>
		<category><![CDATA[Telescope]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/the-sun-in-hidden-photons-cross-listing/</guid>
		<description><![CDATA[We present some aspects and first results of the emission of sub-eV mass hidden photons from the Sun. The contribution from a resonant region below the photosphere can be quite significant, raising previous estimates. This is relevant for the Telescope for Hidden Photon Search, TSHIPS I, currently targeting at meV-mass hidden photons with O(10^-6) kinetic [...]]]></description>
			<content:encoded><![CDATA[<p>We present some aspects and first results of the emission of sub-eV mass hidden photons from the Sun. The contribution from a resonant region below the photosphere can be quite significant, raising previous estimates. This is relevant for the Telescope for Hidden Photon Search, TSHIPS I, currently targeting at meV-mass hidden photons with O(10^-6) kinetic mixing with the photon. These particles could account for the large effective number of neutrinos pointed at by the cosmic microwave background and other large-scale structure probes, and are motivated in some scenarios of string theory.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/the-sun-in-hidden-photons-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Abundances of PNe in the Outer Disk of M31</title>
		<link>http://voxcharta.org/2012/02/22/abundances-of-pne-in-the-outer-disk-of-m31/</link>
		<comments>http://voxcharta.org/2012/02/22/abundances-of-pne-in-the-outer-disk-of-m31/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:44:54 +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[assumption]]></category>
		<category><![CDATA[central star]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[determinations]]></category>
		<category><![CDATA[estimates]]></category>
		<category><![CDATA[gradient]]></category>
		<category><![CDATA[luminosity function]]></category>
		<category><![CDATA[m31]]></category>
		<category><![CDATA[Measurement]]></category>
		<category><![CDATA[milky way galaxy]]></category>
		<category><![CDATA[oxygen abundance]]></category>
		<category><![CDATA[photoionization model]]></category>
		<category><![CDATA[planetary nebula]]></category>
		<category><![CDATA[pne]]></category>
		<category><![CDATA[spectroscopic observation]]></category>
		<category><![CDATA[star properties]]></category>
		<category><![CDATA[Sun]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/abundances-of-pne-in-the-outer-disk-of-m31/</guid>
		<description><![CDATA[We present spectroscopic observations and chemical abundances of 16 planetary nebulae (PNe) in the outer disk of M31. The [O III] 4363 line is detected in all objects, allowing a direct measurement of the nebular temperature essential for accurate abundance determinations. Our results show that the abundances in these M31 PNe display the same correlations [...]]]></description>
			<content:encoded><![CDATA[<p>We present spectroscopic observations and chemical abundances of 16 planetary nebulae (PNe) in the outer disk of M31. The [O III] 4363 line is detected in all objects, allowing a direct measurement of the nebular temperature essential for accurate abundance determinations. Our results show that the abundances in these M31 PNe display the same correlations and general behaviors as Type II PNe in the Milky Way Galaxy. We also calculate photoionization models to derive estimates of central star properties. From these we infer that our sample PNe, all near the peak of the Planetary Nebula Luminosity Function, originated from stars near 2 M_sun. Finally, under the assumption that these PNe are located in M31&#8217;s disk, we plot the oxygen abundance gradient, which appears shallower than the gradient in the Milky Way.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/abundances-of-pne-in-the-outer-disk-of-m31/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Rip/singularity free cosmology models with bulk viscosity</title>
		<link>http://voxcharta.org/2012/02/22/ripsingularity-free-cosmology-models-with-bulk-viscosity/</link>
		<comments>http://voxcharta.org/2012/02/22/ripsingularity-free-cosmology-models-with-bulk-viscosity/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:44:40 +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[concrete model]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[curves]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[dataset]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[exact solution]]></category>
		<category><![CDATA[fate of universe]]></category>
		<category><![CDATA[first model]]></category>
		<category><![CDATA[Hubble]]></category>
		<category><![CDATA[lambda cdm]]></category>
		<category><![CDATA[observational data]]></category>
		<category><![CDATA[phenomena]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[pseudo]]></category>
		<category><![CDATA[realistic universe]]></category>
		<category><![CDATA[singularity]]></category>
		<category><![CDATA[viscosity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/ripsingularity-free-cosmology-models-with-bulk-viscosity/</guid>
		<description><![CDATA[In this paper we present two concrete models of non-perfect fluid with bulk viscosity to interpret the observed cosmic accelerating expansion phenomena, avoiding the introduction of exotic dark energy. The first model we inspect has a viscosity of the form ${\zeta} = {\zeta}_0 + ({\zeta}_1-{\zeta}_2q)H$ by taking into account of the decelerating parameter q, and [...]]]></description>
			<content:encoded><![CDATA[<p>In this paper we present two concrete models of non-perfect fluid with bulk viscosity to interpret the observed cosmic accelerating expansion phenomena, avoiding the introduction of exotic dark energy. The first model we inspect has a viscosity of the form ${\zeta} = {\zeta}_0 + ({\zeta}_1-{\zeta}_2q)H$ by taking into account of the decelerating parameter q, and the other model is of the form ${\zeta} = {\zeta}_0 + {\zeta}_1H + {\zeta}_2H^2$. We give out the exact solutions of such models and further constrain them with the latest Union2 data as well as the currently observed Hubble-parameter dataset (OHD), then we discuss the fate of universe evolution in these models, which confronts neither future singularity nor little/pseudo rip. From the resulting curves by best fittings we find a much more flexible evolution processing due to the presence of viscosity while being consistent with the observational data in the region of data fitting. With the bulk viscosity considered, a more realistic universe scenario is characterized comparable with the {\Lambda}CDM model but without introducing the mysterious dark energy.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/ripsingularity-free-cosmology-models-with-bulk-viscosity/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>On the formation of glycolaldehyde in dense molecular cores</title>
		<link>http://voxcharta.org/2012/02/22/on-the-formation-of-glycolaldehyde-in-dense-molecular-cores/</link>
		<comments>http://voxcharta.org/2012/02/22/on-the-formation-of-glycolaldehyde-in-dense-molecular-cores/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:44:27 +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[abundance]]></category>
		<category><![CDATA[core]]></category>
		<category><![CDATA[core conditions]]></category>
		<category><![CDATA[dense core]]></category>
		<category><![CDATA[estimates]]></category>
		<category><![CDATA[feasibility]]></category>
		<category><![CDATA[gas phase]]></category>
		<category><![CDATA[grain surface]]></category>
		<category><![CDATA[hco]]></category>
		<category><![CDATA[literature]]></category>
		<category><![CDATA[molecular core]]></category>
		<category><![CDATA[monosaccharide sugar]]></category>
		<category><![CDATA[perspective]]></category>
		<category><![CDATA[phase formation]]></category>
		<category><![CDATA[reaction chemistry]]></category>
		<category><![CDATA[reaction mechanisms]]></category>
		<category><![CDATA[temperature]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/on-the-formation-of-glycolaldehyde-in-dense-molecular-cores/</guid>
		<description><![CDATA[Glycolaldehyde is a simple monosaccharide sugar linked to prebiotic chemistry. Recently it was detected in a molecular core in the star-forming region G31.41+0.31 at a reasonably high abundance. We investigate the formation of glycolaldehyde at 10K to determine whether it can form efficiently under typical dense core conditions. Using an astrochemical model, we test five [...]]]></description>
			<content:encoded><![CDATA[<p>Glycolaldehyde is a simple monosaccharide sugar linked to prebiotic chemistry. Recently it was detected in a molecular core in the star-forming region G31.41+0.31 at a reasonably high abundance. We investigate the formation of glycolaldehyde at 10K to determine whether it can form efficiently under typical dense core conditions. Using an astrochemical model, we test five different reaction mechanisms that have been proposed in the astrophysical literature, finding that a gas-phase formation route is unlikely. Of the grain-surface formation routes, only two are efficient enough at very low temperatures to produce sufficient glycolaldehyde to match the observational estimates, with the mechanism culminating in CH3OH + HCO being favoured. However, when we consider the feasibility of these mechanisms from a reaction chemistry perspective, the second grain-surface route looks more promising, H3CO + HCO.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/on-the-formation-of-glycolaldehyde-in-dense-molecular-cores/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The rotation of field stars from CoRoT data</title>
		<link>http://voxcharta.org/2012/02/22/the-rotation-of-field-stars-from-corot-data/</link>
		<comments>http://voxcharta.org/2012/02/22/the-rotation-of-field-stars-from-corot-data/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:44:11 +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[age distribution]]></category>
		<category><![CDATA[binary system]]></category>
		<category><![CDATA[field star]]></category>
		<category><![CDATA[instrumental artifacts]]></category>
		<category><![CDATA[light curve]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[main sequence]]></category>
		<category><![CDATA[myr]]></category>
		<category><![CDATA[orbital period]]></category>
		<category><![CDATA[period measurement]]></category>
		<category><![CDATA[pulsation]]></category>
		<category><![CDATA[rotation period]]></category>
		<category><![CDATA[rotational period]]></category>
		<category><![CDATA[selection biases]]></category>
		<category><![CDATA[solar neighborhood]]></category>
		<category><![CDATA[solar neighbourhood]]></category>
		<category><![CDATA[spectroscopic observation]]></category>
		<category><![CDATA[star formation history]]></category>
		<category><![CDATA[two different directions]]></category>
		<category><![CDATA[young stars]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/the-rotation-of-field-stars-from-corot-data/</guid>
		<description><![CDATA[We present period measurements of a large sample of field stars in the solar neighbourhood, observed by CoRoT in two different directions of the Galaxy. The presence of a period was detected using the Scargle Lomb Normalized Periodogram technique and the autocorrelation analysis. The assessment of the results has been performed through a consistency verification [...]]]></description>
			<content:encoded><![CDATA[<p>We present period measurements of a large sample of field stars in the solar neighbourhood, observed by CoRoT in two different directions of the Galaxy. The presence of a period was detected using the Scargle Lomb Normalized Periodogram technique and the autocorrelation analysis. The assessment of the results has been performed through a consistency verification supported by the folded light curve analysis. The data analysis procedure has discarded a non-negligible fraction of light curves due to instrumental artifacts, however it has allowed us to identify pulsators and binaries among a large number of field stars. We measure a wide range of periods, from 0.25 to 100 days, most of which are rotation periods. The final catalogue includes 1978 periods, with 1727 of them identified as rotational periods, 169 are classified as pulsations and 82 as orbital periods of binary systems. Our sample suffers from selection biases not easily corrected for, thus we do not use the distribution of rotation periods to derive the age distribution of the main-sequence population. Nevertheless, using rotation as a proxy for age, we can identify a sample of young stars (&lt; 600 Myr), that will constitute a valuable sample, supported by further spectroscopic observations, to study the recent star formation history in the solar neighborhood.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/the-rotation-of-field-stars-from-corot-data/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Very Low-Mass Stellar and Substellar Companions to Solar-Like Stars from MARVELS I: A Low Mass Ratio Stellar Companion to TYC 4110-01037-1 in a 79-day Orbit</title>
		<link>http://voxcharta.org/2012/02/22/very-low-mass-stellar-and-substellar-companions-to-solar-like-stars-from-marvels-i-a-low-mass-ratio-stellar-companion-to-tyc-4110-01037-1-in-a-79-day-orbit/</link>
		<comments>http://voxcharta.org/2012/02/22/very-low-mass-stellar-and-substellar-companions-to-solar-like-stars-from-marvels-i-a-low-mass-ratio-stellar-companion-to-tyc-4110-01037-1-in-a-79-day-orbit/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:43:56 +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[binary system]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[marvels]]></category>
		<category><![CDATA[mass ratio]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[orbital period]]></category>
		<category><![CDATA[stellar companion]]></category>
		<category><![CDATA[substellar companion]]></category>
		<category><![CDATA[teff]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/very-low-mass-stellar-and-substellar-companions-to-solar-like-stars-from-marvels-i-a-low-mass-ratio-stellar-companion-to-tyc-4110-01037-1-in-a-79-day-orbit/</guid>
		<description><![CDATA[TYC 4110-01037-1 has a low-mass stellar companion, whose small mass ratio and short orbital period are atypical amongst solar-like (Teff ~&#60; 6000 K) binary systems. Our analysis of TYC 4110-01037-1 reveals it to be a moderately aged (~0.087 +/- 0.003, places it at the lowest end of observed values for short period stellar companions to [...]]]></description>
			<content:encoded><![CDATA[<p>TYC 4110-01037-1 has a low-mass stellar companion, whose small mass ratio and short orbital period are atypical amongst solar-like (Teff ~&lt; 6000 K) binary systems. Our analysis of TYC 4110-01037-1 reveals it to be a moderately aged (~0.087 +/- 0.003, places it at the lowest end of observed values for short period stellar companions to solar-like (Teff ~&lt; 6000 K) stars. One possible way to create such a system would be if a triple-component stellar multiple broke up into a short period, low q binary during the cluster dispersal phase of its lifetime. A candidate tertiary body has been identified in the system via single-epoch, high contrast imagery. If this object is confirmed to be co-moving, we estimate it would be a dM4 star. We present these results in the context of our larger-scale effort to constrain the statistics of low mass stellar and brown dwarf companions to FGK-type stars via the MARVELS survey.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/very-low-mass-stellar-and-substellar-companions-to-solar-like-stars-from-marvels-i-a-low-mass-ratio-stellar-companion-to-tyc-4110-01037-1-in-a-79-day-orbit/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Discovery of the neutron star spin and orbital period from the Be/X-ray binary IGR J05414-6858 in the LMC</title>
		<link>http://voxcharta.org/2012/02/22/discovery-of-the-neutron-star-spin-and-orbital-period-from-the-bex-ray-binary-igr-j05414-6858-in-the-lmc/</link>
		<comments>http://voxcharta.org/2012/02/22/discovery-of-the-neutron-star-spin-and-orbital-period-from-the-bex-ray-binary-igr-j05414-6858-in-the-lmc/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:43:43 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[archival data]]></category>
		<category><![CDATA[discovery of the neutron]]></category>
		<category><![CDATA[epic pn]]></category>
		<category><![CDATA[faint object spectrograph]]></category>
		<category><![CDATA[large magellanic cloud]]></category>
		<category><![CDATA[light curve]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[mjd]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[optical counterpart]]></category>
		<category><![CDATA[orbital period]]></category>
		<category><![CDATA[outburst]]></category>
		<category><![CDATA[photometry]]></category>
		<category><![CDATA[photon index]]></category>
		<category><![CDATA[ray binaries]]></category>
		<category><![CDATA[small magellanic cloud]]></category>
		<category><![CDATA[swift satellite]]></category>
		<category><![CDATA[target]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xmm newton]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/discovery-of-the-neutron-star-spin-and-orbital-period-from-the-bex-ray-binary-igr-j05414-6858-in-the-lmc/</guid>
		<description><![CDATA[The number of known Be/X-ray binaries in the Large Magellanic Cloud is small compared to the observed population of the Galaxy or the Small Magellanic Cloud. The discovery of a system in outburst provides the rare opportunity to measure its X-ray properties in detail. IGR J05414-6858 was serendipitously found in outburst with the Swift satellite [...]]]></description>
			<content:encoded><![CDATA[<p>The number of known Be/X-ray binaries in the Large Magellanic Cloud is small compared to the observed population of the Galaxy or the Small Magellanic Cloud. The discovery of a system in outburst provides the rare opportunity to measure its X-ray properties in detail. IGR J05414-6858 was serendipitously found in outburst with the Swift satellite in August 2011. In order to characterise the system, we analysed the data from a follow-up XMM-Newton target of opportunity observation and investigate the stellar counterpart with photometry and spectroscopy. We modelled the X-ray spectra from the EPIC instruments on XMM-Newton and compared them with Swift archival data. In the X-ray and optical light curves, we searched for periodicities and variability. The optical counterpart was classified using spectroscopy obtained with ESO&#8217;s Faint Object Spectrograph at NTT. The X-ray spectra as seen in 2011 are relatively hard with a photon index of ~0.3 &#8211; 0.4 and show only low absorption. They deviate significantly from earlier spectra of a probable type II outburst in 2010. The neutron star spin period of P_s = 4.4208 s was discovered with EPIC-pn. The I-band light curve revealed a transition from a low to a high state around MJD 54500. The optical counterpart is classified to B0-1IIIe and shows Halpha emission and a variable NIR excess, vanishing during the 2010 outburst. In the optical high state, we found a periodicity at 19.9 days, probably caused by binarity and indicating the orbital period.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/discovery-of-the-neutron-star-spin-and-orbital-period-from-the-bex-ray-binary-igr-j05414-6858-in-the-lmc/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Cosmic Acceleration from Warped Space-time in Brane-world Scenario</title>
		<link>http://voxcharta.org/2012/02/22/cosmic-acceleration-from-warped-space-time-in-brane-world-scenario/</link>
		<comments>http://voxcharta.org/2012/02/22/cosmic-acceleration-from-warped-space-time-in-brane-world-scenario/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:43:06 +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[acceleration]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[friedmann]]></category>
		<category><![CDATA[frw]]></category>
		<category><![CDATA[plays two]]></category>
		<category><![CDATA[space time]]></category>
		<category><![CDATA[universe]]></category>
		<category><![CDATA[variation]]></category>
		<category><![CDATA[warp factor]]></category>
		<category><![CDATA[warped space]]></category>
		<category><![CDATA[world scenario]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/cosmic-acceleration-from-warped-space-time-in-brane-world-scenario/</guid>
		<description><![CDATA[In this work the role of extra dimensions in the accelerated universe through the scenario of higher-dimensional Friedmann-Robertson-Walker (FRW) cosmology has been studied. For this purpose, we first consider warped space-time in the standard flat brane scenario as the modified form of Robertson-Walker (RW) metric in five-dimension (5D) space-time and then the variation of the [...]]]></description>
			<content:encoded><![CDATA[<p>In this work the role of extra dimensions in the accelerated universe through the scenario of higher-dimensional Friedmann-Robertson-Walker (FRW) cosmology has been studied. For this purpose, we first consider warped space-time in the standard flat brane scenario as the modified form of Robertson-Walker (RW) metric in five-dimension (5D) space-time and then the variation of the bulk scale factor (warp factor), with respect to both space-like and time-like extra dimensions is obtained. Finally, it is shown that both of two types of extra dimensions are important in this scenario and also the bulk scale factor plays two different roles.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/cosmic-acceleration-from-warped-space-time-in-brane-world-scenario/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Break up of returning plasma after the 7 June 2011 filament eruption by Rayleigh-Taylor instabilities</title>
		<link>http://voxcharta.org/2012/02/22/break-up-of-returning-plasma-after-the-7-june-2011-filament-eruption-by-rayleigh-taylor-instabilities/</link>
		<comments>http://voxcharta.org/2012/02/22/break-up-of-returning-plasma-after-the-7-june-2011-filament-eruption-by-rayleigh-taylor-instabilities/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:41:34 +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[aia]]></category>
		<category><![CDATA[aim]]></category>
		<category><![CDATA[appearance]]></category>
		<category><![CDATA[corona]]></category>
		<category><![CDATA[coronal]]></category>
		<category><![CDATA[curtain]]></category>
		<category><![CDATA[dense plasma]]></category>
		<category><![CDATA[extreme ultraviolet]]></category>
		<category><![CDATA[filament eruption]]></category>
		<category><![CDATA[horns]]></category>
		<category><![CDATA[images]]></category>
		<category><![CDATA[instances]]></category>
		<category><![CDATA[prominence]]></category>
		<category><![CDATA[rayleigh]]></category>
		<category><![CDATA[solar surface]]></category>
		<category><![CDATA[taylor fingers]]></category>
		<category><![CDATA[taylor instability]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/break-up-of-returning-plasma-after-the-7-june-2011-filament-eruption-by-rayleigh-taylor-instabilities/</guid>
		<description><![CDATA[A prominence eruption on 7 June 2011 produced spectacular curtains of plasma falling through the lower corona. At the solar surface they created an incredible display of extreme ultraviolet brightenings. The aim is to identify and analyze some of the local instabilities which produce structure in the falling plasma. The structures were investigated using SDO/AIA [...]]]></description>
			<content:encoded><![CDATA[<p>A prominence eruption on 7 June 2011 produced spectacular curtains of plasma falling through the lower corona. At the solar surface they created an incredible display of extreme ultraviolet brightenings. The aim is to identify and analyze some of the local instabilities which produce structure in the falling plasma. The structures were investigated using SDO/AIA 171A and 193A images in which the falling plasma appeared dark against the bright coronal emission. Several instances of the Rayleigh-Taylor instability were investigated. In two cases the Alfven velocity associated with the dense plasma could be estimated from the separation of the Rayleigh-Taylor fingers. A second type of feature, which has the appearance of self-similar branching horns, is also discussed.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/break-up-of-returning-plasma-after-the-7-june-2011-filament-eruption-by-rayleigh-taylor-instabilities/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Shower Center of Gravity and Hadronic Interaction Characteristics</title>
		<link>http://voxcharta.org/2012/02/22/shower-center-of-gravity-and-hadronic-interaction-characteristics/</link>
		<comments>http://voxcharta.org/2012/02/22/shower-center-of-gravity-and-hadronic-interaction-characteristics/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:41:22 +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[center of gravity]]></category>
		<category><![CDATA[energy proton]]></category>
		<category><![CDATA[expression]]></category>
		<category><![CDATA[hadron]]></category>
		<category><![CDATA[hadronic]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[interaction]]></category>
		<category><![CDATA[shower development]]></category>
		<category><![CDATA[transparent view]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/shower-center-of-gravity-and-hadronic-interaction-characteristics/</guid>
		<description><![CDATA[Equations for the center of gravity of the shower originated by high energy proton in the atmosphere are written and, within certain simplifications, solved for the case of logarithmically decreasing interaction length of hadrons in the air. Obtained expression provides transparent view of the way in which hadronic interaction characteristics determine the longitudinal shower development.
]]></description>
			<content:encoded><![CDATA[<p>Equations for the center of gravity of the shower originated by high energy proton in the atmosphere are written and, within certain simplifications, solved for the case of logarithmically decreasing interaction length of hadrons in the air. Obtained expression provides transparent view of the way in which hadronic interaction characteristics determine the longitudinal shower development.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/shower-center-of-gravity-and-hadronic-interaction-characteristics/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Intermediate Old Star Clusters in a Young Starburst: The case of NGC 5253</title>
		<link>http://voxcharta.org/2012/02/22/intermediate-old-star-clusters-in-a-young-starburst-the-case-of-ngc-5253/</link>
		<comments>http://voxcharta.org/2012/02/22/intermediate-old-star-clusters-in-a-young-starburst-the-case-of-ngc-5253/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:41:07 +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[advanced camera]]></category>
		<category><![CDATA[archive images]]></category>
		<category><![CDATA[cluster candidates]]></category>
		<category><![CDATA[cluster population]]></category>
		<category><![CDATA[dwarf galaxy]]></category>
		<category><![CDATA[galaxy ngc]]></category>
		<category><![CDATA[global star formation]]></category>
		<category><![CDATA[hubble space telescope]]></category>
		<category><![CDATA[old star]]></category>
		<category><![CDATA[star burst]]></category>
		<category><![CDATA[star cluster]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[starburst galaxy]]></category>
		<category><![CDATA[survey]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/intermediate-old-star-clusters-in-a-young-starburst-the-case-of-ngc-5253/</guid>
		<description><![CDATA[We investigate the star cluster population in the outer parts of the starburst galaxy NGC 5253 using archive images taken with the Hubble Space Telescope&#8217;s Advanced Camera for Surveys. Based on the F415W, F555W, and F814W photometry ages and masses are estimated for bona-fide star cluster candidates. We find three potentially massive ($\ge 10 \time [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate the star cluster population in the outer parts of the starburst galaxy NGC 5253 using archive images taken with the Hubble Space Telescope&#8217;s Advanced Camera for Surveys. Based on the F415W, F555W, and F814W photometry ages and masses are estimated for bona-fide star cluster candidates. We find three potentially massive ($\ge 10 \time 10^5$ \Msun) star clusters at ages of order of 1-2 Gyr, implying, if confirmed, a high global star formation rate in NGC 5253 during that epoch. This result underlines earlier findings that the current star burst is just one episode in an very active dwarf galaxy.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/intermediate-old-star-clusters-in-a-young-starburst-the-case-of-ngc-5253/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>The Gas Properties of the W3 GMC: A HARP study</title>
		<link>http://voxcharta.org/2012/02/22/the-gas-properties-of-the-w3-gmc-a-harp-study/</link>
		<comments>http://voxcharta.org/2012/02/22/the-gas-properties-of-the-w3-gmc-a-harp-study/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:40:05 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accurate determination]]></category>
		<category><![CDATA[cfe]]></category>
		<category><![CDATA[clump]]></category>
		<category><![CDATA[continuum]]></category>
		<category><![CDATA[dense clump]]></category>
		<category><![CDATA[dense structure]]></category>
		<category><![CDATA[feedback effect]]></category>
		<category><![CDATA[gas temperature]]></category>
		<category><![CDATA[harp]]></category>
		<category><![CDATA[hdl]]></category>
		<category><![CDATA[high density]]></category>
		<category><![CDATA[james clerk maxwell]]></category>
		<category><![CDATA[low density]]></category>
		<category><![CDATA[mach number]]></category>
		<category><![CDATA[mass distribution]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[radio astronomy observatory]]></category>
		<category><![CDATA[solar mass]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[temperature gradient]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/the-gas-properties-of-the-w3-gmc-a-harp-study/</guid>
		<description><![CDATA[We present 12CO, 13CO and C18O J=3-2 maps of the W3 GMC made at the James Clerk Maxwell Telescope. We combine these observations with Five Colleges Radio Astronomy Observatory CO J=1-0 data to produce the first map of molecular-gas temperatures across a GMC and the most accurate determination of the mass distribution in W3 yet [...]]]></description>
			<content:encoded><![CDATA[<p>We present 12CO, 13CO and C18O J=3-2 maps of the W3 GMC made at the James Clerk Maxwell Telescope. We combine these observations with Five Colleges Radio Astronomy Observatory CO J=1-0 data to produce the first map of molecular-gas temperatures across a GMC and the most accurate determination of the mass distribution in W3 yet obtained. We measure excitation temperatures in the part of the cloud dominated by triggered star formation (the High Density Layer, HDL) of 15-30 K, while in the rest of the cloud, which is relatively unaffected by triggering (Low Density Layer, LDL), the excitation temperature is generally less than 12 K. We identify a temperature gradient in the HDL which we associate with an age sequence in the embedded massive star-forming regions. We measure the mass of the cloud to be 4.4+/-0.4 x 10^5 solar masses, in agreement with previous estimates. Existing sub-mm continuum data are used to derive the fraction of gas mass in dense clumps as a function of position in the cloud. This fraction, which we interpret as a Clump Formation Efficiency (CFE), is significantly enhanced across the HDL, probably due to the triggering. Finally, we measure the 3D rms Mach Number as a function of position and find a correlation between the Mach number and the CFE within the HDL only. This correlation is interpreted as due to feedback from the newly-formed stars and a change in its slope between the three main star-forming regions is construed as another evolutionary effect. We conclude that triggering has affected the star-formation process in the W3 GMC primarily by creating additional dense structures that can collapse into stars. Any traces of changes in CFE due to additional turbulence have since been overruled by the feedback effects of the star-forming process itself.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/the-gas-properties-of-the-w3-gmc-a-harp-study/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>First Science Observations with SOFIA/FORCAST: The FORCAST Mid-infrared Camera</title>
		<link>http://voxcharta.org/2012/02/22/first-science-observations-with-sofiaforcast-the-forcast-mid-infrared-camera/</link>
		<comments>http://voxcharta.org/2012/02/22/first-science-observations-with-sofiaforcast-the-forcast-mid-infrared-camera/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:39:50 +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[capability]]></category>
		<category><![CDATA[diffraction]]></category>
		<category><![CDATA[first science]]></category>
		<category><![CDATA[images]]></category>
		<category><![CDATA[infrared astronomy]]></category>
		<category><![CDATA[infrared camera]]></category>
		<category><![CDATA[infrared instrument]]></category>
		<category><![CDATA[Lambda]]></category>
		<category><![CDATA[light flight]]></category>
		<category><![CDATA[micron]]></category>
		<category><![CDATA[science flights]]></category>
		<category><![CDATA[science observations]]></category>
		<category><![CDATA[science results]]></category>
		<category><![CDATA[sofia]]></category>
		<category><![CDATA[stratospheric observatory]]></category>
		<category><![CDATA[unique science]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/first-science-observations-with-sofiaforcast-the-forcast-mid-infrared-camera/</guid>
		<description><![CDATA[The Stratospheric Observatory for Infrared Astronomy (SOFIA) completed its first light flight in May of 2010 using the facility mid-infrared instrument FORCAST. Since then, FORCAST has successfully completed thirteen science flights on SOFIA. In this paper we describe the design, operation and performance of FORCAST as it relates to the initial three Short Science flights. [...]]]></description>
			<content:encoded><![CDATA[<p>The Stratospheric Observatory for Infrared Astronomy (SOFIA) completed its first light flight in May of 2010 using the facility mid-infrared instrument FORCAST. Since then, FORCAST has successfully completed thirteen science flights on SOFIA. In this paper we describe the design, operation and performance of FORCAST as it relates to the initial three Short Science flights. FORCAST was able to achieve near diffraction-limited images for lambda &gt; 30 microns allowing unique science results from the start with SOFIA. We also describe ongoing and future modifications that will improve overall capabilities and performance of FORCAST.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/first-science-observations-with-sofiaforcast-the-forcast-mid-infrared-camera/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A two-component jet model based on the Blandford-Znajek and Blandford-Payne processes</title>
		<link>http://voxcharta.org/2012/02/22/a-two-component-jet-model-based-on-the-blandford-znajek-and-blandford-payne-processes/</link>
		<comments>http://voxcharta.org/2012/02/22/a-two-component-jet-model-based-on-the-blandford-znajek-and-blandford-payne-processes/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:39:19 +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 disk]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[agns]]></category>
		<category><![CDATA[baryon]]></category>
		<category><![CDATA[blandford]]></category>
		<category><![CDATA[cen]]></category>
		<category><![CDATA[electromagnetic energy]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[inner edge]]></category>
		<category><![CDATA[jet model]]></category>
		<category><![CDATA[kinetic energy]]></category>
		<category><![CDATA[lorentz]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[mkn]]></category>
		<category><![CDATA[outflow]]></category>
		<category><![CDATA[physical parameter]]></category>
		<category><![CDATA[sheath]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/a-two-component-jet-model-based-on-the-blandford-znajek-and-blandford-payne-processes/</guid>
		<description><![CDATA[We propose a two-component jet model consistent with the observations of several gamma ray bursts (GRBs) and active galactic nuclei (AGNs). The jet consists of inner and outer components, and they are supposed to be driven by the Blandford-Znajek (BZ) and Blandford-Payne (BP) processes, respectively. The baryons in the BP jet is accelerated centrifugally via [...]]]></description>
			<content:encoded><![CDATA[<p>We propose a two-component jet model consistent with the observations of several gamma ray bursts (GRBs) and active galactic nuclei (AGNs). The jet consists of inner and outer components, and they are supposed to be driven by the Blandford-Znajek (BZ) and Blandford-Payne (BP) processes, respectively. The baryons in the BP jet is accelerated centrifugally via the magnetic field anchored in the accretion disk. The BZ jet is assumed to be entrained a fraction of accreting matter leaving the inner edge of the accretion disk, and the baryons are accelerated in the conversion from electromagnetic energy to the kinetic energy. By fitting the Lorentz factors of some GRBs (GRB 030329, GRB 051221A, GRB 080413B) and AGNs (Cen A, Mkn 501 and Mkn 421) with this model, we constrain the physical parameters related to the accretion and outflow of these two kind of objects. We conclude that the spine/sheath structure of the jet from these sources can be interpreted naturally by the BZ and BP processes.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/a-two-component-jet-model-based-on-the-blandford-znajek-and-blandford-payne-processes/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Negative effective magnetic pressure in turbulent convection [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/negative-effective-magnetic-pressure-in-turbulent-convection-replacement/</link>
		<comments>http://voxcharta.org/2012/02/22/negative-effective-magnetic-pressure-in-turbulent-convection-replacement/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:39:07 +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[anisotropy]]></category>
		<category><![CDATA[equation of state]]></category>
		<category><![CDATA[evolution equation]]></category>
		<category><![CDATA[isothermal layer]]></category>
		<category><![CDATA[large scale]]></category>
		<category><![CDATA[lorentz force]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetic pressure]]></category>
		<category><![CDATA[magnetic structure]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[turbulence effects]]></category>
		<category><![CDATA[turbulent convection]]></category>
		<category><![CDATA[vertical direction]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/negative-effective-magnetic-pressure-in-turbulent-convection-replacement/</guid>
		<description><![CDATA[We investigate the effects of weakly and strongly stratified turbulent convection on the mean effective Lorentz force, and especially on the mean effective magnetic pressure. Earlier studies with isotropically forced non-stratified and stratified turbulence have shown that the contribution of the turbulence to the mean magnetic pressure is negative for mean horizontal magnetic fields that [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate the effects of weakly and strongly stratified turbulent convection on the mean effective Lorentz force, and especially on the mean effective magnetic pressure. Earlier studies with isotropically forced non-stratified and stratified turbulence have shown that the contribution of the turbulence to the mean magnetic pressure is negative for mean horizontal magnetic fields that are smaller than the equipartition strength, so that the effective mean magnetic pressure that takes into account the turbulence effects, can be negative. Compared with earlier cases of forced turbulence with an isothermal equation of state, we find that the turbulence effect is similar to or even stronger in the present case of turbulent convection. This is argued to be due to the anisotropy of turbulence in the vertical direction. Another important difference compared with earlier studies is the presence of an evolution equation for the specific entropy. Mean-field modelling with entropy evolution indicates that the negative effective magnetic pressure can still lead to a large-scale instability which forms local flux concentrations, even though the specific entropy evolution tends to have a stabilizing effect when applied to a stably stratified (e.g., isothermal) layer. It is argued that this large-scale instability could be important for the formation of solar large-scale magnetic structures such as active regions.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/negative-effective-magnetic-pressure-in-turbulent-convection-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Spindown of Isolated Neutron Stars: Gravitational Waves or Magnetic Braking? [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/spindown-of-isolated-neutron-stars-gravitational-waves-or-magnetic-braking-replacement/</link>
		<comments>http://voxcharta.org/2012/02/22/spindown-of-isolated-neutron-stars-gravitational-waves-or-magnetic-braking-replacement/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:38:53 +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[evolution]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[modes]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[rapid rotation]]></category>
		<category><![CDATA[rotation rate]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/spindown-of-isolated-neutron-stars-gravitational-waves-or-magnetic-braking-replacement/</guid>
		<description><![CDATA[We study the spindown of isolated neutron stars from initially rapid rotation rates, driven by two factors: (i) gravitational wave emission due to r-modes and (ii) magnetic braking. In the context of isolated neutron stars, we present the first study including self-consistently the magnetic damping of r-modes in the spin evolution. We track the spin [...]]]></description>
			<content:encoded><![CDATA[<p>We study the spindown of isolated neutron stars from initially rapid rotation rates, driven by two factors: (i) gravitational wave emission due to r-modes and (ii) magnetic braking. In the context of isolated neutron stars, we present the first study including self-consistently the magnetic damping of r-modes in the spin evolution. We track the spin evolution employing the RNS code, which accounts for the rotating structure of neutron stars for various equations of state. We find that, despite the strong damping due to the magnetic field, r-modes alter the braking rate from pure magnetic braking for B&lt;10^{13}G. For realistic values of the saturation amplitude, the r-mode can also decrease the time to reach the threshold central density for quark deconfinement. Within a phenomenological model, we assess the gravitational waveform that would result from r-mode driven spindown of a magnetized neutron star. To contrast with the persistent signal during the spindown phase, we also present a preliminary estimate of the transient gravitational wave signal from an explosive quark-hadron phase transition, which can be a signal for the deconfinement of quarks inside neutron stars.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/spindown-of-isolated-neutron-stars-gravitational-waves-or-magnetic-braking-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Bayesian analysis of the astrobiological implications of life&#8217;s early emergence on Earth [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/bayesian-analysis-of-the-astrobiological-implications-of-lifes-early-emergence-on-earth-replacement/</link>
		<comments>http://voxcharta.org/2012/02/22/bayesian-analysis-of-the-astrobiological-implications-of-lifes-early-emergence-on-earth-replacement/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:38:36 +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[abiogenesis]]></category>
		<category><![CDATA[billions of years]]></category>
		<category><![CDATA[curious creatures]]></category>
		<category><![CDATA[dominant influence]]></category>
		<category><![CDATA[early earth]]></category>
		<category><![CDATA[earth life]]></category>
		<category><![CDATA[emergence of life]]></category>
		<category><![CDATA[extrasolar planet]]></category>
		<category><![CDATA[hundred million]]></category>
		<category><![CDATA[life on earth]]></category>
		<category><![CDATA[lineage]]></category>
		<category><![CDATA[million years]]></category>
		<category><![CDATA[organism]]></category>
		<category><![CDATA[posterior probability]]></category>
		<category><![CDATA[priors]]></category>
		<category><![CDATA[solar system]]></category>
		<category><![CDATA[statistical framework]]></category>
		<category><![CDATA[terrestrial life]]></category>
		<category><![CDATA[young earth]]></category>
		<category><![CDATA[young planet]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/bayesian-analysis-of-the-astrobiological-implications-of-lifes-early-emergence-on-earth-replacement/</guid>
		<description><![CDATA[Life arose on Earth sometime in the first few hundred million years after the young planet had cooled to the point that it could support water-based organisms on its surface. The early emergence of life on Earth has been taken as evidence that the probability of abiogenesis is high, if starting from young-Earth-like conditions. We [...]]]></description>
			<content:encoded><![CDATA[<p>Life arose on Earth sometime in the first few hundred million years after the young planet had cooled to the point that it could support water-based organisms on its surface. The early emergence of life on Earth has been taken as evidence that the probability of abiogenesis is high, if starting from young-Earth-like conditions. We revisit this argument quantitatively in a Bayesian statistical framework. By constructing a simple model of the probability of abiogenesis, we calculate a Bayesian estimate of its posterior probability, given the data that life emerged fairly early in Earth&#8217;s history and that, billions of years later, curious creatures noted this fact and considered its implications. We find that, given only this very limited empirical information, the choice of Bayesian prior for the abiogenesis probability parameter has a dominant influence on the computed posterior probability. Although terrestrial life&#8217;s early emergence provides evidence that life might be common in the Universe if early-Earth-like conditions are, the evidence is inconclusive and indeed is consistent with an arbitrarily low intrinsic probability of abiogenesis for plausible uninformative priors. Finding a single case of life arising independently of our lineage (on Earth, elsewhere in the Solar System, or on an extrasolar planet) would provide much stronger evidence that abiogenesis is not extremely rare in the Universe.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/bayesian-analysis-of-the-astrobiological-implications-of-lifes-early-emergence-on-earth-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Mean-field transport in stratified and/or rotating turbulence [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/mean-field-transport-in-stratified-andor-rotating-turbulence-replacement/</link>
		<comments>http://voxcharta.org/2012/02/22/mean-field-transport-in-stratified-andor-rotating-turbulence-replacement/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:38:24 +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[anisotropy]]></category>
		<category><![CDATA[convection]]></category>
		<category><![CDATA[density stratification]]></category>
		<category><![CDATA[diffusivity]]></category>
		<category><![CDATA[electromotive force]]></category>
		<category><![CDATA[fluid velocity]]></category>
		<category><![CDATA[gradient]]></category>
		<category><![CDATA[intermediate length]]></category>
		<category><![CDATA[isothermal layer]]></category>
		<category><![CDATA[length scales]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[rapid rotation]]></category>
		<category><![CDATA[rotation axis]]></category>
		<category><![CDATA[scalar flux]]></category>
		<category><![CDATA[scalar transport]]></category>
		<category><![CDATA[test field]]></category>
		<category><![CDATA[transport coefficients]]></category>
		<category><![CDATA[Turbulence]]></category>
		<category><![CDATA[turbulent diffusion]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/mean-field-transport-in-stratified-andor-rotating-turbulence-replacement/</guid>
		<description><![CDATA[We investigate the mean electromotive force in the kinematic framework, that is, ignoring the back-reaction of the magnetic field on the fluid velocity, under the assumption of axisymmetric turbulence determined by the presence of either rotation, density stratification, or both. We use an analogous approach for the mean passive scalar flux. As an alternative to [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate the mean electromotive force in the kinematic framework, that is, ignoring the back-reaction of the magnetic field on the fluid velocity, under the assumption of axisymmetric turbulence determined by the presence of either rotation, density stratification, or both. We use an analogous approach for the mean passive scalar flux. As an alternative to convection, we consider forced turbulence in an isothermal layer. When using standard ansatzes, the mean magnetic transport is then determined by nine, and the mean passive scalar transport by four coefficients. We give results for all these transport coefficients. We use the test-field method and the test-scalar method, where transport coefficients are determined by solving sets of equations with properly chosen mean magnetic fields or mean scalars. These methods are adapted to mean fields which may depend on all three space coordinates. We find the anisotropy of turbulent diffusion to be moderate in spite of rapid rotation or strong density stratification. Contributions to the mean electromotive force determined by the symmetric part of the gradient tensor of the mean magnetic field, which were ignored in several earlier investigations, turn out to be important. In stratified rotating turbulence, the $\alpha$ effect is strongly anisotropic, suppressed along the rotation axis on large length scales, but strongly enhanced at intermediate length scales. Also the $\OO\times\meanJJ$ effect is enhanced at intermediate length scales. The turbulent passive scalar diffusivity is typically almost twice as large as the turbulent magnetic diffusivity. Both magnetic and passive scalar diffusion are slightly enhanced along the rotation axis, but decreased if there is gravity.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/mean-field-transport-in-stratified-andor-rotating-turbulence-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A remarkably high fraction of strong Ly_alpha emitters amongst luminous redshift 6.0&lt;z&lt;6.5 Lyman break galaxies in the UKIDSS Ultra-Deep Survey [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/a-remarkably-high-fraction-of-strong-ly_alpha-emitters-amongst-luminous-redshift-6-0z6-5-lyman-break-galaxies-in-the-ukidss-ultra-deep-survey-replacement/</link>
		<comments>http://voxcharta.org/2012/02/22/a-remarkably-high-fraction-of-strong-ly_alpha-emitters-amongst-luminous-redshift-6-0z6-5-lyman-break-galaxies-in-the-ukidss-ultra-deep-survey-replacement/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:38:12 +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[alpha emitter]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[redshift]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/a-remarkably-high-fraction-of-strong-ly_alpha-emitters-amongst-luminous-redshift-6-0z6-5-lyman-break-galaxies-in-the-ukidss-ultra-deep-survey-replacement/</guid>
		<description><![CDATA[We present spectroscopic confirmation of ten highly luminous (L &#62;= 2L*) Lyman alpha emitters in the redshift range 6.01&#60;z= 6 Lyman break galaxies (LBGs) selected from an area of 0.25 square degrees within the UKIDSS Ultra-deep Survey (UDS). Overall, our high rate of spectroscopic confirmation (&#62;= 71%) and low rate of contamination provides a strong [...]]]></description>
			<content:encoded><![CDATA[<p>We present spectroscopic confirmation of ten highly luminous (L &gt;= 2L*) Lyman alpha emitters in the redshift range 6.01&lt;z= 6 Lyman break galaxies (LBGs) selected from an area of 0.25 square degrees within the UKIDSS Ultra-deep Survey (UDS). Overall, our high rate of spectroscopic confirmation (&gt;= 71%) and low rate of contamination provides a strong vindication of the photometric redshift analysis used to define the original sample. By considering star-formation rate estimates based on the Ly_alpha and UV continuum luminosity we conclude that our sample is consistent with a Ly_alpha escape fraction of ~25%. Moreover, after careful consideration of the potential uncertainties and biases, we find that 40%-50% of our sample of L &gt;= 2L* galaxies at 6.0&lt;z= 25 Angs), a fraction which is a factor of ~2 higher than previously reported for L =2 L*) LBGs shows a similarly sharp increase to that observed in their lower-luminosity (L &lt;= L*) counterparts.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/a-remarkably-high-fraction-of-strong-ly_alpha-emitters-amongst-luminous-redshift-6-0z6-5-lyman-break-galaxies-in-the-ukidss-ultra-deep-survey-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Cosmological bounds on pseudo Nambu-Goldstone bosons [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/cosmological-bounds-on-pseudo-nambu-goldstone-bosons-replacement/</link>
		<comments>http://voxcharta.org/2012/02/22/cosmological-bounds-on-pseudo-nambu-goldstone-bosons-replacement/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:37:53 +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[alp]]></category>
		<category><![CDATA[bang nucleosynthesis]]></category>
		<category><![CDATA[big bang]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[cosmic microwave background]]></category>
		<category><![CDATA[cosmological implications]]></category>
		<category><![CDATA[coupling]]></category>
		<category><![CDATA[helium abundance]]></category>
		<category><![CDATA[large scale]]></category>
		<category><![CDATA[nambu]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[photon]]></category>
		<category><![CDATA[pngb]]></category>
		<category><![CDATA[primordial deuterium]]></category>
		<category><![CDATA[primordial helium]]></category>
		<category><![CDATA[probes]]></category>
		<category><![CDATA[relic]]></category>
		<category><![CDATA[scale structure]]></category>
		<category><![CDATA[structure data]]></category>
		<category><![CDATA[traditional bounds]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/cosmological-bounds-on-pseudo-nambu-goldstone-bosons-replacement/</guid>
		<description><![CDATA[We review the cosmological implications of a relic population of pseudo Nambu-Goldstone bosons (pNGB) with an anomalous coupling to two photons, often called axion-like particles (ALPs). We establish constraints on the pNGB mass and two-photon coupling by considering big bang nucleosynthesis, the physics of the cosmic microwave background, and the diffuse photon background. The bounds [...]]]></description>
			<content:encoded><![CDATA[<p>We review the cosmological implications of a relic population of pseudo Nambu-Goldstone bosons (pNGB) with an anomalous coupling to two photons, often called axion-like particles (ALPs). We establish constraints on the pNGB mass and two-photon coupling by considering big bang nucleosynthesis, the physics of the cosmic microwave background, and the diffuse photon background. The bounds from WMAP7 and other large-scale-structure data on the effective number of neutrino species can be stronger than the traditional bounds from the primordial helium abundance. These bounds, together with those from primordial deuterium abundance, constitute the most stringent probes of early decays.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/cosmological-bounds-on-pseudo-nambu-goldstone-bosons-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Constraining the topology of the Universe using the polarised CMB maps [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/constraining-the-topology-of-the-universe-using-the-polarised-cmb-maps-replacement/</link>
		<comments>http://voxcharta.org/2012/02/22/constraining-the-topology-of-the-universe-using-the-polarised-cmb-maps-replacement/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:37:39 +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[algorithm]]></category>
		<category><![CDATA[circles]]></category>
		<category><![CDATA[cmb anisotropy]]></category>
		<category><![CDATA[cosmic microwave background]]></category>
		<category><![CDATA[map]]></category>
		<category><![CDATA[minimum radius]]></category>
		<category><![CDATA[next generation]]></category>
		<category><![CDATA[noise level]]></category>
		<category><![CDATA[pair]]></category>
		<category><![CDATA[planck]]></category>
		<category><![CDATA[statistic]]></category>
		<category><![CDATA[temperature data]]></category>
		<category><![CDATA[topology]]></category>
		<category><![CDATA[toru]]></category>
		<category><![CDATA[universe]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/constraining-the-topology-of-the-universe-using-the-polarised-cmb-maps-replacement/</guid>
		<description><![CDATA[We study the possibility for constraining the topology of the Universe by means of the matched circles statistic applied to polarised cosmic microwave background (CMB) anisotropy maps. The advantages of using the CMB polarisation maps in studies of the topology over simply analysing the temperature data as has been done to-date are clearly demonstrated. We [...]]]></description>
			<content:encoded><![CDATA[<p>We study the possibility for constraining the topology of the Universe by means of the matched circles statistic applied to polarised cosmic microwave background (CMB) anisotropy maps. The advantages of using the CMB polarisation maps in studies of the topology over simply analysing the temperature data as has been done to-date are clearly demonstrated. We test our algorithm to search for pairs of matched circles on simulated CMB maps for a universe with the topology of 3-torus. It is found that the noise levels of both Planck and next generation CMB experiments data are no longer prohibitive and should be low enough to enable the use of the polarisation maps for such studies. For such experiments the minimum radius of the back-to-back matched circles which can be detected are determined. We also showed that the polarisation generated after reionisation does not have an impact on detectability of the matched circles.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/constraining-the-topology-of-the-universe-using-the-polarised-cmb-maps-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The X-ray cluster survey with eROSITA: forecasts for cosmology, cluster physics and primordial non-Gaussianity [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/the-x-ray-cluster-survey-with-erosita-forecasts-for-cosmology-cluster-physics-and-primordial-non-gaussianity-replacement/</link>
		<comments>http://voxcharta.org/2012/02/22/the-x-ray-cluster-survey-with-erosita-forecasts-for-cosmology-cluster-physics-and-primordial-non-gaussianity-replacement/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:37:25 +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[cluster physics]]></category>
		<category><![CDATA[cluster survey]]></category>
		<category><![CDATA[clusters of galaxies]]></category>
		<category><![CDATA[cosmic microwave background]]></category>
		<category><![CDATA[delta omega]]></category>
		<category><![CDATA[delta sigma]]></category>
		<category><![CDATA[energy band]]></category>
		<category><![CDATA[experimental probes]]></category>
		<category><![CDATA[galaxy cluster]]></category>
		<category><![CDATA[intracluster medium]]></category>
		<category><![CDATA[matrix analysis]]></category>
		<category><![CDATA[model parameter]]></category>
		<category><![CDATA[ray sky]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[sky survey]]></category>
		<category><![CDATA[temperature anisotropies]]></category>
		<category><![CDATA[tomographic analysis]]></category>
		<category><![CDATA[typical exposure time]]></category>
		<category><![CDATA[unprecedented sensitivity]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/the-x-ray-cluster-survey-with-erosita-forecasts-for-cosmology-cluster-physics-and-primordial-non-gaussianity-replacement/</guid>
		<description><![CDATA[Starting in late 2013, the eROSITA telescope will survey the X-ray sky with unprecedented sensitivity. Assuming a detection limit of 50 photons in the (0.5-2.0) keV energy band with a typical exposure time of 1.6 ks, we predict that eROSITA will detect ~ 9.3 X 10^4 clusters of galaxies more massive than 5 X 10^13 [...]]]></description>
			<content:encoded><![CDATA[<p>Starting in late 2013, the eROSITA telescope will survey the X-ray sky with unprecedented sensitivity. Assuming a detection limit of 50 photons in the (0.5-2.0) keV energy band with a typical exposure time of 1.6 ks, we predict that eROSITA will detect ~ 9.3 X 10^4 clusters of galaxies more massive than 5 X 10^13 Msun/h, with the currently planned all-sky survey. Their median redshift will be z ~ 0.35. We perform a Fisher-matrix analysis to forecast the constraining power of eROSITA on the LambdaCDM cosmology and, simultaneously, on the X-ray scaling relations for galaxy clusters. Special attention is devoted to the possibility of detecting primordial non-Gaussianity. We consider two experimental probes: the number counts and the angular clustering of a photon-count limited sample of clusters. We discuss how the cluster sample should be split to optimize the analysis and we show that redshift information of the individual clusters is vital to break the strong degeneracies among the model parameters. For example, performing a &#8220;tomographic&#8221; analysis based on photometric-redshift estimates and combining 1- and 2-point statistics will give marginal 1-sigma errors of Delta(sigma_8) ~ 0.036 and Delta(Omega_m) ~ 0.012 without priors, and improve the current estimates on the slope of the luminosity-mass relation by a factor of 3. Regarding primordial non-Gaussianity, eROSITA clusters alone will give Delta(f_NL) = 9, 36, 144 for the local, orthogonal and equilateral model, respectively. Measuring redshifts with spectroscopic accuracy would further tighten the constraints by nearly 40 per cent (barring f_NL which displays smaller improvements). Finally, combining eROSITA data with the analysis of temperature anisotropies in the cosmic microwave background by the Planck satellite should give sensational constraints on both the cosmology and the properties of the intracluster medium.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/the-x-ray-cluster-survey-with-erosita-forecasts-for-cosmology-cluster-physics-and-primordial-non-gaussianity-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Measuring our Peculiar Velocity by &quot;Pre-deboosting&quot; the CMB [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/measuring-our-peculiar-velocity-by-pre-deboosting-the-cmb-replacement/</link>
		<comments>http://voxcharta.org/2012/02/22/measuring-our-peculiar-velocity-by-pre-deboosting-the-cmb-replacement/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:37:14 +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[beta]]></category>
		<category><![CDATA[CMB]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[dipole]]></category>
		<category><![CDATA[ell]]></category>
		<category><![CDATA[fitting functions]]></category>
		<category><![CDATA[Measurement]]></category>
		<category><![CDATA[missions]]></category>
		<category><![CDATA[peculiar velocity]]></category>
		<category><![CDATA[perturbation analysis]]></category>
		<category><![CDATA[planck]]></category>
		<category><![CDATA[scales]]></category>
		<category><![CDATA[validity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/measuring-our-peculiar-velocity-by-pre-deboosting-the-cmb-replacement/</guid>
		<description><![CDATA[It was recently shown that our peculiar velocity \beta with respect to the CMB induces mixing among multipoles and off-diagonal correlations at all scales which can be used as a measurement of \beta, which is independent of the standard measurement using the CMB temperature dipole. The proposed techniques rely however on a perturbative expansion which [...]]]></description>
			<content:encoded><![CDATA[<p>It was recently shown that our peculiar velocity \beta with respect to the CMB induces mixing among multipoles and off-diagonal correlations at all scales which can be used as a measurement of \beta, which is independent of the standard measurement using the CMB temperature dipole. The proposed techniques rely however on a perturbative expansion which breaks down for \ell \gtrsim 1/(\beta) \approx 800. Here we propose a technique which consists of deboosting the CMB temperature in the time-ordered data and show that it extends the validity of the perturbation analysis multipoles up to \ell \sim 10000. We also obtain accurate fitting functions for the mixing between multipoles valid in a full non-linear treatment. Finally we forecast the achievable precision with which these correlations can be measured in a number of current and future CMB missions. We show that Planck could measure the velocity with a precision of around 60 km/s, ACTPol in 4 years around 40 km/s, while proposed future experiments could further shrink this error bar by over a factor of around 2.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/measuring-our-peculiar-velocity-by-pre-deboosting-the-cmb-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Circumstellar disks in binary star systems [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/circumstellar-disks-in-binary-star-systems-replacement/</link>
		<comments>http://voxcharta.org/2012/02/22/circumstellar-disks-in-binary-star-systems-replacement/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:36:59 +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[alpha centauri system]]></category>
		<category><![CDATA[binaries]]></category>
		<category><![CDATA[binary star system]]></category>
		<category><![CDATA[cephei]]></category>
		<category><![CDATA[companion star]]></category>
		<category><![CDATA[coplanarity]]></category>
		<category><![CDATA[disk mass]]></category>
		<category><![CDATA[eccentricity]]></category>
		<category><![CDATA[energy equation]]></category>
		<category><![CDATA[epsilon]]></category>
		<category><![CDATA[host star]]></category>
		<category><![CDATA[hydrodynamical simulations]]></category>
		<category><![CDATA[opacity tables]]></category>
		<category><![CDATA[planet formation]]></category>
		<category><![CDATA[planetesimal]]></category>
		<category><![CDATA[realistic conditions]]></category>
		<category><![CDATA[staggered mesh]]></category>
		<category><![CDATA[velocities]]></category>
		<category><![CDATA[viscosity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/circumstellar-disks-in-binary-star-systems-replacement/</guid>
		<description><![CDATA[In this paper we study the evolution of viscous and radiative circumstellar disks under the influence of a companion star. We focus on the eccentric {\gamma} Cephei and {\alpha} Centauri system as examples and compare the disk quantities such as disk eccentricity and precession rate to previous isothermal simulations. We perform two-dimensional hydrodynamical simulations of [...]]]></description>
			<content:encoded><![CDATA[<p>In this paper we study the evolution of viscous and radiative circumstellar disks under the influence of a companion star. We focus on the eccentric {\gamma} Cephei and {\alpha} Centauri system as examples and compare the disk quantities such as disk eccentricity and precession rate to previous isothermal simulations. We perform two-dimensional hydrodynamical simulations of the binary star systems under the assumption of coplanarity of the disk, host star and binary companion. We use the grid-based, staggered mesh code FARGO with an additional energy equation to which we added radiative cooling based on opacity tables. The eccentric binary companion perturbs the disk around the primary star periodically. Upon passing periastron spirals arms are induced that wind from the outer disk towards the star. In isothermal simulations this results in disk eccentricities up to {\epsilon}_disk ~ 0.2, but in more realistic radiative models we obtain much smaller eccentricities of about {\epsilon}_disk ~ 0.04 &#8211; 0.06 with no real precession. Models with varying viscosity and disk mass indicate show that disks with less mass have lower temperatures and higher disk eccentricity. The rather large high disk eccentricities, as indicated in previous isothermal disk simulations, implied a more difficult planet formation in the {\gamma} Cephei system due to the enhanced collision velocities of planetesimals. We have shown that under more realistic conditions with radiative cooling the disk become less eccentric and thus planet formation may be made easier. However, we estimate that the viscosity in the disk has to very small, with {\alpha} \lesssim 0.001, because otherwise the disk&#8217;s lifetime will be too short to allow planet formation to occur along the core instability scenario. We estimate that the periodic heating of the disk in eccentric binaries will be observable in the mid-IR regime.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/circumstellar-disks-in-binary-star-systems-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Updated global fits of the cMSSM including the latest LHC SUSY and Higgs searches and XENON100 data [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/updated-global-fits-of-the-cmssm-including-the-latest-lhc-susy-and-higgs-searches-and-xenon100-data-replacement/</link>
		<comments>http://voxcharta.org/2012/02/22/updated-global-fits-of-the-cmssm-including-the-latest-lhc-susy-and-higgs-searches-and-xenon100-data-replacement/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:36:44 +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[anomalous magnetic moment]]></category>
		<category><![CDATA[astrophysical]]></category>
		<category><![CDATA[bayesian]]></category>
		<category><![CDATA[collider experiments]]></category>
		<category><![CDATA[complementarity]]></category>
		<category><![CDATA[dominant role]]></category>
		<category><![CDATA[focus point]]></category>
		<category><![CDATA[hadronic]]></category>
		<category><![CDATA[higgs boson]]></category>
		<category><![CDATA[higgs search]]></category>
		<category><![CDATA[lhc]]></category>
		<category><![CDATA[mass region]]></category>
		<category><![CDATA[model physics]]></category>
		<category><![CDATA[muon]]></category>
		<category><![CDATA[parameter space]]></category>
		<category><![CDATA[profile likelihood]]></category>
		<category><![CDATA[standard model]]></category>
		<category><![CDATA[statistical perspective]]></category>
		<category><![CDATA[susy]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/updated-global-fits-of-the-cmssm-including-the-latest-lhc-susy-and-higgs-searches-and-xenon100-data-replacement/</guid>
		<description><![CDATA[We present new global fits of the cMSSM, including LHC 1/fb integrated luminosity SUSY exclusion limits, recent LHC 5/fb constraints on the mass of the Higgs boson and XENON100 direct detection data. Our analysis fully takes into account astrophysical and hadronic uncertainties that enter the analysis when translating direct detection limits into constraints on the [...]]]></description>
			<content:encoded><![CDATA[<p>We present new global fits of the cMSSM, including LHC 1/fb integrated luminosity SUSY exclusion limits, recent LHC 5/fb constraints on the mass of the Higgs boson and XENON100 direct detection data. Our analysis fully takes into account astrophysical and hadronic uncertainties that enter the analysis when translating direct detection limits into constraints on the cMSSM parameter space. We provide results for both a Bayesian and a Frequentist statistical analysis. We find that LHC 2011 constraints in combination with XENON100 data can rule out a significant portion of the cMSSM parameter space. Our results further emphasise the complementarity of collider experiments and direct detection searches in constraining extensions of Standard Model physics. The LHC 2011 exclusion limit strongly impacts on low-mass regions of cMSSM parameter space, such as the stau co-annihilation region, while direct detection data can rule out regions of high SUSY masses, such as the Focus-Point region, which is unreachable for the LHC in the near future. We show that, in addition to XENON100 data, the experimental constraint on the anomalous magnetic moment of the muon plays a dominant role in disfavouring large scalar and gaugino masses. We find that, should the LHC 2011 excess hinting towards a Higgs boson at 126 GeV be confirmed, currently favoured regions of the cMSSM parameter space will be robustly ruled out from both a Bayesian and a profile likelihood statistical perspective.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/updated-global-fits-of-the-cmssm-including-the-latest-lhc-susy-and-higgs-searches-and-xenon100-data-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Chandra Survey of Nearby Edge-on Disk Galaxies I: Luminosities of Galactic Coronae [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/chandra-survey-of-nearby-edge-on-disk-galaxies-i-luminosities-of-galactic-coronae-replacement/</link>
		<comments>http://voxcharta.org/2012/02/22/chandra-survey-of-nearby-edge-on-disk-galaxies-i-luminosities-of-galactic-coronae-replacement/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:36:22 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[chandra observation]]></category>
		<category><![CDATA[chemical states]]></category>
		<category><![CDATA[coronal gas]]></category>
		<category><![CDATA[disk galaxy]]></category>
		<category><![CDATA[energy input]]></category>
		<category><![CDATA[galactic halo]]></category>
		<category><![CDATA[gravitational mass]]></category>
		<category><![CDATA[horizontal extent]]></category>
		<category><![CDATA[intergalactic medium]]></category>
		<category><![CDATA[linear relation]]></category>
		<category><![CDATA[nearby galaxy]]></category>
		<category><![CDATA[orders of magnitude]]></category>
		<category><![CDATA[profound implications]]></category>
		<category><![CDATA[radiation efficiency]]></category>
		<category><![CDATA[rotation velocity]]></category>
		<category><![CDATA[sfr]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/chandra-survey-of-nearby-edge-on-disk-galaxies-i-luminosities-of-galactic-coronae-replacement/</guid>
		<description><![CDATA[X-ray-emitting coronae of nearby galaxies are expected to be produced either by accretion from the intergalactic medium and/or by various galactic feedback. We herein present a systematical analysis of the Chandra observations of 53 nearby edge-on disk galaxies over a range of 3 orders of magnitude in SFR. Various coronal properties, such as the luminosity, [...]]]></description>
			<content:encoded><![CDATA[<p>X-ray-emitting coronae of nearby galaxies are expected to be produced either by accretion from the intergalactic medium and/or by various galactic feedback. We herein present a systematical analysis of the Chandra observations of 53 nearby edge-on disk galaxies over a range of 3 orders of magnitude in SFR. Various coronal properties, such as the luminosity, vertical/horizontal extent, and other inferred parameters, are characterized for all the sample galaxies. For galaxies with high enough counting statistics, we also examine the thermal and chemical states of the coronal gas. Here we concentrate on the coronal luminosity (Lx), estimated in 0.5-2keV and within 5 times the diffuse X-ray vertical scale height. We find Lx strongly correlates with the SFR for the whole sample. But the inclusion of Ia SNe in the total energy input (E_SN) gives an even tighter correlation, which may be characterized with a linear relation, Lx=0.5%E_SN, and with a dispersion of 0.45dex. Moreover, the coronal radiation efficiency (\eta=Lx/E_SN) shows little correlation with either the stellar mass or the gravitational mass (M_TF, inferred from the rotation velocity), but is significantly correlated with their ratio (M_TF/M_*), which may be expressed as a linear scaling relation \eta=0.35%M_TF/M_* for the entire ranges of galaxy parameters. This joint scaling relation suggests that the coronae are self-regulated by the combination of gravitational confinement and feedback. But SN appears to be the primary heating source, because about half of our galaxies are not massive enough to allow for the accretion to play a major role. The commonly low \eta further suggests that the bulk of the SN energy likely flows out into large-scale galactic halos for essentially all the galaxies. Such ubiquitous outflows could have profound implications for understanding the ecosystem, hence the evolution of galaxies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/chandra-survey-of-nearby-edge-on-disk-galaxies-i-luminosities-of-galactic-coronae-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Habitability of Earth-type Planets and Moons in the Kepler-16 System [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/habitability-of-earth-type-planets-and-moons-in-the-kepler-16-system-replacement-2/</link>
		<comments>http://voxcharta.org/2012/02/22/habitability-of-earth-type-planets-and-moons-in-the-kepler-16-system-replacement-2/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:35:58 +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[16b]]></category>
		<category><![CDATA[earth mass]]></category>
		<category><![CDATA[earth type]]></category>
		<category><![CDATA[habitability]]></category>
		<category><![CDATA[habitable zone]]></category>
		<category><![CDATA[kepler]]></category>
		<category><![CDATA[moons and planets]]></category>
		<category><![CDATA[orbital stability]]></category>
		<category><![CDATA[planetary atmosphere]]></category>
		<category><![CDATA[planetary orbit]]></category>
		<category><![CDATA[planets and moons]]></category>
		<category><![CDATA[s type]]></category>
		<category><![CDATA[satellite]]></category>
		<category><![CDATA[saturn]]></category>
		<category><![CDATA[type planets]]></category>
		<category><![CDATA[vicinity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/habitability-of-earth-type-planets-and-moons-in-the-kepler-16-system-replacement-2/</guid>
		<description><![CDATA[We demonstrate that habitable Earth-mass planets and moons can exist in the Kepler-16 system, known to host a Saturn-mass planet around a stellar binary, by investigating their orbital stability in the standard and extended habitable zone (HZ). We find that Earth-mass planets in satellite-like (S-type)orbits are possible within the standard HZ in direct vicinity of [...]]]></description>
			<content:encoded><![CDATA[<p>We demonstrate that habitable Earth-mass planets and moons can exist in the Kepler-16 system, known to host a Saturn-mass planet around a stellar binary, by investigating their orbital stability in the standard and extended habitable zone (HZ). We find that Earth-mass planets in satellite-like (S-type)orbits are possible within the standard HZ in direct vicinity of Kepler-16b, thus constituting habitable exomoons. However, Earth-mass planets cannot exist in planetary-like (P-type) orbits around the two stellar components within the standard HZ. Yet, P-type Earth-mass planets can exist superior to the Saturnian planet in the extended HZ pertaining to considerably enhanced back-warming in the planetary atmosphere if facilitated. We briefly discuss the potential detectability of such habitable Earth-mass moons and planets positioned in satellite and planetary orbits, respectively. The range of inferior and superior P-type orbits in the HZ is between 0.657 to 0.71 AU and 0.95 to 1.02 AU, respectively.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/habitability-of-earth-type-planets-and-moons-in-the-kepler-16-system-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>The dust scaling relations of the Herschel Reference Survey [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/the-dust-scaling-relations-of-the-herschel-reference-survey-replacement/</link>
		<comments>http://voxcharta.org/2012/02/22/the-dust-scaling-relations-of-the-herschel-reference-survey-replacement/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:35:43 +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[cluster galaxy]]></category>
		<category><![CDATA[cold dust]]></category>
		<category><![CDATA[dust disk]]></category>
		<category><![CDATA[field galaxies]]></category>
		<category><![CDATA[galactic center]]></category>
		<category><![CDATA[gas phase]]></category>
		<category><![CDATA[hi gas]]></category>
		<category><![CDATA[interstellar medium]]></category>
		<category><![CDATA[mass ratio]]></category>
		<category><![CDATA[mass surface]]></category>
		<category><![CDATA[millimeter observations]]></category>
		<category><![CDATA[monotonically]]></category>
		<category><![CDATA[morphological type]]></category>
		<category><![CDATA[nearby galaxy]]></category>
		<category><![CDATA[nuv]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[surface density]]></category>
		<category><![CDATA[type galaxy]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/the-dust-scaling-relations-of-the-herschel-reference-survey-replacement/</guid>
		<description><![CDATA[We combine new Herschel/SPIRE sub-millimeter observations with existing multiwavelength data to investigate the dust scaling relations of the Herschel Reference Survey, a magnitude-, volume-limited sample of ~300 nearby galaxies in different environments. We show that the dust-to-stellar mass ratio anti-correlates with stellar mass, stellar mass surface density and NUV-r colour across the whole range of [...]]]></description>
			<content:encoded><![CDATA[<p>We combine new Herschel/SPIRE sub-millimeter observations with existing multiwavelength data to investigate the dust scaling relations of the Herschel Reference Survey, a magnitude-, volume-limited sample of ~300 nearby galaxies in different environments. We show that the dust-to-stellar mass ratio anti-correlates with stellar mass, stellar mass surface density and NUV-r colour across the whole range of parameters covered by our sample. Moreover, the dust-to-stellar mass ratio decreases significantly when moving from late- to early-type galaxies. These scaling relations are similar to those observed for the HI gas-fraction, supporting the idea that the cold dust is tightly coupled to the cold atomic gas component in the interstellar medium. We also find a weak increase of the dust-to-HI mass ratio with stellar mass and colour but no trend is seen with stellar mass surface density. By comparing galaxies in different environments we show that, although these scaling relations are followed by both cluster and field galaxies, HI-deficient systems have, at fixed stellar mass, stellar mass surface density and morphological type systematically lower dust-to-stellar mass and higher dust-to-HI mass ratios than HI-normal/field galaxies. This provides clear evidence that dust is removed from the star-forming disk of cluster galaxies but the effect of the environment is less strong than what is observed in the case of the HI disk. Such effects naturally arise if the dust disk is less extended than the HI and follows more closely the distribution of the molecular gas phase, i.e., if the dust-to-atomic gas ratio monotonically decreases with distance from the galactic center.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
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		<item>
		<title>Relativistic Cosmology Number Densities and the Luminosity Function [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/relativistic-cosmology-number-densities-and-the-luminosity-function-replacement/</link>
		<comments>http://voxcharta.org/2012/02/22/relativistic-cosmology-number-densities-and-the-luminosity-function-replacement/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:34:46 +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[cosmology theory]]></category>
		<category><![CDATA[data selection]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[friedmann]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[galaxy distribution]]></category>
		<category><![CDATA[galaxy luminosity function]]></category>
		<category><![CDATA[galaxy survey]]></category>
		<category><![CDATA[light cone]]></category>
		<category><![CDATA[luminosity function]]></category>
		<category><![CDATA[number density]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[parametrization]]></category>
		<category><![CDATA[previous results]]></category>
		<category><![CDATA[redshift range]]></category>
		<category><![CDATA[relativistic cosmology]]></category>
		<category><![CDATA[ribeiro]]></category>
		<category><![CDATA[selection function]]></category>
		<category><![CDATA[spacetime]]></category>
		<category><![CDATA[stoeger]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/relativistic-cosmology-number-densities-and-the-luminosity-function-replacement/</guid>
		<description><![CDATA[This paper studies the connection between the relativistic number density of galaxies down the past light cone in a Friedmann-Lemaitre-Robertson-Walker spacetime with non-vanishing cosmological constant and the galaxy luminosity function (LF) data. It extends the redshift range of previous results presented in Albani et al. (2007:astro-ph/0611032) where the galaxy distribution was studied out to z=1. [...]]]></description>
			<content:encoded><![CDATA[<p>This paper studies the connection between the relativistic number density of galaxies down the past light cone in a Friedmann-Lemaitre-Robertson-Walker spacetime with non-vanishing cosmological constant and the galaxy luminosity function (LF) data. It extends the redshift range of previous results presented in Albani et al. (2007:astro-ph/0611032) where the galaxy distribution was studied out to z=1. Observational inhomogeneities were detected at this range. This research also searches for LF evolution in the context of the framework advanced by Ribeiro and Stoeger (2003:astro-ph/0304094), further developing the theory linking relativistic cosmology theory and LF data. Selection functions are obtained using the Schechter parameters and redshift parametrization of the galaxy luminosity functions obtained from an I-band selected dataset of the FORS Deep Field galaxy survey in the redshift range 0.5&lt;z&lt;5.0 for its blue bands and 0.75&lt;z&lt;3.0 for its red ones. Differential number counts, densities and other related observables are obtained, and then used with the calculated selection functions to study the empirical radial distribution of the galaxies in a fully relativistic framework. The redshift range of the dataset used in this work, which is up to five times larger than the one used in previous studies, shows an increased relevance of the relativistic effects of expansion when compared to the evolution of the LF at the higher redshifts. The results also agree with the preliminary ones presented in Albani et al. (2007:astro-ph/0611032), suggesting a power-law behavior of relativistic densities at high redshifts when they are defined in terms of the luminosity distance.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/relativistic-cosmology-number-densities-and-the-luminosity-function-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>First order Fermi acceleration driven by magnetic reconnection [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/first-order-fermi-acceleration-driven-by-magnetic-reconnection-replacement/</link>
		<comments>http://voxcharta.org/2012/02/22/first-order-fermi-acceleration-driven-by-magnetic-reconnection-replacement/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:34:33 +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 time]]></category>
		<category><![CDATA[applicability]]></category>
		<category><![CDATA[box model]]></category>
		<category><![CDATA[magnetic reconnection]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[shock acceleration]]></category>
		<category><![CDATA[spectral index]]></category>
		<category><![CDATA[time scale]]></category>
		<category><![CDATA[universal spectrum]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/first-order-fermi-acceleration-driven-by-magnetic-reconnection-replacement/</guid>
		<description><![CDATA[A box model is used to study first order Fermi acceleration driven by magnetic reconnection. It is shown, at least in this simple model, that the spectral index of the accelerated particles is related to the total compression in the same way as in diffusive shock acceleration and is not, as has been suggested, a [...]]]></description>
			<content:encoded><![CDATA[<p>A box model is used to study first order Fermi acceleration driven by magnetic reconnection. It is shown, at least in this simple model, that the spectral index of the accelerated particles is related to the total compression in the same way as in diffusive shock acceleration and is not, as has been suggested, a universal $E^{-5/2}$ spectrum. The acceleration time-scale is estimated and some comments made about the applicability of the process.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/first-order-fermi-acceleration-driven-by-magnetic-reconnection-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Possible optical counterpart of PSR J1357-6429 [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/possible-optical-counterpart-of-psr-j1357-6429-replacement/</link>
		<comments>http://voxcharta.org/2012/02/22/possible-optical-counterpart-of-psr-j1357-6429-replacement/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:34:15 +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[AGN]]></category>
		<category><![CDATA[error circle]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[hes]]></category>
		<category><![CDATA[knot]]></category>
		<category><![CDATA[nebula]]></category>
		<category><![CDATA[optical counterpart]]></category>
		<category><![CDATA[optical identification]]></category>
		<category><![CDATA[optical observation]]></category>
		<category><![CDATA[proper motion]]></category>
		<category><![CDATA[pulsars]]></category>
		<category><![CDATA[radio pulsar]]></category>
		<category><![CDATA[spectral index]]></category>
		<category><![CDATA[TeV]]></category>
		<category><![CDATA[transverse velocity]]></category>
		<category><![CDATA[vela pulsar]]></category>
		<category><![CDATA[wavelength]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/possible-optical-counterpart-of-psr-j1357-6429-replacement/</guid>
		<description><![CDATA[(Abridged) PSR J1357-6429 is a Vela-like radio pulsar that has been recently detected in X-rays and gamma-rays. It powers a compact tail-like X-ray pulsar wind nebula and X-ray-radio plerion associated with an extended TeV source HESS J1356-645. We present our deep optical observations with the Very Large Telescope to search for an optical counterpart of [...]]]></description>
			<content:encoded><![CDATA[<p>(Abridged) PSR J1357-6429 is a Vela-like radio pulsar that has been recently detected in X-rays and gamma-rays. It powers a compact tail-like X-ray pulsar wind nebula and X-ray-radio plerion associated with an extended TeV source HESS J1356-645. We present our deep optical observations with the Very Large Telescope to search for an optical counterpart of the pulsar and its nebula. We detect a point-like source in V, R, and I bands whose position is within the 1-sigma error circle of the X-ray position of the pulsar, and whose colours are distinct from those of ordinary stars. We consider it as a candidate optical counterpart of the pulsar. If it is indeed the counterpart, its 5-sigma offset from the radio pulsar position, measured about 9 yr earlier, implies that the transverse velocity of the pulsar is in the range of 1600&#8211;2000 km s^{-1} at the distance of 2&#8211;2.5 kpc, making it the fastest moving pulsar known. The direction of the estimated proper motion coincides with the extension of the pulsar&#8217;s X-ray tail, suggesting that this is a jet. The tentative optical luminosity and efficiency of the pulsar are similar to those of the Vela pulsar, which also supports the optical identification. However, the candidate undergoes an unusually steep dereddened flux increase towards the infrared with a spectral index of about 5, that is not typical of optical pulsars. It implies a strong double-knee spectral break in the pulsar emission between the optical and X-rays. The reasons for the spectral steepness are unclear. It may be caused by a nebula knot projected onto the jet and strongly overlapping with the pulsar, as observed for the Crab, where the knot has a significantly steeper spectrum than the pulsar. We find no other signs of the pulsar nebula in the optical. Alternatively, the detected source may be a faint AGN, that has not yet been seen at other wavelengths.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
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		<item>
		<title>A Super-Damped Lyman-alpha QSO Absorber at z=2.2 [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/a-super-damped-lyman-alpha-qso-absorber-at-z2-2-replacement/</link>
		<comments>http://voxcharta.org/2012/02/22/a-super-damped-lyman-alpha-qso-absorber-at-z2-2-replacement/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:33:55 +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[absorber]]></category>
		<category><![CDATA[absorption]]></category>
		<category><![CDATA[digital sky survey]]></category>
		<category><![CDATA[electron density]]></category>
		<category><![CDATA[extinction]]></category>
		<category><![CDATA[GRB]]></category>
		<category><![CDATA[lmc]]></category>
		<category><![CDATA[lyman alpha]]></category>
		<category><![CDATA[metallicity]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[qso]]></category>
		<category><![CDATA[radiation field]]></category>
		<category><![CDATA[sfr]]></category>
		<category><![CDATA[sloan digital]]></category>
		<category><![CDATA[smc]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[surface density]]></category>
		<category><![CDATA[trough]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/a-super-damped-lyman-alpha-qso-absorber-at-z2-2-replacement/</guid>
		<description><![CDATA[We report the discovery of a &#8220;super-damped&#8221; Lyman-alpha absorber at $z_{abs}=2.2068$ toward QSO Q1135-0010 in the Sloan Digital Sky Survey, and follow-up VLT UVES spectroscopy. Voigt profile fit to the DLA line indicates log $N_{\rm H I} = 22.05 \pm 0.1$. This is the second QSO DLA discovered to date with such high $N_{\rm H [...]]]></description>
			<content:encoded><![CDATA[<p>We report the discovery of a &#8220;super-damped&#8221; Lyman-alpha absorber at $z_{abs}=2.2068$ toward QSO Q1135-0010 in the Sloan Digital Sky Survey, and follow-up VLT UVES spectroscopy. Voigt profile fit to the DLA line indicates log $N_{\rm H I} = 22.05 \pm 0.1$. This is the second QSO DLA discovered to date with such high $N_{\rm H I}$. We derive element abundances [Si/H] = $-1.10 \pm 0.10$, [Zn/H] = $-1.06 \pm 0.10$, [Cr/H] = $-1.55 \pm 0.10$, [Ni/H] = $-1.60 \pm 0.10$, [Fe/H] = $-1.76 \pm 0.10$, [Ti/H] = $-1.69 \pm 0.11$, [P/H] = $-0.93 \pm 0.23$, and [Cu/H] = $-0.75 \pm 0.14$. Our data indicate detection of Ly-$\alpha$ emission in the DLA trough, implying a star formation rate of $\sim$10 $M_{\odot}$ yr$^{-1}$ in the absence of dust attenuation. C II$^{*} \, \lambda 1336$ absorption is also detected, suggesting SFR surface density $-2 &lt; {\rm log} \, \dot{\psi_{*}} &lt; 0$ $M_{\odot}$ yr$^{-1}$ kpc$^{-2}$. We estimate electron density in the range $3.5 \times 10^{-4}$ to 24.7 cm$^{-3}$ from C II$^{*}$/C II, and $\sim$0.5-0.9 cm$^{-3}$ from Si II$^{*}$/Si II. Overall, this is a robustly star-forming, moderately enriched absorber, but with relatively low dust depletion. Fitting of the SDSS spectrum yields low reddening for Milky Way, LMC, or SMC extinction curves. No CO absorption is detected, and C I absorption is weak. The low dust and molecular content, reminiscent of some SMC sight-lines, may result from the lower metallicity, and a stronger radiation field (due to higher SFR). Finally, we compare this absorber with other QSO and GRB DLAs.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/a-super-damped-lyman-alpha-qso-absorber-at-z2-2-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Critical Conditions for Core-Collapse Supernovae [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/critical-conditions-for-core-collapse-supernovae-replacement/</link>
		<comments>http://voxcharta.org/2012/02/22/critical-conditions-for-core-collapse-supernovae-replacement/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:33:41 +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[accretion]]></category>
		<category><![CDATA[core collapse supernova]]></category>
		<category><![CDATA[core collapse supernovae]]></category>
		<category><![CDATA[critical condition]]></category>
		<category><![CDATA[critical flow]]></category>
		<category><![CDATA[critical value]]></category>
		<category><![CDATA[explosion]]></category>
		<category><![CDATA[isothermal layer]]></category>
		<category><![CDATA[neutrino luminosity]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[numerical result]]></category>
		<category><![CDATA[proto]]></category>
		<category><![CDATA[radius]]></category>
		<category><![CDATA[shell]]></category>
		<category><![CDATA[shock]]></category>
		<category><![CDATA[steady state solution]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/critical-conditions-for-core-collapse-supernovae-replacement/</guid>
		<description><![CDATA[The explosion of a core-collapse supernova is approximated by the breakdown of the steady-state solution for accretion onto a proto-neutron-star (PNS). We analytically show that as the neutrino luminosity exceeds a critical value L_c, the neutrinosphere pressure exceeds the hydrostatic limit even for an optimal shock radius R. This yields L_c \propto M^2 T^2 (with [...]]]></description>
			<content:encoded><![CDATA[<p>The explosion of a core-collapse supernova is approximated by the breakdown of the steady-state solution for accretion onto a proto-neutron-star (PNS). We analytically show that as the neutrino luminosity exceeds a critical value L_c, the neutrinosphere pressure exceeds the hydrostatic limit even for an optimal shock radius R. This yields L_c \propto M^2 T^2 (with logarithmic corrections) and R \propto M/T, in agreement with numerical results, where M, T are the PNS mass, neutrino temperature. The near-critical flow can be approximated as a ballistic shell on top of an isothermal layer.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Thermodynamics of phantom Reissner-Nordstrom-AdS black hole [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/thermodynamics-of-phantom-reissner-nordstrom-ads-black-hole-replacement/</link>
		<comments>http://voxcharta.org/2012/02/22/thermodynamics-of-phantom-reissner-nordstrom-ads-black-hole-replacement/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:33:29 +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[black hole]]></category>
		<category><![CDATA[de sitter]]></category>
		<category><![CDATA[einstein]]></category>
		<category><![CDATA[ensembles]]></category>
		<category><![CDATA[extreme case]]></category>
		<category><![CDATA[maxwell theory]]></category>
		<category><![CDATA[new solution]]></category>
		<category><![CDATA[nordstrom]]></category>
		<category><![CDATA[phantom]]></category>
		<category><![CDATA[phase transition]]></category>
		<category><![CDATA[specific heat]]></category>
		<category><![CDATA[thermodynamic stability]]></category>
		<category><![CDATA[thermodynamics]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/thermodynamics-of-phantom-reissner-nordstrom-ads-black-hole-replacement/</guid>
		<description><![CDATA[We obtain a new solution of the Einstein-anti-Maxwell theory with cosmological constant, called anti-Reissner-Nordstrom-(A)de Sitter (anti-RN-(A)dS) solution. The basic properties of this solution were reviewed. Its thermodynamics is consistently established, with the extreme cases and phase transitions, making the analysis through two methods, the usual and that of Geometrothermodynamics. The analysis by Geometrothermodynamics does not [...]]]></description>
			<content:encoded><![CDATA[<p>We obtain a new solution of the Einstein-anti-Maxwell theory with cosmological constant, called anti-Reissner-Nordstrom-(A)de Sitter (anti-RN-(A)dS) solution. The basic properties of this solution were reviewed. Its thermodynamics is consistently established, with the extreme cases and phase transitions, making the analysis through two methods, the usual and that of Geometrothermodynamics. The analysis by Geometrothermodynamics does not provide us a result in agreement with the usual method, and by the specific heat. We establish local and global thermodynamic stability of anti-RN-AdS solution through the specific heat and the canonical and grand-canonical ensembles.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/thermodynamics-of-phantom-reissner-nordstrom-ads-black-hole-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/2012/02/22/the-strong-multifield-slowroll-condition-and-spiral-inflation-replacement/</link>
		<comments>http://voxcharta.org/2012/02/22/the-strong-multifield-slowroll-condition-and-spiral-inflation-replacement/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:33:14 +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[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[models]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[spiral]]></category>
		<category><![CDATA[string theory]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/the-strong-multifield-slowroll-condition-and-spiral-inflation-replacement/</guid>
		<description><![CDATA[We point out the existing confusions about the slowroll parameters and conditions for multifield inflation. If one requires the field 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 field 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 and even bypasses the first slowroll condition. We provide the &#8220;spiral inflation&#8221; as a generic blueprint of such inflation models and point out that it might be common in string theory through the abundant monodromy loci.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/the-strong-multifield-slowroll-condition-and-spiral-inflation-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Citations to Australian Astronomy: 5 and 10 Year Benchmarks [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/citations-to-australian-astronomy-5-and-10-year-benchmarks-replacement-2/</link>
		<comments>http://voxcharta.org/2012/02/22/citations-to-australian-astronomy-5-and-10-year-benchmarks-replacement-2/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:32:46 +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[astronomical society]]></category>
		<category><![CDATA[astrophysics data system]]></category>
		<category><![CDATA[australian astronomy]]></category>
		<category><![CDATA[australian universities]]></category>
		<category><![CDATA[benchmark]]></category>
		<category><![CDATA[career researchers]]></category>
		<category><![CDATA[citation]]></category>
		<category><![CDATA[citation count]]></category>
		<category><![CDATA[first decade]]></category>
		<category><![CDATA[hirsch]]></category>
		<category><![CDATA[histogram]]></category>
		<category><![CDATA[metrics]]></category>
		<category><![CDATA[nasa]]></category>
		<category><![CDATA[nasa astrophysics data]]></category>
		<category><![CDATA[nasa astrophysics data system]]></category>
		<category><![CDATA[observatory]]></category>
		<category><![CDATA[percentile]]></category>
		<category><![CDATA[professional astronomers]]></category>
		<category><![CDATA[research organisations]]></category>
		<category><![CDATA[web page]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/citations-to-australian-astronomy-5-and-10-year-benchmarks-replacement-2/</guid>
		<description><![CDATA[Expanding upon Pimbblet&#8217;s informative 2011 analysis of career h-indices for members of the Astronomical Society of Australia, we provide additional citation metrics which are geared to a) quantifying the current performance of b) all professional astronomers in Australia. We have trawled the staff web-pages of Australian Universities, Observatories and Research Organisations hosting professional astronomers, and [...]]]></description>
			<content:encoded><![CDATA[<p>Expanding upon Pimbblet&#8217;s informative 2011 analysis of career h-indices for members of the Astronomical Society of Australia, we provide additional citation metrics which are geared to a) quantifying the current performance of b) all professional astronomers in Australia. We have trawled the staff web-pages of Australian Universities, Observatories and Research Organisations hosting professional astronomers, and identified 383 PhD-qualified, research-active, astronomers in the nation &#8211; 131 of these are not members of the Astronomical Society of Australia. Using the SAO/NASA Astrophysics Data System, we provide the three following common metrics based on publications in the first decade of the 21st century (2001-2010): h-index, author-normalised citation count and lead-author citation count. We additionally present a somewhat more inclusive analysis, applicable for many early-career researchers, that is based on publications from 2006-2010. Histograms and percentiles, plus top-performer lists, are presented for each category. Finally, building on Hirsch&#8217;s empirical equation, we find that the (10-year) h-index and (10-year) total citation count T can be approximated by the relation h = (0.5+sqrt{T})/sqrt{5} for h &gt; 5.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/citations-to-australian-astronomy-5-and-10-year-benchmarks-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Future constraints on variations of the fine structure constant from combined CMB and weak lensing measurements [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/future-constraints-on-variations-of-the-fine-structure-constant-from-combined-cmb-and-weak-lensing-measurements-replacement-2/</link>
		<comments>http://voxcharta.org/2012/02/22/future-constraints-on-variations-of-the-fine-structure-constant-from-combined-cmb-and-weak-lensing-measurements-replacement-2/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:32:25 +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[accuracy]]></category>
		<category><![CDATA[alpha alpha]]></category>
		<category><![CDATA[biases]]></category>
		<category><![CDATA[cmb experiments]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[cosmological parameters]]></category>
		<category><![CDATA[delta alpha]]></category>
		<category><![CDATA[fine structure constant]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[Hubble]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[recombination]]></category>
		<category><![CDATA[satellite experiment]]></category>
		<category><![CDATA[spectral index]]></category>
		<category><![CDATA[survey]]></category>
		<category><![CDATA[variation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/future-constraints-on-variations-of-the-fine-structure-constant-from-combined-cmb-and-weak-lensing-measurements-replacement-2/</guid>
		<description><![CDATA[We forecast the ability of future CMB and galaxy lensing surveys to constrain variations of the fine structure constant. We found that lensing data, as those expected from satellite experiments as Euclid could improve the constraint from future CMB experiments leading to a \Delta \alpha / \alpha = 8*10^{-4} accuracy. A variation of the fine [...]]]></description>
			<content:encoded><![CDATA[<p>We forecast the ability of future CMB and galaxy lensing surveys to constrain variations of the fine structure constant. We found that lensing data, as those expected from satellite experiments as Euclid could improve the constraint from future CMB experiments leading to a \Delta \alpha / \alpha = 8*10^{-4} accuracy. A variation of the fine structure constant \alpha is strongly degenerate with the Hubble constant H_0 and with inflationary parameters as the scalar spectral index n_s. These degeneracies may cause significant biases in the determination of cosmological parameters if a variation in \alpha as large as \sim 0.5 % is present at the epoch of recombination.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/future-constraints-on-variations-of-the-fine-structure-constant-from-combined-cmb-and-weak-lensing-measurements-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Effects of Leakage Neutral Particles on Shocks [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/effects-of-leakage-neutral-particles-on-shocks-replacement/</link>
		<comments>http://voxcharta.org/2012/02/22/effects-of-leakage-neutral-particles-on-shocks-replacement/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:32:09 +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[analytical solution]]></category>
		<category><![CDATA[approximation]]></category>
		<category><![CDATA[compression ratio]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[interstellar medium]]></category>
		<category><![CDATA[neutral particle]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[percents]]></category>
		<category><![CDATA[pickup ions]]></category>
		<category><![CDATA[precursor]]></category>
		<category><![CDATA[shock]]></category>
		<category><![CDATA[shock compression]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[supernova remnant]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/effects-of-leakage-neutral-particles-on-shocks-replacement/</guid>
		<description><![CDATA[The interstellar medium is not necessary fully ionized. When a shock propagates into the partially ionized medium, some neutral particles leak into the upstream region from the downstream region. In this paper, we investigate how leakage neutral particles affect the upstream structure of the shock and particle accelerations. By using four fluid approximations (upstream ions, [...]]]></description>
			<content:encoded><![CDATA[<p>The interstellar medium is not necessary fully ionized. When a shock propagates into the partially ionized medium, some neutral particles leak into the upstream region from the downstream region. In this paper, we investigate how leakage neutral particles affect the upstream structure of the shock and particle accelerations. By using four fluid approximations (upstream ions, upstream neutral particles, leakage neutral particles and pickup ions), we provide analytical solutions of the precursor structure due to leakage neutral particles. It is shown that the upstream flow is decelerated in the precursor and the shock compression ratio becomes smaller than that of the strong shock limit, but the total compression ratio is the same as that of the strong shock limit. Even if leakage of neutral particles is small (a few percents of upstream particles), this smaller compression ratio of the shock can explain steep gamma-ray spectra from young supernova remnants.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/effects-of-leakage-neutral-particles-on-shocks-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Mergers and ejections of black holes in globular clusters [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/mergers-and-ejections-of-black-holes-in-globular-clusters-replacement/</link>
		<comments>http://voxcharta.org/2012/02/22/mergers-and-ejections-of-black-holes-in-globular-clusters-replacement/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:31:55 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[algorithmic]]></category>
		<category><![CDATA[body simulation]]></category>
		<category><![CDATA[characteristic feature]]></category>
		<category><![CDATA[cluster model]]></category>
		<category><![CDATA[coalescence]]></category>
		<category><![CDATA[dense core]]></category>
		<category><![CDATA[eccentricity]]></category>
		<category><![CDATA[ejections]]></category>
		<category><![CDATA[energy loss]]></category>
		<category><![CDATA[globular cluster]]></category>
		<category><![CDATA[hellstrom]]></category>
		<category><![CDATA[merger]]></category>
		<category><![CDATA[mikkola]]></category>
		<category><![CDATA[neutron stars and black holes]]></category>
		<category><![CDATA[radiation energy]]></category>
		<category><![CDATA[schwarzschild radii]]></category>
		<category><![CDATA[segregation]]></category>
		<category><![CDATA[shrinkage]]></category>
		<category><![CDATA[subsystems]]></category>
		<category><![CDATA[velocities]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/mergers-and-ejections-of-black-holes-in-globular-clusters-replacement/</guid>
		<description><![CDATA[We report on results of fully consistent N-body simulations of globular cluster models with N = 100 000 members containing neutron stars and black holes. Using the improved `algorithmic regularization&#8217; method of Hellstrom and Mikkola for compact subsystems, the new code NBODY7 enables for the first time general relativistic coalescence to be achieved for post-Newtonian [...]]]></description>
			<content:encoded><![CDATA[<p>We report on results of fully consistent N-body simulations of globular cluster models with N = 100 000 members containing neutron stars and black holes. Using the improved `algorithmic regularization&#8217; method of Hellstrom and Mikkola for compact subsystems, the new code NBODY7 enables for the first time general relativistic coalescence to be achieved for post-Newtonian terms and realistic parameters. Following an early stage of mass segregation, a few black holes form a small dense core which usually leads to the formation of one dominant binary. The subsequent evolution by dynamical shrinkage involves the competing processes of ejection and mergers by radiation energy loss. Unless the binary is ejected, long-lived triple systems often exhibit Kozai cycles with extremely high inner eccentricity (e &gt; 0.999) which may terminate in coalescence at a few Schwarzschild radii. A characteristic feature is that ordinary stars as well as black holes and even BH binaries are ejected with high velocities. On the basis of the models studied so far, the results suggest a limited growth of a few remaining stellar mass black holes in globular clusters.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/mergers-and-ejections-of-black-holes-in-globular-clusters-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Lesser Role of Shear in Star Formation: Insight from the Galactic Ring Survey [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/the-lesser-role-of-shear-in-star-formation-insight-from-the-galactic-ring-survey-replacement/</link>
		<comments>http://voxcharta.org/2012/02/22/the-lesser-role-of-shear-in-star-formation-insight-from-the-galactic-ring-survey-replacement/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:31:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[clouds the clouds]]></category>
		<category><![CDATA[co line]]></category>
		<category><![CDATA[correlates]]></category>
		<category><![CDATA[critical surface]]></category>
		<category><![CDATA[dense core]]></category>
		<category><![CDATA[fragmentation]]></category>
		<category><![CDATA[galactic ring]]></category>
		<category><![CDATA[galactic star]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gravity]]></category>
		<category><![CDATA[insight]]></category>
		<category><![CDATA[molecular cloud]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[profile]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[surface density]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/the-lesser-role-of-shear-in-star-formation-insight-from-the-galactic-ring-survey-replacement/</guid>
		<description><![CDATA[We analyse the role played by shear in regulating star formation in the Galaxy on the scale of individual molecular clouds. The clouds are selected from the $^{13}$CO $J=1-0$ line of the Galactic Ring Survey. We estimate the shear parameter which is the ratio of a critical surface density for the clouds to be disrupted [...]]]></description>
			<content:encoded><![CDATA[<p>We analyse the role played by shear in regulating star formation in the Galaxy on the scale of individual molecular clouds. The clouds are selected from the $^{13}$CO $J=1-0$ line of the Galactic Ring Survey. We estimate the shear parameter which is the ratio of a critical surface density for the clouds to be disrupted by shear to their actual surface density. We find that for almost all molecular clouds considered in the sample, there is no evidence that shear is playing a significant role in opposing the effects of self-gravity. Furthermore, we find that the shear parameter of the clouds does not depend on their position in the Galaxy, which implies that shear can not explain the radial profiles of the Galactic star formation rates. We also find that for gravitationally bound clouds, higher shear parameters do not imply lower masses nor that the shear parameter correlates with the clouds level of fragmentation. Our results suggest that shear is playing only a minor role in affecting the rates at which gravitationally bound molecular clouds convert their gas into dense cores and thereafter into stars.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/the-lesser-role-of-shear-in-star-formation-insight-from-the-galactic-ring-survey-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Modulated Reheating and Large Non-Gaussianity in String Cosmology [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/22/modulated-reheating-and-large-non-gaussianity-in-string-cosmology-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/22/modulated-reheating-and-large-non-gaussianity-in-string-cosmology-cross-listing/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:31:23 +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[coupling]]></category>
		<category><![CDATA[decay rate]]></category>
		<category><![CDATA[degrees of freedom]]></category>
		<category><![CDATA[density perturbations]]></category>
		<category><![CDATA[different regions]]></category>
		<category><![CDATA[divisor]]></category>
		<category><![CDATA[energy field]]></category>
		<category><![CDATA[explicit example]]></category>
		<category><![CDATA[field theory]]></category>
		<category><![CDATA[fNL]]></category>
		<category><![CDATA[generic values]]></category>
		<category><![CDATA[Hubble]]></category>
		<category><![CDATA[kaehler]]></category>
		<category><![CDATA[low energy]]></category>
		<category><![CDATA[mass spectrum]]></category>
		<category><![CDATA[modulation]]></category>
		<category><![CDATA[primordial fluctuations]]></category>
		<category><![CDATA[string cosmology]]></category>
		<category><![CDATA[type iib]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/modulated-reheating-and-large-non-gaussianity-in-string-cosmology-cross-listing/</guid>
		<description><![CDATA[A generic feature of the known string inflationary models is that the same physics that makes the inflaton lighter than the Hubble scale during inflation often also makes other scalars this light. These scalars can acquire isocurvature fluctuations during inflation, and given that their VEVs determine the mass spectrum and the coupling constants of the [...]]]></description>
			<content:encoded><![CDATA[<p>A generic feature of the known string inflationary models is that the same physics that makes the inflaton lighter than the Hubble scale during inflation often also makes other scalars this light. These scalars can acquire isocurvature fluctuations during inflation, and given that their VEVs determine the mass spectrum and the coupling constants of the effective low-energy field theory, these fluctuations give rise to couplings and masses that are modulated from one Hubble patch to another. These seem just what is required to obtain primordial adiabatic fluctuations through conversion into density perturbations through the `modulation mechanism&#8217;, wherein reheating takes place with different efficiency in different regions of our Universe. Fluctuations generated in this way can generically produce non-gaussianity larger than obtained in single-field slow-roll inflation; potentially observable in the near future. We provide here the first explicit example of the modulation mechanism at work in string cosmology, within the framework of LARGE Volume Type-IIB string flux compactifications. The inflationary dynamics involves two light Kaehler moduli: a fibre divisor plays the role of the inflaton whose decay rate to visible sector degrees of freedom is modulated by the primordial fluctuations of a blow-up mode (which is made light by the use of poly-instanton corrections). We find the challenges of embedding the mechanism into a concrete UV completion constrains the properties of the non-gaussianity that is found, since for generic values of the underlying parameters, the model predicts a local bi-spectrum with fNL of order `a few&#8217;. However, a moderate tuning of the parameters gives also rise to explicit examples with fNL O(20) potentially observable by the Planck satellite.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/modulated-reheating-and-large-non-gaussianity-in-string-cosmology-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Nuclear symmetry energy and the r-mode instability of neutron stars [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/22/nuclear-symmetry-energy-and-the-r-mode-instability-of-neutron-stars-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/22/nuclear-symmetry-energy-and-the-r-mode-instability-of-neutron-stars-cross-listing/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:31:05 +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[brueckner]]></category>
		<category><![CDATA[conclusion]]></category>
		<category><![CDATA[core temperature]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[dependence]]></category>
		<category><![CDATA[equation of state]]></category>
		<category><![CDATA[field model]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[mass x]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[nuclear equation]]></category>
		<category><![CDATA[observational data]]></category>
		<category><![CDATA[radius]]></category>
		<category><![CDATA[slope parameter]]></category>
		<category><![CDATA[symmetry]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/nuclear-symmetry-energy-and-the-r-mode-instability-of-neutron-stars-cross-listing/</guid>
		<description><![CDATA[We analyze the role of the symmetry energy slope parameter $L$ on the {\it r}-mode instability of neutron stars. Our study is performed using the microscopic Brueckner&#8211;Hartree&#8211;Fock approach of the nuclear equation of state, and several phenomenological Skyrme forces and relativistic mean field models. Our results show that the {\it r}-mode instability region is smaller [...]]]></description>
			<content:encoded><![CDATA[<p>We analyze the role of the symmetry energy slope parameter $L$ on the {\it r}-mode instability of neutron stars. Our study is performed using the microscopic Brueckner&#8211;Hartree&#8211;Fock approach of the nuclear equation of state, and several phenomenological Skyrme forces and relativistic mean field models. Our results show that the {\it r}-mode instability region is smaller for those models which give larger values of $L$. The reason is that both bulk ($\xi$) and shear ($\eta$) viscosities increase with $L$ and, therefore, the damping of the mode is more efficient for the models with larger $L$. We show also that the dependence of both viscosities on $L$ can be described at each density by simple power-laws of the type $\xi=A_{\xi}L^{B_\xi}$ and $\eta=A_{\eta}L^{B_\eta}$. Using the measured spin frequency and the estimated core temperature of the pulsar in the low-mass X-ray binary 4U 1608-52, we conclude that observational data seems to favor larger values of $L$ if the radius of this object is in the range $11.5-12$(10-12) km and its mass $1.4M_\odot$($2M_\odot$). Outside this range it is not possible to draw any conclusion on $L$ from this pulsar.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/nuclear-symmetry-energy-and-the-r-mode-instability-of-neutron-stars-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Inflationary signatures of single-field models beyond slow-roll</title>
		<link>http://voxcharta.org/2012/02/21/inflationary-signatures-of-single-field-models-beyond-slow-roll/</link>
		<comments>http://voxcharta.org/2012/02/21/inflationary-signatures-of-single-field-models-beyond-slow-roll/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 02:07:28 +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 microwave background]]></category>
		<category><![CDATA[cosmological constraints]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[deviations]]></category>
		<category><![CDATA[early universe]]></category>
		<category><![CDATA[exact scale]]></category>
		<category><![CDATA[explicit example]]></category>
		<category><![CDATA[field model]]></category>
		<category><![CDATA[fluctuation]]></category>
		<category><![CDATA[ghost]]></category>
		<category><![CDATA[Hubble]]></category>
		<category><![CDATA[imprints]]></category>
		<category><![CDATA[inflation]]></category>
		<category><![CDATA[instabilities]]></category>
		<category><![CDATA[perturbation]]></category>
		<category><![CDATA[phase speed]]></category>
		<category><![CDATA[propagator]]></category>
		<category><![CDATA[rapid change]]></category>
		<category><![CDATA[signature]]></category>
		<category><![CDATA[spectral index]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/inflationary-signatures-of-single-field-models-beyond-slow-roll/</guid>
		<description><![CDATA[If the expansion of the early Universe was not purely de Sitter, the statistical imprints of the primordial density perturbation on the cosmic microwave background can be quite different from those following slow-roll inflation. In this paper we study the inflationary signatures of all single-field models not plagued by ghost-like instabilities. We assume small deviations [...]]]></description>
			<content:encoded><![CDATA[<p>If the expansion of the early Universe was not purely de Sitter, the statistical imprints of the primordial density perturbation on the cosmic microwave background can be quite different from those following slow-roll inflation. In this paper we study the inflationary signatures of all single-field models not plagued by ghost-like instabilities. We assume small deviations from exact scale-invariance, as supported by current cosmological constraints, allow for a rapid change of the Hubble parameter and the phase speed of scalar fluctuations. We obtain the propagator of scalar fluctuations and compute the bispectrum, keeping next-order corrections proportional to the deviation of the spectral index from unity. These theories offer an explicit example where the shape and scale dependences of the bispectrum are highly non-trivial for reasonable breaking of slow-roll.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/inflationary-signatures-of-single-field-models-beyond-slow-roll/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Loops formed by tidal tails as fossil records of a major merger</title>
		<link>http://voxcharta.org/2012/02/21/loops-formed-by-tidal-tails-as-fossil-records-of-a-major-merger/</link>
		<comments>http://voxcharta.org/2012/02/21/loops-formed-by-tidal-tails-as-fossil-records-of-a-major-merger/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 02:06:58 +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[bulge]]></category>
		<category><![CDATA[cosmological simulations]]></category>
		<category><![CDATA[disc galaxies]]></category>
		<category><![CDATA[fossil record]]></category>
		<category><![CDATA[free parameter]]></category>
		<category><![CDATA[gadget 2]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[merger]]></category>
		<category><![CDATA[NGC]]></category>
		<category><![CDATA[nucleus]]></category>
		<category><![CDATA[numerical simulation]]></category>
		<category><![CDATA[orbital parameters]]></category>
		<category><![CDATA[relic]]></category>
		<category><![CDATA[remnant]]></category>
		<category><![CDATA[spiral galaxy]]></category>
		<category><![CDATA[thin disc]]></category>
		<category><![CDATA[tidal tail]]></category>
		<category><![CDATA[warp]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/loops-formed-by-tidal-tails-as-fossil-records-of-a-major-merger/</guid>
		<description><![CDATA[Many haloes of nearby disc galaxies contain faint and extended features, including loops, which are often interpreted as relics of satellite infall in the main galaxy&#8217;s potential well. In most cases, however, the residual nucleus of the satellite is not seen, although it is predicted by numerical simulations. We test whether such faint and extended [...]]]></description>
			<content:encoded><![CDATA[<p>Many haloes of nearby disc galaxies contain faint and extended features, including loops, which are often interpreted as relics of satellite infall in the main galaxy&#8217;s potential well. In most cases, however, the residual nucleus of the satellite is not seen, although it is predicted by numerical simulations. We test whether such faint and extended features can be associated to gas-rich, major mergers, which may also lead to disc rebuilding and thus be a corner stone for the formation of spiral galaxies. Using the TreeSPH code GADGET-2, we model the formation of an almost bulge-less galaxy similar to NGC 5907 (B/T $\le$ 0.2) after a gas-rich major merger. We indeed find that 3:1 major mergers can form features similar to the loops found in many galactic haloes, including in NGC 5907, and can reproduce an extended thin disc, a bulge, as well as the pronounced warp of the gaseous disc. Even though it remains difficult to fully cover the large volume of free parameters, the present modelling of the loops in NGC 5907 proves that they could well be the result of a major merger. It has many advantages over the satellite infall scenario; e.g., it solves the problem of the visibility of the satellite remnant, and it may explain some additional features in the NGC 5907 halo, as well as some gas properties of this system. For orbital parameters derived from cosmological simulations, the loops in NGC 5907 can be reproduced by major mergers (3:1 to 5:1) and possibly by intermediate mergers (5:1 to 12:1). The major merger scenario thus challenges the minor merger one and could explain many properties that haloes of spiral galaxies have in common, including their red colours and the presence of faint extended features.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/loops-formed-by-tidal-tails-as-fossil-records-of-a-major-merger/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>An attractor for the dynamical state of the intracluster medium</title>
		<link>http://voxcharta.org/2012/02/21/an-attractor-for-the-dynamical-state-of-the-intracluster-medium/</link>
		<comments>http://voxcharta.org/2012/02/21/an-attractor-for-the-dynamical-state-of-the-intracluster-medium/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 02:06:38 +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[attractor]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[dynamical state]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[galaxy cluster]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[important information]]></category>
		<category><![CDATA[intensity profile]]></category>
		<category><![CDATA[intergalactic medium]]></category>
		<category><![CDATA[move towards]]></category>
		<category><![CDATA[numerical simulation]]></category>
		<category><![CDATA[perturbation]]></category>
		<category><![CDATA[ray radiation]]></category>
		<category><![CDATA[sz effect]]></category>
		<category><![CDATA[temperature profile]]></category>
		<category><![CDATA[universe]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/an-attractor-for-the-dynamical-state-of-the-intracluster-medium/</guid>
		<description><![CDATA[Galaxy clusters provide us with important information about the cosmology of our universe. Observations of the X-ray radiation or of the SZ effect allow us to measure the density and temperature of the hot intergalactic medium between the galaxies in a cluster, which then allow us to calculate the total mass of the galaxy cluster. [...]]]></description>
			<content:encoded><![CDATA[<p>Galaxy clusters provide us with important information about the cosmology of our universe. Observations of the X-ray radiation or of the SZ effect allow us to measure the density and temperature of the hot intergalactic medium between the galaxies in a cluster, which then allow us to calculate the total mass of the galaxy cluster. However, no simple connection between the density and the temperature profiles has been identified. Here we use controlled high-resolution numerical simulations to identify a relation between the density and temperature of the gas in equilibrated galaxy clusters. We demonstrate that the temperature-density relation is a real attractor, by showing that a wide range of equilibrated structures all move towards the attractor when perturbed and subsequently allowed to relax. For structures which have undergone sufficient perturbations for this connection to hold, one can therefore extract the mass profile directly from the X-ray intensity profile.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/an-attractor-for-the-dynamical-state-of-the-intracluster-medium/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Hubble constant and new discoveries in cosmology</title>
		<link>http://voxcharta.org/2012/02/21/the-hubble-constant-and-new-discoveries-in-cosmology/</link>
		<comments>http://voxcharta.org/2012/02/21/the-hubble-constant-and-new-discoveries-in-cosmology/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 02:06:14 +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[accurate measurement]]></category>
		<category><![CDATA[budget]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[curvature]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[determinations]]></category>
		<category><![CDATA[general relativity]]></category>
		<category><![CDATA[Hubble]]></category>
		<category><![CDATA[kavli institute]]></category>
		<category><![CDATA[Measurement]]></category>
		<category><![CDATA[new discovery]]></category>
		<category><![CDATA[participants]]></category>
		<category><![CDATA[particle astrophysics]]></category>
		<category><![CDATA[physics]]></category>
		<category><![CDATA[precision and accuracy]]></category>
		<category><![CDATA[stanford university]]></category>
		<category><![CDATA[universe]]></category>
		<category><![CDATA[validity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/the-hubble-constant-and-new-discoveries-in-cosmology/</guid>
		<description><![CDATA[We report the outcome of a 3-day workshop on the Hubble constant (H_0) that took place during February 6-8 2012 at the Kavli Institute for Particle Astrophysics and Cosmology, on the campus of Stanford University. The participants met to address the following questions. Are there compelling scientific reasons to obtain more precise and more accurate [...]]]></description>
			<content:encoded><![CDATA[<p>We report the outcome of a 3-day workshop on the Hubble constant (H_0) that took place during February 6-8 2012 at the Kavli Institute for Particle Astrophysics and Cosmology, on the campus of Stanford University. The participants met to address the following questions. Are there compelling scientific reasons to obtain more precise and more accurate measurements of H_0 than currently available? If there are, how can we achieve this goal? The answers that emerged from the workshop are (1) better measurements of H_0 provide critical independent constraints on dark energy, spatial curvature of the Universe, neutrino physics, and validity of general relativity, (2) a measurement of H_0 to 1% in both precision and accuracy, supported by rigorous error budgets, is within reach for several methods, and (3) multiple paths to independent determinations of H_0 are needed in order to access and control systematics.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/the-hubble-constant-and-new-discoveries-in-cosmology/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Stellar lifetime and ultraviolet properties of the old metal-rich Galactic open cluster NGC6791: a pathway to understand the UV upturn of elliptical galaxies</title>
		<link>http://voxcharta.org/2012/02/21/stellar-lifetime-and-ultraviolet-properties-of-the-old-metal-rich-galactic-open-cluster-ngc6791-a-pathway-to-understand-the-uv-upturn-of-elliptical-galaxies/</link>
		<comments>http://voxcharta.org/2012/02/21/stellar-lifetime-and-ultraviolet-properties-of-the-old-metal-rich-galactic-open-cluster-ngc6791-a-pathway-to-understand-the-uv-upturn-of-elliptical-galaxies/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 02:05:55 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[elliptical galaxy]]></category>
		<category><![CDATA[fanelli]]></category>
		<category><![CDATA[fuel consumption]]></category>
		<category><![CDATA[helium abundance]]></category>
		<category><![CDATA[infrared colors]]></category>
		<category><![CDATA[k color]]></category>
		<category><![CDATA[mg2]]></category>
		<category><![CDATA[minimum mass]]></category>
		<category><![CDATA[open cluster]]></category>
		<category><![CDATA[padova]]></category>
		<category><![CDATA[photometry]]></category>
		<category><![CDATA[star number]]></category>
		<category><![CDATA[stellar core]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[stellar spectra]]></category>
		<category><![CDATA[theoretical expectations]]></category>
		<category><![CDATA[ultraviolet properties]]></category>
		<category><![CDATA[upturn]]></category>
		<category><![CDATA[white dwarf]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/stellar-lifetime-and-ultraviolet-properties-of-the-old-metal-rich-galactic-open-cluster-ngc6791-a-pathway-to-understand-the-uv-upturn-of-elliptical-galaxies/</guid>
		<description><![CDATA[The evolutionary properties of the old metal-rich Galactic open cluster NGC6791 are assessed, based on deep UB photometry and 2Mass JK data. For 4739 stars in the cluster, bolometric luminosity and effective temperature have been derived from theoretical (U-B) and (J-K) color fitting. The derived H-R diagram has been matched with the UVBLUE grid of [...]]]></description>
			<content:encoded><![CDATA[<p>The evolutionary properties of the old metal-rich Galactic open cluster NGC6791 are assessed, based on deep UB photometry and 2Mass JK data. For 4739 stars in the cluster, bolometric luminosity and effective temperature have been derived from theoretical (U-B) and (J-K) color fitting. The derived H-R diagram has been matched with the UVBLUE grid of synthetic stellar spectra to obtain the integrated SED of the system, together with a full set UV (Fanelli) and optical (Lick) narrow-band indices. The cluster appears to be a fairly good proxy of standard elliptical galaxies, although with significantly bluer infrared colors, a shallower 4000A Balmer break, and a lower Mg2 index. The confirmed presence of a dozen hot stars, along their EHB evolution, leads the cluster SED to consistently match the properties of the most active UV-upturn galaxies, with 1.7+/-0.4% of the total bolometric luminosity emitted shortward of 2500A.   The cluster Helium abundance results Y=0.30 +/-0.04, while the Post-MS implied stellar lifetime from star number counts fairly agrees with the theoretical expectations from both the Padova and BASTI stellar tracks. A Post-MS fuel consumption of 0.43 +/- 0.01 M_sun is found for NGC6791 stars, in close agreement with the estimated mass of cluster He-rich white dwarfs. Such a tight figure may lead to suspect that a fraction of the cluster stellar population does actually not reach the minimum mass required to effectively ignite He in the stellar core.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/stellar-lifetime-and-ultraviolet-properties-of-the-old-metal-rich-galactic-open-cluster-ngc6791-a-pathway-to-understand-the-uv-upturn-of-elliptical-galaxies/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Rebirth of X-ray Emission from the Born-Again Planetary Nebula A 30</title>
		<link>http://voxcharta.org/2012/02/21/rebirth-of-x-ray-emission-from-the-born-again-planetary-nebula-a-30/</link>
		<comments>http://voxcharta.org/2012/02/21/rebirth-of-x-ray-emission-from-the-born-again-planetary-nebula-a-30/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 02:05:41 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[central star]]></category>
		<category><![CDATA[charge exchange]]></category>
		<category><![CDATA[diffuse emission]]></category>
		<category><![CDATA[ejecta]]></category>
		<category><![CDATA[mass loading]]></category>
		<category><![CDATA[neutral material]]></category>
		<category><![CDATA[planetary nebula]]></category>
		<category><![CDATA[poor material]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[soft x]]></category>
		<category><![CDATA[spatial properties]]></category>
		<category><![CDATA[spectral property]]></category>
		<category><![CDATA[stellar parameters]]></category>
		<category><![CDATA[stellar wind]]></category>
		<category><![CDATA[thermal pulse]]></category>
		<category><![CDATA[uv spectrum]]></category>
		<category><![CDATA[wind properties]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xmm newton]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/rebirth-of-x-ray-emission-from-the-born-again-planetary-nebula-a-30/</guid>
		<description><![CDATA[The planetary nebula (PN) A 30 is believed to have undergone a very late thermal pulse resulting in the ejection of knots of hydrogen-poor material. Using multi-epoch HST images we have detected the angular expansion of these knots and derived an age of 850+280-150 yr. To investigate the spectral and spatial properties of the soft [...]]]></description>
			<content:encoded><![CDATA[<p>The planetary nebula (PN) A 30 is believed to have undergone a very late thermal pulse resulting in the ejection of knots of hydrogen-poor material. Using multi-epoch HST images we have detected the angular expansion of these knots and derived an age of 850+280-150 yr. To investigate the spectral and spatial properties of the soft X-ray emission detected by ROSAT, we have obtained Chandra and XMM-Newton deep observations of A 30. The X-ray emission from A 30 can be separated into two components: a point-source at the central star and diffuse X-ray emission associated with the hydrogen-poor knots and the cloverleaf structure inside the nebular shell. To help us assess the role of the current stellar wind in powering this X-ray emission, we have determined the stellar parameters and wind properties of the central star of A 30 using a non-LTE model fit to its optical and UV spectrum. The spatial distribution and spectral properties of the diffuse X-ray emission is highly suggestive that it is generated by the post-born-again and present fast stellar winds interacting with the hydrogen-poor ejecta of the born-again event. Charge-exchange reactions between the ions of the stellar winds and neutral material of the born-again ejecta seem the most likely mechanism for the production of diffuse X-ray emission. Shock-heated plasma may also contribute to this emission, as the hydrogen-poor knots are ablated by the stellar winds, in which case efficient mass-loading of the stellar winds is needed to raise the density and damp the velocity of the stellar winds to reproduce the spectral properties of the diffuse emission. The origin of the X-ray emission from the central star of A 30 is puzzling: shocks in the present fast stellar wind and photospheric emission can be ruled out, while the development of a new, compact hot bubble confining the fast stellar wind seems implausible.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/rebirth-of-x-ray-emission-from-the-born-again-planetary-nebula-a-30/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Stellar Halos of Massive Elliptical Galaxies</title>
		<link>http://voxcharta.org/2012/02/21/the-stellar-halos-of-massive-elliptical-galaxies/</link>
		<comments>http://voxcharta.org/2012/02/21/the-stellar-halos-of-massive-elliptical-galaxies/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 02:05:04 +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[accretion]]></category>
		<category><![CDATA[arcsec]]></category>
		<category><![CDATA[chemical signature]]></category>
		<category><![CDATA[elliptical galaxy]]></category>
		<category><![CDATA[equivalent width]]></category>
		<category><![CDATA[gradient]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[integral field spectrograph]]></category>
		<category><![CDATA[mcdonald observatory]]></category>
		<category><![CDATA[metal absorption lines]]></category>
		<category><![CDATA[mgb]]></category>
		<category><![CDATA[order of magnitude]]></category>
		<category><![CDATA[radial dependence]]></category>
		<category><![CDATA[radii]]></category>
		<category><![CDATA[signal to noise ratio]]></category>
		<category><![CDATA[smith telescope]]></category>
		<category><![CDATA[star formation history]]></category>
		<category><![CDATA[stellar system]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/the-stellar-halos-of-massive-elliptical-galaxies/</guid>
		<description><![CDATA[We use the Mitchell Spectrograph (formerly VIRUS-P) on the McDonald Observatory 2.7m Harlan J. Smith Telescope to search for the chemical signatures of massive elliptical galaxy assembly. The Mitchell Spectrograph is an integral-field spectrograph with a uniquely wide field of view (107&#215;107 sq arcsec), allowing us to achieve remarkably high signal-to-noise ratios of ~20-70 per [...]]]></description>
			<content:encoded><![CDATA[<p>We use the Mitchell Spectrograph (formerly VIRUS-P) on the McDonald Observatory 2.7m Harlan J. Smith Telescope to search for the chemical signatures of massive elliptical galaxy assembly. The Mitchell Spectrograph is an integral-field spectrograph with a uniquely wide field of view (107&#215;107 sq arcsec), allowing us to achieve remarkably high signal-to-noise ratios of ~20-70 per pixel in radial bins of 2-2.5 times the effective radii of the eight galaxies in our sample. Focusing on a sample of massive elliptical galaxies with stellar velocity dispersions sigma* &gt; 150 km/s, we study the radial dependence in the equivalent widths (EWs) of key metal absorption lines. By twice the effective radius, the Mgb EWs have dropped by ~50%, and only a weak correlation between sigma* and Mgb EW remains. The Mgb EWs at large radii are comparable to those seen in the centers of elliptical galaxies that are approximately an order of magnitude less massive. We find that the well-known metallicity gradients often observed within an effective radius continue smoothly to 2.5R_e, while the abundance ratio gradients remain flat. Much like the halo of the Milky Way, the stellar halos of our galaxies have low metallicities and high alpha-abundance ratios, as expected for very old stars formed in small stellar systems. Our observations support a picture in which the outer parts of massive elliptical galaxies are built by the accretion of much smaller systems whose star formation history was truncated at early times.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/the-stellar-halos-of-massive-elliptical-galaxies/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Modelling fully convective stars in eclipsing binaries: KOI-126 and CM Draconis</title>
		<link>http://voxcharta.org/2012/02/21/modelling-fully-convective-stars-in-eclipsing-binaries-koi-126-and-cm-draconis/</link>
		<comments>http://voxcharta.org/2012/02/21/modelling-fully-convective-stars-in-eclipsing-binaries-koi-126-and-cm-draconis/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 02:04:45 +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[binary system]]></category>
		<category><![CDATA[boundary condition]]></category>
		<category><![CDATA[chemical composition]]></category>
		<category><![CDATA[consistent solution]]></category>
		<category><![CDATA[convection zone]]></category>
		<category><![CDATA[discrepancy]]></category>
		<category><![CDATA[draconis]]></category>
		<category><![CDATA[gyr]]></category>
		<category><![CDATA[koi]]></category>
		<category><![CDATA[length parameter]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[metallicity]]></category>
		<category><![CDATA[model atmosphere]]></category>
		<category><![CDATA[nextgen]]></category>
		<category><![CDATA[poor composition]]></category>
		<category><![CDATA[radii]]></category>
		<category><![CDATA[solar values]]></category>
		<category><![CDATA[surface boundary]]></category>
		<category><![CDATA[surface temperature]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/modelling-fully-convective-stars-in-eclipsing-binaries-koi-126-and-cm-draconis/</guid>
		<description><![CDATA[We present models of the components of the systems KOI-126 and CM Draconis, the two eclipsing binary systems known to date to contain stars with masses low enough to have fully convective interiors. We are able to model satisfactorily the system KOI-126, finding consistent solutions for the radii and surface temperatures of all three components, [...]]]></description>
			<content:encoded><![CDATA[<p>We present models of the components of the systems KOI-126 and CM Draconis, the two eclipsing binary systems known to date to contain stars with masses low enough to have fully convective interiors. We are able to model satisfactorily the system KOI-126, finding consistent solutions for the radii and surface temperatures of all three components, using a solar-like value of the mixing-length parameter \alpha in the convection zone, and PHOENIX NextGen 1D model atmospheres for the surface boundary conditions. Depending on the chemical composition, we estimate the age of the system to be in the range 3-5 Gyr. For CM Draconis, on the other hand, we cannot reconcile our models with the observed radii and T_eff using the current metal-poor composition estimate based on kinematics. Higher metallicities lessen but do not remove the discrepancy. We then explore the effect of varying the mixing length parameter \alpha. As previously noted in the literature, a reduced \alpha can be used as a simple measure of the lower convective efficiency due to rotation and induced magnetic fields. Our models show a sensitivity to \alpha (for \alpha &lt; 1.0) sufficient to partially account for the radius discrepancies. It is, however, impossible to reconcile the models with the observations on the basis of the effect of the reduced \alpha alone. We therefore suggest that the combined effects of high metallicity and \alpha reduction could explain the observations of CM Draconis. For example, increasing the metallicity of the system towards super-solar values (i.e. Z = 2 Z_sun) yields an agreement within 2 \sigma with \alpha = 1.0.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/modelling-fully-convective-stars-in-eclipsing-binaries-koi-126-and-cm-draconis/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Vsini-s for late-type stars from spectral synthesis in K-band region</title>
		<link>http://voxcharta.org/2012/02/21/vsini-s-for-late-type-stars-from-spectral-synthesis-in-k-band-region/</link>
		<comments>http://voxcharta.org/2012/02/21/vsini-s-for-late-type-stars-from-spectral-synthesis-in-k-band-region/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 02:04:25 +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[band features]]></category>
		<category><![CDATA[fwhm]]></category>
		<category><![CDATA[incorrect choice]]></category>
		<category><![CDATA[k band]]></category>
		<category><![CDATA[medium resolution]]></category>
		<category><![CDATA[model parameter]]></category>
		<category><![CDATA[observational data]]></category>
		<category><![CDATA[regime]]></category>
		<category><![CDATA[resolution spectra]]></category>
		<category><![CDATA[resolutions]]></category>
		<category><![CDATA[rotators]]></category>
		<category><![CDATA[spectral class]]></category>
		<category><![CDATA[spectral resolution]]></category>
		<category><![CDATA[spectral synthesis]]></category>
		<category><![CDATA[synthetic spectra]]></category>
		<category><![CDATA[type star]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/vsini-s-for-late-type-stars-from-spectral-synthesis-in-k-band-region/</guid>
		<description><![CDATA[We analyse medium-resolution spectra (R\sim 18000) of 19 late type dwarfs in order to determine vsini-s using synthetic rather than observational template spectra. For this purpose observational data around 2.2 $\mu$m of stars with spectral classes from G8V to M9.5V were modelled.   We find that the Na I (2.2062 and 2.2090 $\mu$m) and [...]]]></description>
			<content:encoded><![CDATA[<p>We analyse medium-resolution spectra (R\sim 18000) of 19 late type dwarfs in order to determine vsini-s using synthetic rather than observational template spectra. For this purpose observational data around 2.2 $\mu$m of stars with spectral classes from G8V to M9.5V were modelled.   We find that the Na I (2.2062 and 2.2090 $\mu$m) and $^{12}$CO 2-0 band features are modelled well enough to use for vsini determination without the need for a suitable observational template spectra. Within the limit of the resolution of our spectra, we use synthetic spectra templates to derive vsini values consistent with those derived in the optical regime using observed templates. We quantify the errors in our vsini determination due to incorrect choice of model parameters \Teff, log $g$, $v_{\rm micro}$, [Fe/H] or FWHM and show that they are typically less than 10 per cent. We note that the spectral resolution of our data(\sim 16 km/s) limited this study to relatively fast rotators and that resolutions of 60000 will required to access most late-type dwarfs.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/vsini-s-for-late-type-stars-from-spectral-synthesis-in-k-band-region/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>RX J1548.9+0851, a fossil cluster?</title>
		<link>http://voxcharta.org/2012/02/21/rx-j1548-90851-a-fossil-cluster/</link>
		<comments>http://voxcharta.org/2012/02/21/rx-j1548-90851-a-fossil-cluster/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 02:04:08 +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[distinct class]]></category>
		<category><![CDATA[elliptical galaxy]]></category>
		<category><![CDATA[ellipticals]]></category>
		<category><![CDATA[faint galaxy]]></category>
		<category><![CDATA[fossil]]></category>
		<category><![CDATA[full spectrum]]></category>
		<category><![CDATA[galaxy group]]></category>
		<category><![CDATA[galaxy population]]></category>
		<category><![CDATA[group member]]></category>
		<category><![CDATA[group membership]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[luminosity function]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[membership confirmation]]></category>
		<category><![CDATA[ray sources]]></category>
		<category><![CDATA[sdss]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[velocity dispersion]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/rx-j1548-90851-a-fossil-cluster/</guid>
		<description><![CDATA[Fossil galaxy groups are spatially extended X-ray sources with X-ray luminosities above L_X,bol &#62; 10^42 h_50^-2 ergs s^-1 and a central elliptical galaxy dominating the optical, the second-brightest galaxy being at least 2 magnitudes fainter in the R band. Whether these systems are a distinct class of objects resulting from exceptional formation and evolution histories [...]]]></description>
			<content:encoded><![CDATA[<p>Fossil galaxy groups are spatially extended X-ray sources with X-ray luminosities above L_X,bol &gt; 10^42 h_50^-2 ergs s^-1 and a central elliptical galaxy dominating the optical, the second-brightest galaxy being at least 2 magnitudes fainter in the R band. Whether these systems are a distinct class of objects resulting from exceptional formation and evolution histories is still unclear, mainly due to the small number of objects studied so far, mostly lacking spectroscopy of group members for group membership confirmation and a detailed kinematical analysis. To complement the scarce sample of spectroscopically studied fossils down to their faint galaxy populations, the fossil candidate RX J1548.9+0851 (z=0.072) is studied in this work. Our results are compared with existing data from fossils in the literature. We use ESO VLT VIMOS multi-object spectroscopy to determine redshifts of the faint galaxy population and study the luminosity-weighted dynamics and luminosity function of the system. The full-spectrum fitting package ULySS is used to determine ages and metallicities of group members. VIMOS imaging data are used to study the morphology of the central elliptical. We identify 40 group members spectroscopically within the central ~300 kpc of the system and find 31 additional redshifts from the literature, resulting in a total number of 54 spectroscopically confirmed group members within 1 Mpc. RX J1548.9+0851 is made up of two bright ellipticals in the central region with a magnitude gap of m_1,2 = 1.34 in the SDSS r&#8217; band leaving the definition of RX J1548.9+0851 being a fossil to the assumption of the virial radius. We find a luminosity-weighted velocity dispersion of 568 km s^-1 and a mass of ~2.5 x 10^14 M_sun for the system confirming previous studies that revealed fossils to be massive. (abridged)</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/rx-j1548-90851-a-fossil-cluster/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Magnetic field, differential rotation and activity of the hot-Jupiter hosting star HD 179949</title>
		<link>http://voxcharta.org/2012/02/21/magnetic-field-differential-rotation-and-activity-of-the-hot-jupiter-hosting-star-hd-179949/</link>
		<comments>http://voxcharta.org/2012/02/21/magnetic-field-differential-rotation-and-activity-of-the-hot-jupiter-hosting-star-hd-179949/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 02:03:33 +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[differential]]></category>
		<category><![CDATA[differential rotation]]></category>
		<category><![CDATA[dipole]]></category>
		<category><![CDATA[field configuration]]></category>
		<category><![CDATA[fluctuation]]></category>
		<category><![CDATA[gauss]]></category>
		<category><![CDATA[giant planet]]></category>
		<category><![CDATA[host star]]></category>
		<category><![CDATA[jupiter]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetosphere]]></category>
		<category><![CDATA[orbital period]]></category>
		<category><![CDATA[planet orbit]]></category>
		<category><![CDATA[polar rotation]]></category>
		<category><![CDATA[rotation period]]></category>
		<category><![CDATA[star hd]]></category>
		<category><![CDATA[stellar activity]]></category>
		<category><![CDATA[surface maps]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/magnetic-field-differential-rotation-and-activity-of-the-hot-jupiter-hosting-star-hd-179949/</guid>
		<description><![CDATA[HD 179949 is an F8V star, orbited by a giant planet at ~8 R* every 3.092514 days. The system was reported to undergo episodes of stellar activity enhancement modulated by the orbital period, interpreted as caused by Star-Planet Interactions (SPIs). One possible cause of SPIs is the large-scale magnetic field of the host star in [...]]]></description>
			<content:encoded><![CDATA[<p>HD 179949 is an F8V star, orbited by a giant planet at ~8 R* every 3.092514 days. The system was reported to undergo episodes of stellar activity enhancement modulated by the orbital period, interpreted as caused by Star-Planet Interactions (SPIs). One possible cause of SPIs is the large-scale magnetic field of the host star in which the close-in giant planet orbits.   In this paper we present spectropolarimetric observations of HD 179949 during two observing campaigns (2009 September and 2007 June). We detect a weak large-scale magnetic field of a few Gauss at the surface of the star. The field configuration is mainly poloidal at both observing epochs. The star is found to rotate differentially, with a surface rotation shear of dOmega=0.216\pm0.061 rad/d, corresponding to equatorial and polar rotation periods of 7.62\pm0.07 and 10.3\pm0.8 d respectively. The coronal field estimated by extrapolating the surface maps resembles a dipole tilted at ~70 degrees. We also find that the chromospheric activity of HD 179949 is mainly modulated by the rotation of the star, with two clear maxima per rotation period as expected from a highly tilted magnetosphere. In September 2009, we find that the activity of HD 179949 shows hints of low amplitude fluctuations with a period close to the beat period of the system.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/magnetic-field-differential-rotation-and-activity-of-the-hot-jupiter-hosting-star-hd-179949/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Resolved Structure and Dynamics of an Isolated Dwarf Galaxy: A VLT and Keck Spectroscopic Survey of WLM</title>
		<link>http://voxcharta.org/2012/02/21/the-resolved-structure-and-dynamics-of-an-isolated-dwarf-galaxy-a-vlt-and-keck-spectroscopic-survey-of-wlm/</link>
		<comments>http://voxcharta.org/2012/02/21/the-resolved-structure-and-dynamics-of-an-isolated-dwarf-galaxy-a-vlt-and-keck-spectroscopic-survey-of-wlm/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 02:03:17 +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[driven evolution]]></category>
		<category><![CDATA[dwarf galaxy]]></category>
		<category><![CDATA[dynamical evolution]]></category>
		<category><![CDATA[gaseous component]]></category>
		<category><![CDATA[giant branch stars]]></category>
		<category><![CDATA[giant molecular cloud]]></category>
		<category><![CDATA[internal feedback]]></category>
		<category><![CDATA[irregular galaxy]]></category>
		<category><![CDATA[keck ii]]></category>
		<category><![CDATA[light radius]]></category>
		<category><![CDATA[observational result]]></category>
		<category><![CDATA[radio data]]></category>
		<category><![CDATA[rotation curves]]></category>
		<category><![CDATA[spectroscopic data]]></category>
		<category><![CDATA[spectroscopic survey]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[stellar rotation]]></category>
		<category><![CDATA[velocity dispersion]]></category>
		<category><![CDATA[vertical structure]]></category>
		<category><![CDATA[wlm]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/the-resolved-structure-and-dynamics-of-an-isolated-dwarf-galaxy-a-vlt-and-keck-spectroscopic-survey-of-wlm/</guid>
		<description><![CDATA[We present spectroscopic data for 180 red giant branch stars in the isolated dwarf irregular galaxy WLM. Observations of the Calcium II triplet lines in spectra of RGB stars covering the entire galaxy were obtained with FORS2 at the VLT and DEIMOS on Keck II allowing us to derive velocities, metallicities, and ages for the [...]]]></description>
			<content:encoded><![CDATA[<p>We present spectroscopic data for 180 red giant branch stars in the isolated dwarf irregular galaxy WLM. Observations of the Calcium II triplet lines in spectra of RGB stars covering the entire galaxy were obtained with FORS2 at the VLT and DEIMOS on Keck II allowing us to derive velocities, metallicities, and ages for the stars. With accompanying photometric and radio data we have measured the structural parameters of the stellar and gaseous populations over the full galaxy. The stellar populations show an intrinsically thick configuration with $0.39 \leq q_{0} \leq 0.57$. The stellar rotation in WLM is measured to be $17 \pm 1$ km s$^{-1}$, however the ratio of rotation to pressure support for the stars is $V/\sigma \sim 1$, in contrast to the gas whose ratio is seven times larger. This, along with the structural data and alignment of the kinematic and photometric axes, suggests we are viewing WLM as a highly inclined oblate spheroid. Stellar rotation curves, corrected for asymmetric drift, are used to compute a dynamical mass of $4.3\pm 0.3\times10^{8} $M$_{\odot}$ at the half light radius ($r_{h} = 1656 \pm 49$ pc). The stellar velocity dispersion increases with stellar age in a manner consistent with giant molecular cloud and substructure interactions producing the heating in WLM. Coupled with WLM&#8217;s isolation, this suggests that the extended vertical structure of its stellar and gaseous components and increase in stellar velocity dispersion with age are due to internal feedback, rather than tidally driven evolution. These represent some of the first observational results from an isolated Local Group dwarf galaxy which can offer important constraints on how strongly internal feedback and secular processes modulate SF and dynamical evolution in low mass isolated objects.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/the-resolved-structure-and-dynamics-of-an-isolated-dwarf-galaxy-a-vlt-and-keck-spectroscopic-survey-of-wlm/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>First Science Observations with SOFIA/FORCAST: 6 to 37 micron Imaging of the Central Orion Nebula</title>
		<link>http://voxcharta.org/2012/02/21/first-science-observations-with-sofiaforcast-6-to-37-micron-imaging-of-the-central-orion-nebula/</link>
		<comments>http://voxcharta.org/2012/02/21/first-science-observations-with-sofiaforcast-6-to-37-micron-imaging-of-the-central-orion-nebula/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 02:03:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[airborne telescope]]></category>
		<category><![CDATA[first science]]></category>
		<category><![CDATA[infrared image]]></category>
		<category><![CDATA[micron]]></category>
		<category><![CDATA[orion nebula]]></category>
		<category><![CDATA[resolution observations]]></category>
		<category><![CDATA[science observations]]></category>
		<category><![CDATA[sofia]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/first-science-observations-with-sofiaforcast-6-to-37-micron-imaging-of-the-central-orion-nebula/</guid>
		<description><![CDATA[We present new mid-infrared images of the central region of the Orion Nebula using the newly commissioned SOFIA airborne telescope and its 5 &#8212; 40 micron camera FORCAST. The 37.1 micron images represent the highest resolution observations (&#60;4&#34;) ever obtained of this region at these wavelengths. After BN/KL (which is described in a separate letter [...]]]></description>
			<content:encoded><![CDATA[<p>We present new mid-infrared images of the central region of the Orion Nebula using the newly commissioned SOFIA airborne telescope and its 5 &#8212; 40 micron camera FORCAST. The 37.1 micron images represent the highest resolution observations (&lt;4&quot;) ever obtained of this region at these wavelengths. After BN/KL (which is described in a separate letter in this issue), the dominant source at all wavelengths except 37.1 micron is the Ney-Allen Nebula, a crescent-shaped extended source associated with theta 1D. The morphology of the Ney-Allen nebula in our images is consistent with the interpretation that it is ambient dust swept up by the stellar wind from theta 1D, as suggested by Smith et al. (2005). Our observations also reveal emission from two &quot;proplyds&quot; (proto-planetary disks), and a few embedded young stellar objects (YSOs; IRc9, and OMC1S IRS1, 2, and 10). The spectral energy distribution for IRc9 is presented and fitted with standard YSO models from Robitaille et al. (2007) to constrain the total luminosity, disk size, and envelope size. The diffuse, nebular emission we observe at all FORCAST wavelengths is most likely from the background photodissociation region (PDR) and shows structure that coincides roughly with H_alpha and [N II] emission. We conclude that the spatial variations in the diffuse emission are likely due to undulations in the surface of the background PDR.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/first-science-observations-with-sofiaforcast-6-to-37-micron-imaging-of-the-central-orion-nebula/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Constraints on the Formation of the Galactic Bulge from Na, Al, and Heavy Element Abundances in Plaut&#8217;s Field</title>
		<link>http://voxcharta.org/2012/02/21/constraints-on-the-formation-of-the-galactic-bulge-from-na-al-and-heavy-element-abundances-in-plauts-field/</link>
		<comments>http://voxcharta.org/2012/02/21/constraints-on-the-formation-of-the-galactic-bulge-from-na-al-and-heavy-element-abundances-in-plauts-field/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 02:02:49 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abundance]]></category>
		<category><![CDATA[clump stars]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[element]]></category>
		<category><![CDATA[extinction]]></category>
		<category><![CDATA[galactic bulge]]></category>
		<category><![CDATA[giant branch]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[Lithium]]></category>
		<category><![CDATA[metallicity]]></category>
		<category><![CDATA[ratios]]></category>
		<category><![CDATA[signal to noise]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectrograph]]></category>
		<category><![CDATA[spectrum synthesis]]></category>
		<category><![CDATA[Telescope]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/constraints-on-the-formation-of-the-galactic-bulge-from-na-al-and-heavy-element-abundances-in-plauts-field/</guid>
		<description><![CDATA[We report chemical abundances of Na, Al, Zr, La, Nd, and Eu for 39 red giant branch (RGB) stars and 23 potential inner disk red clump stars located in Plaut-s low extinction window. We also measure lithium for a super Li-rich RGB star. The abundances were determined by spectrum synthesis of high resolution (R~25,000), high [...]]]></description>
			<content:encoded><![CDATA[<p>We report chemical abundances of Na, Al, Zr, La, Nd, and Eu for 39 red giant branch (RGB) stars and 23 potential inner disk red clump stars located in Plaut-s low extinction window. We also measure lithium for a super Li-rich RGB star. The abundances were determined by spectrum synthesis of high resolution (R~25,000), high signal-to-noise (S/N~50-100 pixel-1) spectra obtained with the Blanco 4m telescope and Hydra multifiber spectrograph. For the bulge RGB stars, we find a general increase in the [Na/Fe] and [Na/Al] ratios with increasing metallicity, and a similar decrease in [La/Fe] and [Nd/Fe]. Additionally, the [Al/Fe] and [Eu/Fe] abundance trends almost identically follow those of the {\alpha}-elements, and the [Zr/Fe] ratios exhibit relatively little change with [Fe/H]. The consistently low [La/Eu] ratios of the RGB stars indicate that at least a majority of bulge stars formed rapidly (&lt;1 Gyr) and before the main s-process could become a significant pollution source. In contrast, we find that the potential inner disk clump stars exhibit abundance patterns more similar to those of the thin and thick disks. Comparisons between the abundance trends at different bulge locations suggest that the inner and outer bulge formed on similar timescales. However, we find evidence of some abundance differences between the most metal-poor and metal-rich stars in various bulge fields. The data also indicate that the halo may have had a more significant impact on the outer bulge initial composition than the inner bulge composition. The [Na/Fe] and to a lesser extent [La/Fe] abundances further indicate that the metal-poor bulge, at least at ~1 kpc from the Galactic center, and thick disk may not share an identical chemistry.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/constraints-on-the-formation-of-the-galactic-bulge-from-na-al-and-heavy-element-abundances-in-plauts-field/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Mid-Infrared Environments of High-Redshift Radio Galaxies</title>
		<link>http://voxcharta.org/2012/02/21/the-mid-infrared-environments-of-high-redshift-radio-galaxies/</link>
		<comments>http://voxcharta.org/2012/02/21/the-mid-infrared-environments-of-high-redshift-radio-galaxies/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 02:02:22 +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[environments]]></category>
		<category><![CDATA[galaxies at high redshift]]></category>
		<category><![CDATA[massive galaxy]]></category>
		<category><![CDATA[radio galaxy]]></category>
		<category><![CDATA[redshift radio]]></category>
		<category><![CDATA[Spitzer]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/the-mid-infrared-environments-of-high-redshift-radio-galaxies/</guid>
		<description><![CDATA[Taking advantage of the impressive sensitivity of Spitzer to detect massive galaxies at high redshift, we study the mid-infrared environments of powerful, high-redshift radio galaxies at 1.2&#60;z-0.1 (AB), in the fields of 48 radio galaxies at 1.2&#60;z1.2. Using a counts-in-cell analysis, we identify a field as overdense when 15 or more red IRAC sources are [...]]]></description>
			<content:encoded><![CDATA[<p>Taking advantage of the impressive sensitivity of Spitzer to detect massive galaxies at high redshift, we study the mid-infrared environments of powerful, high-redshift radio galaxies at 1.2&lt;z-0.1 (AB), in the fields of 48 radio galaxies at 1.2&lt;z1.2. Using a counts-in-cell analysis, we identify a field as overdense when 15 or more red IRAC sources are found within 1arcmin (i.e.,~0.5Mpc at 1.2&lt;z1.2.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/the-mid-infrared-environments-of-high-redshift-radio-galaxies/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Overdensities of 24um Sources in the Vicinities of High-Redshift Radio Galaxies</title>
		<link>http://voxcharta.org/2012/02/21/overdensities-of-24um-sources-in-the-vicinities-of-high-redshift-radio-galaxies/</link>
		<comments>http://voxcharta.org/2012/02/21/overdensities-of-24um-sources-in-the-vicinities-of-high-redshift-radio-galaxies/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 02:01:54 +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[environments]]></category>
		<category><![CDATA[radio galaxy]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[redshift radio]]></category>
		<category><![CDATA[statistical study]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/overdensities-of-24um-sources-in-the-vicinities-of-high-redshift-radio-galaxies/</guid>
		<description><![CDATA[We present a statistical study of the environments of 63 high-redshift radio galaxies (HzRGs) between redshifts 1&#60;z&#60;5.2, using the 24um, waveband of the MIPS instrument aboard the Spitzer Space Telescope. Using a counts-in-cell analysis, a statistically significant source overdensity is found in 1.75arcmin radius circular cells centred on the HzRGs when compared to reference fields. [...]]]></description>
			<content:encoded><![CDATA[<p>We present a statistical study of the environments of 63 high-redshift radio galaxies (HzRGs) between redshifts 1&lt;z&lt;5.2, using the 24um, waveband of the MIPS instrument aboard the Spitzer Space Telescope. Using a counts-in-cell analysis, a statistically significant source overdensity is found in 1.75arcmin radius circular cells centred on the HzRGs when compared to reference fields. We report an average overdensity of delta (= {N}_{targets} / {N}_{reference}) = 2.2 +/- 1.2 at a flux density cut of f24um=0.3mJy. This result implies that HzRGs are likely to lie in protoclusters of active and star-forming galaxies at high redshift. Over 95% of our targeted HzRGs lie in higher than average density fields. Further, 20 (32%) of our selected fields are found to be overdense to at least a 3sigma significance, of which 9 are newly identified protocluster candidates. We observe a weak correlation between redshift and 24um, source density, and discuss the populations being probed at different redshifts. In our uniformly selected sample, which was designed to cover two orders of magnitude in radio luminosity throughout z=1-4, we find that the 24um, source density does not depend on radio luminosity. We also compare this result with recent work describing IRAC source overdensities around the same HzRGs and find correlations between the results.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/overdensities-of-24um-sources-in-the-vicinities-of-high-redshift-radio-galaxies/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>3-D Monte Carlo radiative transfer calculation of resonance line formation in the inhomogeneous expanding stellar wind</title>
		<link>http://voxcharta.org/2012/02/21/3-d-monte-carlo-radiative-transfer-calculation-of-resonance-line-formation-in-the-inhomogeneous-expanding-stellar-wind/</link>
		<comments>http://voxcharta.org/2012/02/21/3-d-monte-carlo-radiative-transfer-calculation-of-resonance-line-formation-in-the-inhomogeneous-expanding-stellar-wind/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:59:38 +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[3 d shapes]]></category>
		<category><![CDATA[clump]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[determinations]]></category>
		<category><![CDATA[line formation]]></category>
		<category><![CDATA[mass loss]]></category>
		<category><![CDATA[Monte Carlo]]></category>
		<category><![CDATA[observation]]></category>
		<category><![CDATA[opacity]]></category>
		<category><![CDATA[radiative transfer]]></category>
		<category><![CDATA[resonance line]]></category>
		<category><![CDATA[stellar wind]]></category>
		<category><![CDATA[variation]]></category>
		<category><![CDATA[velocity dispersion]]></category>
		<category><![CDATA[velocity field]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/3-d-monte-carlo-radiative-transfer-calculation-of-resonance-line-formation-in-the-inhomogeneous-expanding-stellar-wind/</guid>
		<description><![CDATA[We study the effects of optically thick clumps, non-void inter-clump medium, variation of the onset of clumping, and velocity dispersion inside clumps on the formation of resonance lines. For this purpose we developed a full 3-D Monte Carlo Radiative Transfer (MCRT) code that is able to handle 3-D shapes of clumps and arbitrary 3-D velocity [...]]]></description>
			<content:encoded><![CDATA[<p>We study the effects of optically thick clumps, non-void inter-clump medium, variation of the onset of clumping, and velocity dispersion inside clumps on the formation of resonance lines. For this purpose we developed a full 3-D Monte Carlo Radiative Transfer (MCRT) code that is able to handle 3-D shapes of clumps and arbitrary 3-D velocity fields. The method we developed allows us to take into account contributions from density and velocity wind inhomogeneities to the total opacity very precisely. The first comparison with observation shows that 3-D density and velocity wind inhomogeneities have a very strong influence on the resonance line formation, and that they have to be accounted for in order to obtain reliable mass-loss rate determinations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/3-d-monte-carlo-radiative-transfer-calculation-of-resonance-line-formation-in-the-inhomogeneous-expanding-stellar-wind/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Physical Processes of Interstellar Turbulence</title>
		<link>http://voxcharta.org/2012/02/21/physical-processes-of-interstellar-turbulence/</link>
		<comments>http://voxcharta.org/2012/02/21/physical-processes-of-interstellar-turbulence/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:58:54 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[clump]]></category>
		<category><![CDATA[cold gas]]></category>
		<category><![CDATA[collapse]]></category>
		<category><![CDATA[compressions]]></category>
		<category><![CDATA[dense molecular clouds]]></category>
		<category><![CDATA[density fluctuations]]></category>
		<category><![CDATA[heating and cooling]]></category>
		<category><![CDATA[interstellar turbulence]]></category>
		<category><![CDATA[ism]]></category>
		<category><![CDATA[mach number]]></category>
		<category><![CDATA[numerical simulation]]></category>
		<category><![CDATA[physical processes]]></category>
		<category><![CDATA[radiative]]></category>
		<category><![CDATA[shock wave]]></category>
		<category><![CDATA[sound speed]]></category>
		<category><![CDATA[spiral arm]]></category>
		<category><![CDATA[temperature range]]></category>
		<category><![CDATA[thermal instability]]></category>
		<category><![CDATA[thermal processes]]></category>
		<category><![CDATA[velocity dispersion]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/physical-processes-of-interstellar-turbulence/</guid>
		<description><![CDATA[I discuss the role of self-gravity and radiative heating and cooling in shaping the nature of the turbulence in the interstellar medium (ISM) of our galaxy. The heating and cooling cause it to be highly compressible, and, in some regimes of density and temperature, to become thermally unstable, tending to spontaneously segregate into warm/diffuse and [...]]]></description>
			<content:encoded><![CDATA[<p>I discuss the role of self-gravity and radiative heating and cooling in shaping the nature of the turbulence in the interstellar medium (ISM) of our galaxy. The heating and cooling cause it to be highly compressible, and, in some regimes of density and temperature, to become thermally unstable, tending to spontaneously segregate into warm/diffuse and cold/dense phases. On the other hand, turbulence is an inherently mixing process, tending to replenish the density and temperature ranges that would be forbidden under thermal processes alone. The turbulence in the ionized ISM appears to be transonic (i.e, with Mach numbers $\Ms \sim 1$), and thus to behave essentially incompressibly. However, in the neutral medium, thermal instability causes the sound speed of the gas to fluctuate by up to factors of $\sim 30$, and thus the flow can be highly supersonic with respect to the dense/cold gas, although numerical simulations suggest that this behavior corresponds more to the ensemble of cold clumps than to the clumps&#8217; internal velocity dispersion. Finally, coherent large-scale compressions in the warm neutral medium (induced by, say, the passage of spiral arms or by supernova shock waves) can produce large, dense molecular clouds that are subject to their own self-gravity, and begin to contract gravitationally. Because they are populated by nonlinear density fluctuations, whose local free-fall times are significantly smaller than that of the whole cloud, the fluctuations terminate their collapse earlier, giving rise to a regime of hierarchical gravitational fragmentation, with small-scale collapses occurring within larger-scale ones. Thus, the &#8220;turbulence&#8221; in molecular clouds may be dominated by a gravitationally contracting component at all scales.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/physical-processes-of-interstellar-turbulence/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Gamma-Ray Blazar PKS 0208-512, a Multi-Wavelength Investigation</title>
		<link>http://voxcharta.org/2012/02/21/the-gamma-ray-blazar-pks-0208-512-a-multi-wavelength-investigation/</link>
		<comments>http://voxcharta.org/2012/02/21/the-gamma-ray-blazar-pks-0208-512-a-multi-wavelength-investigation/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:58:34 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[AGN]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[flux density]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[inclusion]]></category>
		<category><![CDATA[jets]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[map]]></category>
		<category><![CDATA[optical depth]]></category>
		<category><![CDATA[period]]></category>
		<category><![CDATA[pks]]></category>
		<category><![CDATA[radio frequency]]></category>
		<category><![CDATA[time series analysis]]></category>
		<category><![CDATA[vlbi data]]></category>
		<category><![CDATA[wavelength]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/the-gamma-ray-blazar-pks-0208-512-a-multi-wavelength-investigation/</guid>
		<description><![CDATA[The gamma-ray blazar PKS 0208-512 has shown strong periods of flaring, at all frequencies from radio to gamma-ray. This has led to its inclusion in the TANAMI project, which tracks the jets of southern AGN using VLBI as well as supporting flux density monitoring programs. Time series analysis of the light curves generated by such [...]]]></description>
			<content:encoded><![CDATA[<p>The gamma-ray blazar PKS 0208-512 has shown strong periods of flaring, at all frequencies from radio to gamma-ray. This has led to its inclusion in the TANAMI project, which tracks the jets of southern AGN using VLBI as well as supporting flux density monitoring programs. Time series analysis of the light curves generated by such monitoring is presented and discussed and VLBI maps of the source are used to show the evolution in the jet. A frequency dependent lag is observed between flaring at different radio frequencies which does not appear to correspond to purely optical depth effects. Major flaring at gamma-ray frequencies appears to be preceded by a new component in the jet seen in our VLBI data.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/the-gamma-ray-blazar-pks-0208-512-a-multi-wavelength-investigation/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Compact continuum source-finding for next generation radio surveys</title>
		<link>http://voxcharta.org/2012/02/21/compact-continuum-source-finding-for-next-generation-radio-surveys/</link>
		<comments>http://voxcharta.org/2012/02/21/compact-continuum-source-finding-for-next-generation-radio-surveys/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:58:16 +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[aegean]]></category>
		<category><![CDATA[algorithm]]></category>
		<category><![CDATA[blind radio]]></category>
		<category><![CDATA[completeness]]></category>
		<category><![CDATA[continuum source]]></category>
		<category><![CDATA[daily basis]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[generation radio]]></category>
		<category><![CDATA[kernel]]></category>
		<category><![CDATA[next generation]]></category>
		<category><![CDATA[radio astronomy]]></category>
		<category><![CDATA[radio source]]></category>
		<category><![CDATA[radio survey]]></category>
		<category><![CDATA[reliability]]></category>
		<category><![CDATA[source catalogue]]></category>
		<category><![CDATA[square kilometer array]]></category>
		<category><![CDATA[Telescope]]></category>
		<category><![CDATA[transients]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/compact-continuum-source-finding-for-next-generation-radio-surveys/</guid>
		<description><![CDATA[We present a detailed analysis of four of the most widely used radio source finding packages in radio astronomy, and a program being developed for the Australian Square Kilometer Array Pathfinder (ASKAP) telescope. The four packages; SExtractor, SFind, IMSAD and Selavy are shown to produce source catalogues with high completeness and reliability. In this paper [...]]]></description>
			<content:encoded><![CDATA[<p>We present a detailed analysis of four of the most widely used radio source finding packages in radio astronomy, and a program being developed for the Australian Square Kilometer Array Pathfinder (ASKAP) telescope. The four packages; SExtractor, SFind, IMSAD and Selavy are shown to produce source catalogues with high completeness and reliability. In this paper we analyse the small fraction (~1%) of cases in which these packages do not perform well. This small fraction of sources will be of concern for the next generation of radio surveys which will produce many thousands of sources on a daily basis, in particular for blind radio transients surveys. From our analysis we identify the ways in which the underlying source finding algorithms fail. We demonstrate a new source finding algorithm Aegean, based on the application of a Laplacian kernel, which can avoid these problems and can produce complete and reliable source catalogues for the next generation of radio surveys.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/compact-continuum-source-finding-for-next-generation-radio-surveys/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Testing Gravity with the Stacked Phase Space around Galaxy Clusters</title>
		<link>http://voxcharta.org/2012/02/21/testing-gravity-with-the-stacked-phase-space-around-galaxy-clusters/</link>
		<comments>http://voxcharta.org/2012/02/21/testing-gravity-with-the-stacked-phase-space-around-galaxy-clusters/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:57:56 +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[body simulation]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[field phase]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[galaxy cluster]]></category>
		<category><![CDATA[general relativity]]></category>
		<category><![CDATA[gravity]]></category>
		<category><![CDATA[orders of magnitude]]></category>
		<category><![CDATA[phase space density]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[redshift survey]]></category>
		<category><![CDATA[scales]]></category>
		<category><![CDATA[velocity field]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/testing-gravity-with-the-stacked-phase-space-around-galaxy-clusters/</guid>
		<description><![CDATA[In General Relativity, the average velocity field of dark matter around galaxy clusters is uniquely determined by the mass profile. The latter can be measured through weak lensing. We propose a new method of measuring the velocity field (phase space density) by stacking redshifts of surrounding galaxies from a spectroscopic sample. In combination with lensing, [...]]]></description>
			<content:encoded><![CDATA[<p>In General Relativity, the average velocity field of dark matter around galaxy clusters is uniquely determined by the mass profile. The latter can be measured through weak lensing. We propose a new method of measuring the velocity field (phase space density) by stacking redshifts of surrounding galaxies from a spectroscopic sample. In combination with lensing, this yields a direct test of gravity on scales of 1-30 Mpc. Using N-body simulations, we show that this method can improve upon current constraints by several orders of magnitude when applied to upcoming imaging and redshift surveys.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/testing-gravity-with-the-stacked-phase-space-around-galaxy-clusters/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>ATLBS Extended Source Sample: The evolution in radio source morphology with flux density</title>
		<link>http://voxcharta.org/2012/02/21/atlbs-extended-source-sample-the-evolution-in-radio-source-morphology-with-flux-density/</link>
		<comments>http://voxcharta.org/2012/02/21/atlbs-extended-source-sample-the-evolution-in-radio-source-morphology-with-flux-density/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:57:02 +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[activity cycles]]></category>
		<category><![CDATA[asymmetry]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[density limits]]></category>
		<category><![CDATA[extended radio]]></category>
		<category><![CDATA[extent]]></category>
		<category><![CDATA[faint radio]]></category>
		<category><![CDATA[giant radio]]></category>
		<category><![CDATA[lobes]]></category>
		<category><![CDATA[mjy]]></category>
		<category><![CDATA[morphological properties]]></category>
		<category><![CDATA[mpc]]></category>
		<category><![CDATA[radio galaxy]]></category>
		<category><![CDATA[radio source]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[relative abundance]]></category>
		<category><![CDATA[surface brightness]]></category>
		<category><![CDATA[type structure]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/atlbs-extended-source-sample-the-evolution-in-radio-source-morphology-with-flux-density/</guid>
		<description><![CDATA[Based on the ATLBS survey we present a sample of extended radio sources and derive morphological properties of faint radio sources. 119 radio galaxies form the ATLBS-Extended Source Sample (ATLBS-ESS) consisting of all sources exceeding 30&#8243; in extent and integrated flux densities exceeding 1 mJy. We give structural details along with information on galaxy identifications [...]]]></description>
			<content:encoded><![CDATA[<p>Based on the ATLBS survey we present a sample of extended radio sources and derive morphological properties of faint radio sources. 119 radio galaxies form the ATLBS-Extended Source Sample (ATLBS-ESS) consisting of all sources exceeding 30&#8243; in extent and integrated flux densities exceeding 1 mJy. We give structural details along with information on galaxy identifications and source classifications. The ATLBS-ESS, unlike samples with higher flux-density limits, has almost equal fractions of FR-I and FR-II radio galaxies with a large fraction of the FR-I population exhibiting 3C31-type structures. Significant asymmetry in lobe extents appears to be a common occurrence in the ATLBS-ESS FR-I sources compared to FR-II sources. We present a sample of 22 FR-Is at z&gt;0.5 with good structural information. The detection of several giant radio sources, with size exceeding 0.7 Mpc, at z&gt;1 suggests that giant radio sources are not less common at high redshifts. The ESS also includes a sample of 28 restarted radio galaxies. The relative abundance of dying and restarting sources is indicative of a model where radio sources undergo episodic activity in which an active phase is followed by a brief dying phase that terminates with restarting of the central activity; in any massive elliptical a few such activity cycles wherein adjacent events blend may constitute the lifetime of a radio source and such bursts of blended activity cycles may be repeated over the age of the host. The ATLBS-ESS includes a 2-Mpc giant radio galaxy with the lowest surface brightness lobes known to date.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/atlbs-extended-source-sample-the-evolution-in-radio-source-morphology-with-flux-density/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Revision of Solar Spicule Classification</title>
		<link>http://voxcharta.org/2012/02/21/revision-of-solar-spicule-classification/</link>
		<comments>http://voxcharta.org/2012/02/21/revision-of-solar-spicule-classification/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:56:49 +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[3d motion]]></category>
		<category><![CDATA[chromosphere]]></category>
		<category><![CDATA[corona]]></category>
		<category><![CDATA[downward motion]]></category>
		<category><![CDATA[dozens]]></category>
		<category><![CDATA[dynamic properties]]></category>
		<category><![CDATA[fades]]></category>
		<category><![CDATA[key role]]></category>
		<category><![CDATA[lifetime]]></category>
		<category><![CDATA[magnetic structure]]></category>
		<category><![CDATA[quiet sun]]></category>
		<category><![CDATA[slit]]></category>
		<category><![CDATA[space time]]></category>
		<category><![CDATA[spicule]]></category>
		<category><![CDATA[subject headings]]></category>
		<category><![CDATA[time plot]]></category>
		<category><![CDATA[transition region]]></category>
		<category><![CDATA[wavelength]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/revision-of-solar-spicule-classification/</guid>
		<description><![CDATA[Solar spicules are the fundamental magnetic structures in the chromosphere and considered to play a key role in channelling the chromosphere and corona. Recently, it was suggested by De Pontieu et al. that there were two types of spicules with very different dynamic properties, which were detected by space- time plot technique in the Ca [...]]]></description>
			<content:encoded><![CDATA[<p>Solar spicules are the fundamental magnetic structures in the chromosphere and considered to play a key role in channelling the chromosphere and corona. Recently, it was suggested by De Pontieu et al. that there were two types of spicules with very different dynamic properties, which were detected by space- time plot technique in the Ca ii H line (3968 A) wavelength from Hinode/SOT observations. &#8216;Type I&#8217; spicule, with a 3-7 minute lifetime, undergoes a cycle of upward and downward motion; in contrast, &#8216;Type II&#8217; spicule fades away within dozens of seconds, without descending phase. We are motivated by the fact that for a spicule with complicated 3D motion, the space-time plot, which is made through a slit on a fixed position, could not match the spicule behavior all the time and might lose its real life story. By revisiting the same data sets, we identify and trace 105 and 102 spicules in quiet sun (QS) and coronal hole (CH), respectively, and obtain their statistical dynamic properties. First, we have not found a single convincing example of &#8216;Type II&#8217; spicules. Secondly, more than 60% of the identified spicules in each region show a complete cycle, i.e., majority spicules are &#8216;Type I&#8217;. Thirdly, the lifetime of spicules in QS and CH are 148 s and 112 s, respectively, but there is no fundamental lifetime difference between the spicules in QS and CH reported earlier. Therefore, the suggestion of coronal heating by &#8216;Type II&#8217; spicules should be taken with cautions. Subject headings: Sun: chromosphere Sun:transition region Sun:corona</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/revision-of-solar-spicule-classification/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>On the Anisotropy of E0 &gt;= 5.5$\times$1019 eV Cosmic Rays according to Data of the Pierre Auger Collaboration</title>
		<link>http://voxcharta.org/2012/02/21/on-the-anisotropy-of-e0-5-5times1019-ev-cosmic-rays-according-to-data-of-the-pierre-auger-collaboration/</link>
		<comments>http://voxcharta.org/2012/02/21/on-the-anisotropy-of-e0-5-5times1019-ev-cosmic-rays-according-to-data-of-the-pierre-auger-collaboration/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:56:36 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[anisotropy]]></category>
		<category><![CDATA[bearing]]></category>
		<category><![CDATA[collaboration]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[galactic coordinates]]></category>
		<category><![CDATA[great attractor]]></category>
		<category><![CDATA[local group]]></category>
		<category><![CDATA[pierre auger]]></category>
		<category><![CDATA[radio galaxy]]></category>
		<category><![CDATA[radius]]></category>
		<category><![CDATA[solid angle]]></category>
		<category><![CDATA[supercluster of galaxies]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/on-the-anisotropy-of-e0-5-5times1019-ev-cosmic-rays-according-to-data-of-the-pierre-auger-collaboration/</guid>
		<description><![CDATA[The Pierre Auger Collaboration discovered, in a solid angle of radius about 18\degree, a local group of cosmic rays having energies in the region E0 \geq 5.5\times1019 eV and coming from the region of the Gen A radio galaxy, whose galactic coordinates are lG = 309.5\degree and bG = 19.4\degree. Near it, there is the [...]]]></description>
			<content:encoded><![CDATA[<p>The Pierre Auger Collaboration discovered, in a solid angle of radius about 18\degree, a local group of cosmic rays having energies in the region E0 \geq 5.5\times1019 eV and coming from the region of the Gen A radio galaxy, whose galactic coordinates are lG = 309.5\degree and bG = 19.4\degree. Near it, there is the Centaur supercluster of galaxies, its galactic coordinates being lG = 302.4\degree and bG = 21.6\degree. It is noteworthy that the Great Attractor, which may have a direct bearing on the observed picture, is also there.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/on-the-anisotropy-of-e0-5-5times1019-ev-cosmic-rays-according-to-data-of-the-pierre-auger-collaboration/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>New activity in the large circumstellar disk of the Be-shell star 48 Lib</title>
		<link>http://voxcharta.org/2012/02/21/new-activity-in-the-large-circumstellar-disk-of-the-be-shell-star-48-lib/</link>
		<comments>http://voxcharta.org/2012/02/21/new-activity-in-the-large-circumstellar-disk-of-the-be-shell-star-48-lib/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:56:16 +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[absorption]]></category>
		<category><![CDATA[asymmetry]]></category>
		<category><![CDATA[broad band]]></category>
		<category><![CDATA[component structure]]></category>
		<category><![CDATA[core]]></category>
		<category><![CDATA[deg]]></category>
		<category><![CDATA[density gas]]></category>
		<category><![CDATA[disk evolution]]></category>
		<category><![CDATA[high density]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[interferometry]]></category>
		<category><![CDATA[line profile]]></category>
		<category><![CDATA[metal shell]]></category>
		<category><![CDATA[nineties]]></category>
		<category><![CDATA[polarimetric observations]]></category>
		<category><![CDATA[position angle]]></category>
		<category><![CDATA[radial velocity]]></category>
		<category><![CDATA[radial velocity variations]]></category>
		<category><![CDATA[spectral resolution]]></category>
		<category><![CDATA[stellar radii]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/new-activity-in-the-large-circumstellar-disk-of-the-be-shell-star-48-lib/</guid>
		<description><![CDATA[Spectroscopic, polarimetric, and high spectral resolution interferometric data covering the period 1995-2011 are analyzed to document the transition into a new phase of circumstellar disk activity in the classical Be-shell star 48 Lib. The long-term disk evolution is described using the V/R ratio of the violet and red emission components of H alpha and Br [...]]]></description>
			<content:encoded><![CDATA[<p>Spectroscopic, polarimetric, and high spectral resolution interferometric data covering the period 1995-2011 are analyzed to document the transition into a new phase of circumstellar disk activity in the classical Be-shell star 48 Lib. The long-term disk evolution is described using the V/R ratio of the violet and red emission components of H alpha and Br gamma, radial velocities and profiles of He I and optical metal shell lines, multi-band BVRI polarimetry, broad-band and high-resolution interferometric visibilities and phases. Spectroscopic signatures of disk asymmetries in 48 Lib vanished in the late nineties but recovered some time between 2004 and 2007. Variations in the radial velocity and line profile of conventional shell lines correlate with the V/R behavior. They are shared by narrow absorption cores superimposed on otherwise seemingly photospheric He I lines, which may form in high-density gas at the inner disk close to the photosphere. Large radial velocity variations continued also during the V/R-quiet years. The broad H-band interferometry gives a disk diameter of (1.72+-0.2) mas (equivalent to 15 stellar radii), position angle of the disk (50+-9) deg and a relatively low disk flattening of 1.66+-0.3. Within the errors the same disk position angle is derived from polarimetric observations and from photocenter shifts across Br gamma. The high-resolution interferometric visibility and phase profiles show a double or even multiple-component structure. A preliminary estimate based on the size of the Br gamma emitting region indicates a large diameter for the disk (tens of stellar radii).</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/new-activity-in-the-large-circumstellar-disk-of-the-be-shell-star-48-lib/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Generation of strong magnetic fields via the small-scale dynamo during the formation of the first stars</title>
		<link>http://voxcharta.org/2012/02/21/generation-of-strong-magnetic-fields-via-the-small-scale-dynamo-during-the-formation-of-the-first-stars/</link>
		<comments>http://voxcharta.org/2012/02/21/generation-of-strong-magnetic-fields-via-the-small-scale-dynamo-during-the-formation-of-the-first-stars/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:55:56 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[amplification]]></category>
		<category><![CDATA[central core region]]></category>
		<category><![CDATA[computer simulation]]></category>
		<category><![CDATA[dynamo]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[gravitational collapse]]></category>
		<category><![CDATA[grid cell]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[jeans]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[mass distribution]]></category>
		<category><![CDATA[motion]]></category>
		<category><![CDATA[primordial star]]></category>
		<category><![CDATA[resolution computer]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[stars in the universe]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/generation-of-strong-magnetic-fields-via-the-small-scale-dynamo-during-the-formation-of-the-first-stars/</guid>
		<description><![CDATA[Here we summarize our recent results of high-resolution computer simulations on the turbulent amplification of weak magnetic seed fields showing that such fields will be exponentially amplified also during the gravitational collapse reminiscent to the situation during primordial star formation. The exponential magnetic field amplification is driven by the turbulent small-scale dynamo that can be [...]]]></description>
			<content:encoded><![CDATA[<p>Here we summarize our recent results of high-resolution computer simulations on the turbulent amplification of weak magnetic seed fields showing that such fields will be exponentially amplified also during the gravitational collapse reminiscent to the situation during primordial star formation. The exponential magnetic field amplification is driven by the turbulent small-scale dynamo that can be only observed in computer simulations if the turbulent motions in the central core are sufficiently resolved. We find that the Jeans length, which determines the central core region, has to be resolved by at least 30 grid cells to capture the dynamo activity. We conclude from our studies that strong magnetic fields will be unavoidably created already during the formation of the first stars in the Universe, potentially influencing their evolution and mass distribution.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/generation-of-strong-magnetic-fields-via-the-small-scale-dynamo-during-the-formation-of-the-first-stars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Spectroscopic detection of Carbon Monoxide in the Young Supernova Remnant Cassiopeia A</title>
		<link>http://voxcharta.org/2012/02/21/spectroscopic-detection-of-carbon-monoxide-in-the-young-supernova-remnant-cassiopeia-a/</link>
		<comments>http://voxcharta.org/2012/02/21/spectroscopic-detection-of-carbon-monoxide-in-the-young-supernova-remnant-cassiopeia-a/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:55:18 +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[band profile]]></category>
		<category><![CDATA[carbon monoxide]]></category>
		<category><![CDATA[co detection]]></category>
		<category><![CDATA[co emission]]></category>
		<category><![CDATA[decay]]></category>
		<category><![CDATA[ejecta]]></category>
		<category><![CDATA[emission models]]></category>
		<category><![CDATA[energetic electron]]></category>
		<category><![CDATA[estimates]]></category>
		<category><![CDATA[explosion]]></category>
		<category><![CDATA[infrared camera]]></category>
		<category><![CDATA[molecule]]></category>
		<category><![CDATA[nuclei]]></category>
		<category><![CDATA[slit]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[supernova remnant cassiopeia]]></category>
		<category><![CDATA[supernovae]]></category>
		<category><![CDATA[thermodynamic equilibrium]]></category>
		<category><![CDATA[vibrational mode]]></category>
		<category><![CDATA[wavelength]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/spectroscopic-detection-of-carbon-monoxide-in-the-young-supernova-remnant-cassiopeia-a/</guid>
		<description><![CDATA[We report the detection of carbon monoxide (CO) emission from the young supernova remnant Cassiopeia A (Cas A) at wavelengths corresponding to the fundamental vibrational mode at 4.65 micron. We obtained AKARI Infrared Camera spectra towards 4 positions which unambiguously reveal the broad characteristic CO ro-vibrational band profile. The observed positions include unshocked ejecta at [...]]]></description>
			<content:encoded><![CDATA[<p>We report the detection of carbon monoxide (CO) emission from the young supernova remnant Cassiopeia A (Cas A) at wavelengths corresponding to the fundamental vibrational mode at 4.65 micron. We obtained AKARI Infrared Camera spectra towards 4 positions which unambiguously reveal the broad characteristic CO ro-vibrational band profile. The observed positions include unshocked ejecta at the center, indicating that CO molecules form in the ejecta at an early phase. We extracted a dozen spectra across Cas A along the long 1 arcmin slits, and compared these to simple CO emission models in Local Thermodynamic Equilibrium to obtain first-order estimates of the excitation temperatures and CO masses involved. Our observations suggest that significant amounts of carbon may have been locked up in CO since the explosion 330 years ago. Surprisingly, CO has not been efficiently destroyed by reactions with ionized He or the energetic electrons created by the decay of the radiative nuclei. Our CO detection thus implies that less carbon is available to form carbonaceous dust in supernovae than is currently thought and that molecular gas could lock up a significant amount of heavy elements in supernova ejecta.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/spectroscopic-detection-of-carbon-monoxide-in-the-young-supernova-remnant-cassiopeia-a/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Kinematics and helicity evolution of a loop-like eruptive prominence</title>
		<link>http://voxcharta.org/2012/02/21/kinematics-and-helicity-evolution-of-a-loop-like-eruptive-prominence/</link>
		<comments>http://voxcharta.org/2012/02/21/kinematics-and-helicity-evolution-of-a-loop-like-eruptive-prominence/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:54:22 +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[chromosphere]]></category>
		<category><![CDATA[cme]]></category>
		<category><![CDATA[constant velocity]]></category>
		<category><![CDATA[critical value]]></category>
		<category><![CDATA[filament]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[lasco c2]]></category>
		<category><![CDATA[lasco soho]]></category>
		<category><![CDATA[magnetic field configuration]]></category>
		<category><![CDATA[magnetic flux rope]]></category>
		<category><![CDATA[magnetic reconnection]]></category>
		<category><![CDATA[maximum height]]></category>
		<category><![CDATA[northern periphery]]></category>
		<category><![CDATA[prominence]]></category>
		<category><![CDATA[sdo]]></category>
		<category><![CDATA[solar prominence]]></category>
		<category><![CDATA[twisted threads]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/kinematics-and-helicity-evolution-of-a-loop-like-eruptive-prominence/</guid>
		<description><![CDATA[We aim at investigating the morphology, kinematic and helicity evolution of a loop-like prominence during its eruption. We use multi-instrument observations from AIA/SDO, EUVI/STEREO and LASCO/SoHO. The kinematic, morphological, geometrical, and helicity evolution of a loop-like eruptive prominence are studied in the context of the magnetic flux rope model of solar prominences. The prominence eruption [...]]]></description>
			<content:encoded><![CDATA[<p>We aim at investigating the morphology, kinematic and helicity evolution of a loop-like prominence during its eruption. We use multi-instrument observations from AIA/SDO, EUVI/STEREO and LASCO/SoHO. The kinematic, morphological, geometrical, and helicity evolution of a loop-like eruptive prominence are studied in the context of the magnetic flux rope model of solar prominences. The prominence eruption evolved as a height expanding twisted loop with both legs anchored in the chromosphere of a plage area. The eruption process consists of a prominence activation, acceleration, and a phase of constant velocity. The prominence body was composed of left-hand (counter-clockwise) twisted threads around the main prominence axis. The twist during the eruption was estimated at 6pi (3 turns). The prominence reached a maximum height of 526 Mm before contracting to its primary location and partially reformed in the same place two days after the eruption. This ejection, however, triggered a CME seen in LASCO C2. The prominence was located in the northern periphery of the CME magnetic field configuration and, therefore, the background magnetic field was asymmetric with respect to the filament position. The physical conditions of the falling plasma blobs were analysed with respect to the prominence kinematics. The same sign of the prominence body twist and writhe, as well as the amount of twisting above the critical value of 2pi after the activation phase indicate that possibly conditions for kink instability were present. No signature of magnetic reconnection was observed anywhere in the prominence body and its surroundings. The filament/prominence descent following the eruption and its partial reformation at the same place two days later suggest a confined type of eruption. The asymmetric background magnetic field possibly played an important role in the failed eruption.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/kinematics-and-helicity-evolution-of-a-loop-like-eruptive-prominence/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Validity of clumping approximations for mass-loss rates determination</title>
		<link>http://voxcharta.org/2012/02/21/validity-of-clumping-approximations-for-mass-loss-rates-determination/</link>
		<comments>http://voxcharta.org/2012/02/21/validity-of-clumping-approximations-for-mass-loss-rates-determination/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:53:49 +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[approximation]]></category>
		<category><![CDATA[clumping factor]]></category>
		<category><![CDATA[conclusion]]></category>
		<category><![CDATA[consequence]]></category>
		<category><![CDATA[critical point]]></category>
		<category><![CDATA[empirical mass]]></category>
		<category><![CDATA[free parameter]]></category>
		<category><![CDATA[mass loss rates]]></category>
		<category><![CDATA[radiative transfer calculations]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[stellar atmosphere]]></category>
		<category><![CDATA[stellar wind]]></category>
		<category><![CDATA[theoretical prediction]]></category>
		<category><![CDATA[validity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/validity-of-clumping-approximations-for-mass-loss-rates-determination/</guid>
		<description><![CDATA[Clumping in stellar winds of hot stars is a possible consequence of radiative-acoustic instability appearing in solutions of radiative-hydrodynamical equations. However, clumping is usually included to stellar atmosphere modeling and radiative transfer calculations in a highly approximate way via a global free parameter called the clumping factor. Using different values of clumping factors many researchers [...]]]></description>
			<content:encoded><![CDATA[<p>Clumping in stellar winds of hot stars is a possible consequence of radiative-acoustic instability appearing in solutions of radiative-hydrodynamical equations. However, clumping is usually included to stellar atmosphere modeling and radiative transfer calculations in a highly approximate way via a global free parameter called the clumping factor. Using different values of clumping factors many researchers succeeded to fit the observed spectra better and to correct empirical mass loss rates. This usually leads to a conclusion that the stellar wind is clumped. To understand how clumping may influence theoretical predictions of mass-loss rates, different clumping properties have to be taken into account. If clumping appears already below the critical point, the mass-loss rates is changed.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/validity-of-clumping-approximations-for-mass-loss-rates-determination/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Fundamental Physics and Relativistic Laboratory Astrophysics with Extreme Power Lasers</title>
		<link>http://voxcharta.org/2012/02/21/fundamental-physics-and-relativistic-laboratory-astrophysics-with-extreme-power-lasers/</link>
		<comments>http://voxcharta.org/2012/02/21/fundamental-physics-and-relativistic-laboratory-astrophysics-with-extreme-power-lasers/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:53:20 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[compact object]]></category>
		<category><![CDATA[early universe]]></category>
		<category><![CDATA[energy density]]></category>
		<category><![CDATA[extreme power]]></category>
		<category><![CDATA[fundamental physics]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[laboratory astrophysics]]></category>
		<category><![CDATA[matter dynamics]]></category>
		<category><![CDATA[power laser]]></category>
		<category><![CDATA[process simulation]]></category>
		<category><![CDATA[prospects]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/fundamental-physics-and-relativistic-laboratory-astrophysics-with-extreme-power-lasers/</guid>
		<description><![CDATA[The prospects of using extreme relativistic laser-matter interactions for laboratory astrophysics are discussed. Laser-driven process simulation of matter dynamics at ultra-high energy density is proposed for the studies of astrophysical compact objects and the early universe.
]]></description>
			<content:encoded><![CDATA[<p>The prospects of using extreme relativistic laser-matter interactions for laboratory astrophysics are discussed. Laser-driven process simulation of matter dynamics at ultra-high energy density is proposed for the studies of astrophysical compact objects and the early universe.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/fundamental-physics-and-relativistic-laboratory-astrophysics-with-extreme-power-lasers/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Probing the properties of Be star discs with spectroastrometry and NLTE radiative transfer modelling: beta CMi</title>
		<link>http://voxcharta.org/2012/02/21/probing-the-properties-of-be-star-discs-with-spectroastrometry-and-nlte-radiative-transfer-modelling-beta-cmi/</link>
		<comments>http://voxcharta.org/2012/02/21/probing-the-properties-of-be-star-discs-with-spectroastrometry-and-nlte-radiative-transfer-modelling-beta-cmi/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:52:45 +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[angular momentum]]></category>
		<category><![CDATA[cmi]]></category>
		<category><![CDATA[disc model]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[radiative transfer calculations]]></category>
		<category><![CDATA[resolution data]]></category>
		<category><![CDATA[signature]]></category>
		<category><![CDATA[spectral resolution]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/probing-the-properties-of-be-star-discs-with-spectroastrometry-and-nlte-radiative-transfer-modelling-beta-cmi/</guid>
		<description><![CDATA[While the presence of discs around classical Be stars is well established, their origin is still uncertain. To understand what processes result in the creation of these discs and how angular momentum is transported within them, their physical properties must be constrained. This requires comparing high spatial and spectral resolution data with detailed radiative transfer [...]]]></description>
			<content:encoded><![CDATA[<p>While the presence of discs around classical Be stars is well established, their origin is still uncertain. To understand what processes result in the creation of these discs and how angular momentum is transported within them, their physical properties must be constrained. This requires comparing high spatial and spectral resolution data with detailed radiative transfer modelling. We present a high spectral resolution, R~80,000, sub milli-arcsecond precision, spectroastrometric study of the circumstellar disc around the Be star beta CMi. The data are confronted with three-dimensional, NLTE radiative transfer calculations to directly constrain the properties of the disc. Furthermore, we compare the data to disc models featuring two velocity laws; Keperian, the prediction of the viscous disc model, and angular momentum conserving rotation. It is shown that the observations of beta CMi can only be reproduced using Keplerian rotation. The agreement between the model and the observed SED, polarisation and spectroastrometric signature of beta CMi confirms that the discs around Be stars are well modelled as viscous decretion discs.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/probing-the-properties-of-be-star-discs-with-spectroastrometry-and-nlte-radiative-transfer-modelling-beta-cmi/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Magnetic fields of an active region filament from full Stokes analysis of Si I 1082.7 nm and He I 1083.0 nm</title>
		<link>http://voxcharta.org/2012/02/21/magnetic-fields-of-an-active-region-filament-from-full-stokes-analysis-of-si-i-1082-7-nm-and-he-i-1083-0-nm/</link>
		<comments>http://voxcharta.org/2012/02/21/magnetic-fields-of-an-active-region-filament-from-full-stokes-analysis-of-si-i-1082-7-nm-and-he-i-1083-0-nm/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:52:24 +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[atmosphere layers]]></category>
		<category><![CDATA[data acquisition]]></category>
		<category><![CDATA[eddington]]></category>
		<category><![CDATA[emergence]]></category>
		<category><![CDATA[field intensity]]></category>
		<category><![CDATA[filament]]></category>
		<category><![CDATA[inversion]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetic field strength]]></category>
		<category><![CDATA[magnetic field vector]]></category>
		<category><![CDATA[magnetic topology]]></category>
		<category><![CDATA[milne]]></category>
		<category><![CDATA[polarimetric observations]]></category>
		<category><![CDATA[rope]]></category>
		<category><![CDATA[triplet]]></category>
		<category><![CDATA[upper chromosphere]]></category>
		<category><![CDATA[vacuum tower telescope]]></category>
		<category><![CDATA[vector]]></category>
		<category><![CDATA[velocity maps]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/magnetic-fields-of-an-active-region-filament-from-full-stokes-analysis-of-si-i-1082-7-nm-and-he-i-1083-0-nm/</guid>
		<description><![CDATA[Vector magnetic fields of an active region filament in the photosphere and upper chromosphere are obtained from spectro-polarimetric observations recorded with the Tenerife Infrared Polarimeter (TIP II) at the German Vacuum Tower Telescope (VTT). We apply Milne-Eddington inversions on full Stokes vectors of the photospheric Si I 1082.7 nm and the upper chromospheric He I [...]]]></description>
			<content:encoded><![CDATA[<p>Vector magnetic fields of an active region filament in the photosphere and upper chromosphere are obtained from spectro-polarimetric observations recorded with the Tenerife Infrared Polarimeter (TIP II) at the German Vacuum Tower Telescope (VTT). We apply Milne-Eddington inversions on full Stokes vectors of the photospheric Si I 1082.7 nm and the upper chromospheric He I triplet at 1083.0 nm to obtain magnetic field vector and velocity maps in two atmosphere layers. We find that: (1)A complete filament was already present in H$\alpha$ at the beginning of the TIP II data acquisition. Only a partially formed one, composed of multiple small threads, was present in He I. (2) The AR filament comprises two sections. One shows strong magnetic field intensities, about 600 &#8211; 800 G in the upper chromosphere and 800 &#8211; 1000 G in the photosphere. The other exhibits only comparatively weak magnetic field strengths in both layers. (3) The Stokes V signal is indicative of a dip in the magnetic field strength close to the chromospheric PIL. (3) In the chromosphere consistent upflows are found along the PIL flanked by downflows. (4) The transversal magnetic field is nearly parallel to the PIL in the photosphere and inclined by 20 &#8211; 30 degree in the chromosphere. (5) The chromospheric magnetic field around the filament is found to be in normal configuration, while the photospheric field presents a concave magnetic topology. The observations are consistent with the emergence of a flux rope with a subsequent formation of a filament.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/magnetic-fields-of-an-active-region-filament-from-full-stokes-analysis-of-si-i-1082-7-nm-and-he-i-1083-0-nm/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A Search for UHE Tau Neutrinos with IceCube</title>
		<link>http://voxcharta.org/2012/02/21/a-search-for-uhe-tau-neutrinos-with-icecube/</link>
		<comments>http://voxcharta.org/2012/02/21/a-search-for-uhe-tau-neutrinos-with-icecube/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:51:27 +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[astrophysical sources]]></category>
		<category><![CDATA[cm 2]]></category>
		<category><![CDATA[electron]]></category>
		<category><![CDATA[energy range]]></category>
		<category><![CDATA[flavors]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[pev]]></category>
		<category><![CDATA[phi]]></category>
		<category><![CDATA[selection criteria]]></category>
		<category><![CDATA[sr 1]]></category>
		<category><![CDATA[stat]]></category>
		<category><![CDATA[string configuration]]></category>
		<category><![CDATA[tau neutrino]]></category>
		<category><![CDATA[TeV]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/a-search-for-uhe-tau-neutrinos-with-icecube/</guid>
		<description><![CDATA[The first dedicated search for ultra-high energy (UHE) tau neutrinos of astrophysical origin was performed using the IceCube detector in its 22-string configuration. The search also had sensitivity to UHE electron and muon neutrinos. After application of all selection criteria to approximately 200 live-days of data, we expect a background of 0.60 +/- 0.19 (stat.) [...]]]></description>
			<content:encoded><![CDATA[<p>The first dedicated search for ultra-high energy (UHE) tau neutrinos of astrophysical origin was performed using the IceCube detector in its 22-string configuration. The search also had sensitivity to UHE electron and muon neutrinos. After application of all selection criteria to approximately 200 live-days of data, we expect a background of 0.60 +/- 0.19 (stat.) $^{+0.56}_{-0.58}$ (sys.) events and observe three events, which after inspection emerge as being compatible with background. Therefore, we set an upper limit on neutrinos of all flavors from UHE astrophysical sources at 90% CL of $E^{2} \Phi(\nu_{x}) &lt; 16.2 * 10^-8 GeV cm^-2 sr^-1 s^-1 over an estimated primary neutrino energy range of 340 TeV to 200 PeV.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/a-search-for-uhe-tau-neutrinos-with-icecube/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Lovelock gravity in the critical spacetime dimension [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/21/the-lovelock-gravity-in-the-critical-spacetime-dimension-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/21/the-lovelock-gravity-in-the-critical-spacetime-dimension-cross-listing/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:51:05 +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[analogue]]></category>
		<category><![CDATA[bianchi]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[critical dimension]]></category>
		<category><![CDATA[derivative]]></category>
		<category><![CDATA[einstein]]></category>
		<category><![CDATA[gravity]]></category>
		<category><![CDATA[homogeneous polynomial]]></category>
		<category><![CDATA[Lambda]]></category>
		<category><![CDATA[monopole]]></category>
		<category><![CDATA[riemann curvature]]></category>
		<category><![CDATA[spacetime dimension]]></category>
		<category><![CDATA[vacuum solution]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/the-lovelock-gravity-in-the-critical-spacetime-dimension-cross-listing/</guid>
		<description><![CDATA[It is well known that the vacuum in the Einstein gravity, which is linear in the Riemann curvature, is trivial in the critical (2+1=3) dimension because vacuum solution is flat. It turns out that this is true in general for any odd critical $d=2n+1$ dimension where $n$ is the degree of homogeneous polynomial in Riemann [...]]]></description>
			<content:encoded><![CDATA[<p>It is well known that the vacuum in the Einstein gravity, which is linear in the Riemann curvature, is trivial in the critical (2+1=3) dimension because vacuum solution is flat. It turns out that this is true in general for any odd critical $d=2n+1$ dimension where $n$ is the degree of homogeneous polynomial in Riemann defining its higher order analogue whose trace is the nth order Lovelock polynomial. This is the &#8220;curvature&#8221; for nth order pure Lovelock gravity as the trace of its Bianchi derivative gives the corresponding analogue of the Einstein tensor \cite{bianchi}. Thus the vacuum in the pure Lovelock gravity is always trivial in the odd critical (2n+1) dimension which means it is pure Lovelock flat but it is not Riemann flat unless $n=1$ and then it describes a field of a global monopole. Further by adding Lambda we obtain the Lovelock analogue of the BTZ black hole.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/the-lovelock-gravity-in-the-critical-spacetime-dimension-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The starburst-AGN connection in the merger galaxy Mrk 938: an infrared and X-ray view</title>
		<link>http://voxcharta.org/2012/02/21/the-starburst-agn-connection-in-the-merger-galaxy-mrk-938-an-infrared-and-x-ray-view/</link>
		<comments>http://voxcharta.org/2012/02/21/the-starburst-agn-connection-in-the-merger-galaxy-mrk-938-an-infrared-and-x-ray-view/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:50:48 +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[AGN]]></category>
		<category><![CDATA[coexistence]]></category>
		<category><![CDATA[decomposition]]></category>
		<category><![CDATA[estimation]]></category>
		<category><![CDATA[galaxy merger]]></category>
		<category><![CDATA[herschel]]></category>
		<category><![CDATA[infrared emission]]></category>
		<category><![CDATA[intense star]]></category>
		<category><![CDATA[mrk]]></category>
		<category><![CDATA[nucleus]]></category>
		<category><![CDATA[physical nature]]></category>
		<category><![CDATA[ray view]]></category>
		<category><![CDATA[remnant]]></category>
		<category><![CDATA[spectroscopic observation]]></category>
		<category><![CDATA[spectrum]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[universe]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/the-starburst-agn-connection-in-the-merger-galaxy-mrk-938-an-infrared-and-x-ray-view/</guid>
		<description><![CDATA[Mrk938 is a luminous infrared galaxy in the local Universe believed to be the remnant of a galaxy merger. It shows a Seyfert 2 nucleus and intense star formation according to optical spectroscopic observations. We have studied this galaxy using new Herschel far-IR imaging data in addition to archival X-ray, UV, optical, near-IR and mid-IR [...]]]></description>
			<content:encoded><![CDATA[<p>Mrk938 is a luminous infrared galaxy in the local Universe believed to be the remnant of a galaxy merger. It shows a Seyfert 2 nucleus and intense star formation according to optical spectroscopic observations. We have studied this galaxy using new Herschel far-IR imaging data in addition to archival X-ray, UV, optical, near-IR and mid-IR data. Mid- and far-IR data are crucial to characterise the starburst contribution, allowing us to shed new light on its nature and to study the coexistence of AGN and starburst activity in the local Universe. The decomposition of the mid-IR Spitzer spectrum shows that the AGN bolometric contribution to the mid-IR and total infrared luminosity is small (Lbol(AGN)/LIR~0.02), which agrees with previous estimations. We have characterised the physical nature of its strong infrared emission and constrained it to a relatively compact emitting region of &lt;2kpc. It is in this obscured region where most of the current star formation activity is taking place as expected for LIRGs. We have used Herschel imaging data for the first time to constrain the cold dust emission with unprecedented accuracy. We have fitted the integrated far-IR spectral energy distribution and derived the properties of the dust, obtaining a dust mass of 3&#215;10^7Msun. The far-IR is dominated by emission at 35K, consistent with dust heated by the on-going star formation activity.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/the-starburst-agn-connection-in-the-merger-galaxy-mrk-938-an-infrared-and-x-ray-view/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Presupernova evolution and explosive nucleosynthesis of zero metal massive stars</title>
		<link>http://voxcharta.org/2012/02/21/presupernova-evolution-and-explosive-nucleosynthesis-of-zero-metal-massive-stars/</link>
		<comments>http://voxcharta.org/2012/02/21/presupernova-evolution-and-explosive-nucleosynthesis-of-zero-metal-massive-stars/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:50:28 +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[core collapse supernovae]]></category>
		<category><![CDATA[ejecta]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[nucleosynthesis]]></category>
		<category><![CDATA[orfeo]]></category>
		<category><![CDATA[roma]]></category>
		<category><![CDATA[solar metallicity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/presupernova-evolution-and-explosive-nucleosynthesis-of-zero-metal-massive-stars/</guid>
		<description><![CDATA[We present a new set of zero metallicity models in the range 13-80 $\rm M_\odot$ together to the associated explosive nucleosynthesis. These models are fully homogeneous with the solar metallicity set we published in Limongi &#38; Chieffi (2006) and will be freely available at the web site http://www.iasf-roma.inaf.it./orfeo/public{\_}html. A comparison between these yields and an [...]]]></description>
			<content:encoded><![CDATA[<p>We present a new set of zero metallicity models in the range 13-80 $\rm M_\odot$ together to the associated explosive nucleosynthesis. These models are fully homogeneous with the solar metallicity set we published in Limongi &amp; Chieffi (2006) and will be freely available at the web site <a href="http://www.iasf-roma.inaf.it">http://www.iasf-roma.inaf.it</a>./orfeo/public{\_}html. A comparison between these yields and an average star that represents the average behavior of most of the very metal poor stars in the range $\rm -5.0&lt;[Fe/H]&lt;-2.5$ confirms previous findings that only a fraction of the elemental [X/Fe] may be fitted by the ejecta of $\it standard$ core collapse supernovae.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/presupernova-evolution-and-explosive-nucleosynthesis-of-zero-metal-massive-stars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A lucky imaging multiplicity study of exoplanet host stars</title>
		<link>http://voxcharta.org/2012/02/21/a-lucky-imaging-multiplicity-study-of-exoplanet-host-stars/</link>
		<comments>http://voxcharta.org/2012/02/21/a-lucky-imaging-multiplicity-study-of-exoplanet-host-stars/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:50:09 +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[astralux]]></category>
		<category><![CDATA[astrometry]]></category>
		<category><![CDATA[calar alto]]></category>
		<category><![CDATA[direct imaging]]></category>
		<category><![CDATA[extrasolar planet]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[host star]]></category>
		<category><![CDATA[imaging camera]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[multiplicity]]></category>
		<category><![CDATA[northern hemisphere]]></category>
		<category><![CDATA[planet formation]]></category>
		<category><![CDATA[proper motion]]></category>
		<category><![CDATA[radial velocity]]></category>
		<category><![CDATA[stellar companion]]></category>
		<category><![CDATA[stellar system]]></category>
		<category><![CDATA[Telescope]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/a-lucky-imaging-multiplicity-study-of-exoplanet-host-stars/</guid>
		<description><![CDATA[To understand the influence of additional wide stellar companions on planet formation, it is necessary to determine the fraction of multiple stellar systems amongst the known extrasolar planet population. We target recently discovered radial velocity exoplanetary systems observable from the northern hemisphere and with sufficiently high proper motion to detect stellar companions via direct imaging. [...]]]></description>
			<content:encoded><![CDATA[<p>To understand the influence of additional wide stellar companions on planet formation, it is necessary to determine the fraction of multiple stellar systems amongst the known extrasolar planet population. We target recently discovered radial velocity exoplanetary systems observable from the northern hemisphere and with sufficiently high proper motion to detect stellar companions via direct imaging. We utilize the Calar Alto 2.2m telescope in combination with its lucky imaging camera AstraLux. 71 planet host stars have been observed so far, yielding one new low-mass (0.239 \pm 0.022M\odot) stellar companion, 4.5 arcsec (227AU of projected separation) northeast of the planet host star HD185269, detected via astrometry with AstraLux. We also present follow-up astrometry on three previously discovered stellar companions, showing for the first time common proper motion of the 0.5 arcsec companion to HD126614. Additionally, we determined the achieved detection limits for all targets, which allows us to characterize the detection space of possible further companions of these stars.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/a-lucky-imaging-multiplicity-study-of-exoplanet-host-stars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Distinguishing between a true period and its alias, and other tasks of model discrimination</title>
		<link>http://voxcharta.org/2012/02/21/distinguishing-between-a-true-period-and-its-alias-and-other-tasks-of-model-discrimination/</link>
		<comments>http://voxcharta.org/2012/02/21/distinguishing-between-a-true-period-and-its-alias-and-other-tasks-of-model-discrimination/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:49:56 +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[alias]]></category>
		<category><![CDATA[ambiguity]]></category>
		<category><![CDATA[closeness]]></category>
		<category><![CDATA[extrasolar planetary system]]></category>
		<category><![CDATA[hasty conclusions]]></category>
		<category><![CDATA[information criterion]]></category>
		<category><![CDATA[model discrimination]]></category>
		<category><![CDATA[rival models]]></category>
		<category><![CDATA[time series data]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/distinguishing-between-a-true-period-and-its-alias-and-other-tasks-of-model-discrimination/</guid>
		<description><![CDATA[We consider the task of distinguishing between two different alternative models that can roughly equally explain observed time series data, mainly focusing on the period ambiguity case (aliasing). We propose a test for checking whether the rival models are observationally equivalent for now or they are already distinguishable. It is the Vuong closeness test, which [...]]]></description>
			<content:encoded><![CDATA[<p>We consider the task of distinguishing between two different alternative models that can roughly equally explain observed time series data, mainly focusing on the period ambiguity case (aliasing). We propose a test for checking whether the rival models are observationally equivalent for now or they are already distinguishable. It is the Vuong closeness test, which is based on the Kullback-Leibler Information Criterion. It is asymptotically normal and can work (in certain sense) even in the misspecified case, when the both proposed alternatives are actually wrong. This test is also very simple for practical use. We apply it to several known extrasolar planetary systems and find that our method often helps to resolve various model ambiguities emerging in astronomical practice, but preventing us from hasty conclusions in other cases.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/distinguishing-between-a-true-period-and-its-alias-and-other-tasks-of-model-discrimination/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The colours of BL Lac objects: a new approach to their classification</title>
		<link>http://voxcharta.org/2012/02/21/the-colours-of-bl-lac-objects-a-new-approach-to-their-classification/</link>
		<comments>http://voxcharta.org/2012/02/21/the-colours-of-bl-lac-objects-a-new-approach-to-their-classification/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:49:30 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bl lac objects]]></category>
		<category><![CDATA[colour index]]></category>
		<category><![CDATA[colour plots]]></category>
		<category><![CDATA[distribution type]]></category>
		<category><![CDATA[energy source]]></category>
		<category><![CDATA[galaxy cluster]]></category>
		<category><![CDATA[galaxy type]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[host galaxy]]></category>
		<category><![CDATA[interacting systems]]></category>
		<category><![CDATA[k band]]></category>
		<category><![CDATA[lacs]]></category>
		<category><![CDATA[low frequency]]></category>
		<category><![CDATA[narrow strip]]></category>
		<category><![CDATA[peak frequency]]></category>
		<category><![CDATA[photometry]]></category>
		<category><![CDATA[radio flux]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[spectral energy distribution]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/the-colours-of-bl-lac-objects-a-new-approach-to-their-classification/</guid>
		<description><![CDATA[We selected a sample of 437 BL Lac objects, taken from the RomaBZCat catalogue, for which spectroscopic information and SDSS photometry is available. We propose a new classification of BL Lacs in which the sources&#8217; type is not defined only on the basis of the peak frequency of the synchrotron component in their Spectral Energy [...]]]></description>
			<content:encoded><![CDATA[<p>We selected a sample of 437 BL Lac objects, taken from the RomaBZCat catalogue, for which spectroscopic information and SDSS photometry is available. We propose a new classification of BL Lacs in which the sources&#8217; type is not defined only on the basis of the peak frequency of the synchrotron component in their Spectral Energy Distribution (types L and H), but also on the relevance of this component with respect to the brightness of the host galaxy (types N and G, for nuclear or galaxy dominated sources). We found that the SDSS colour index u-r=1.4 is a good separator between these two types. We used multiband colour-colour plots to study the properties of the BL Lac classes and found that in the X-ray to radio flux ratio vs u-r plot most of the N (blue) sources are located in a rather narrow strip, while the G-sources (red) are spread in a large area, and most of them are located in galaxy clusters or interacting systems, suggesting that their X-ray emission is not from a genuine BL Lac nucleus but it is related to their environment. Of the about 135 sources detected in the gamma-rays by Fermi-GST, nearly all belong to the N-type, indicating that only this type of sources should be considered as genuine BL Lac nuclei. The J-H, H-K plot of sources detected in the 2MASS catalogue is consistent with that of the &#8220;bona fide&#8221; BL Lac objects, independently of their N or G classification from the optical indices, indicating the existence in G-type sources of a K-band excess possibly due to a steep, low frequency peaked emission which deserves further investigations. We propose to use these colour plots as a further tool for searching candidate counterparts of newly discovered high-energy sources.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/the-colours-of-bl-lac-objects-a-new-approach-to-their-classification/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Surface Brightness Variation of the Contact Binary SW Lac: Clues From Doppler Imaging</title>
		<link>http://voxcharta.org/2012/02/21/surface-brightness-variation-of-the-contact-binary-sw-lac-clues-from-doppler-imaging/</link>
		<comments>http://voxcharta.org/2012/02/21/surface-brightness-variation-of-the-contact-binary-sw-lac-clues-from-doppler-imaging/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:49:15 +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[brightness variation]]></category>
		<category><![CDATA[circular spot]]></category>
		<category><![CDATA[doppler imaging]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[light curve]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[map]]></category>
		<category><![CDATA[mcdonald observatory]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[otto struve]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[surface brightness]]></category>
		<category><![CDATA[Telescope]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/surface-brightness-variation-of-the-contact-binary-sw-lac-clues-from-doppler-imaging/</guid>
		<description><![CDATA[In this study, we present the preliminary light curve analysis of the contact binary SW Lac, using B, V light curves of the system spanning 2 years (2009 &#8211; 2010). During the spot modeling process, we used the information coming from the Doppler maps of the system, which was performed using the high resolution and [...]]]></description>
			<content:encoded><![CDATA[<p>In this study, we present the preliminary light curve analysis of the contact binary SW Lac, using B, V light curves of the system spanning 2 years (2009 &#8211; 2010). During the spot modeling process, we used the information coming from the Doppler maps of the system, which was performed using the high resolution and phase dependent spectra obtained at the 2.1 m Otto Struve Telescope of the McDonald Observatory, in 2009. The results showed that the spot modeling from the light curve analysis are in accordance with the Doppler maps, while the non-circular spot modeling technique is needed in order to obtain much better and reliable spot models.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/surface-brightness-variation-of-the-contact-binary-sw-lac-clues-from-doppler-imaging/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Effects of Leakage Neutral Particles on Shocks</title>
		<link>http://voxcharta.org/2012/02/21/effects-of-leakage-neutral-particles-on-shocks/</link>
		<comments>http://voxcharta.org/2012/02/21/effects-of-leakage-neutral-particles-on-shocks/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:48:48 +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]]></category>
		<category><![CDATA[analytical solution]]></category>
		<category><![CDATA[approximation]]></category>
		<category><![CDATA[compression ratio]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[interstellar medium]]></category>
		<category><![CDATA[neutral particle]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[percents]]></category>
		<category><![CDATA[pickup ions]]></category>
		<category><![CDATA[precursor]]></category>
		<category><![CDATA[shock]]></category>
		<category><![CDATA[shock compression]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[supernova remnant]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/effects-of-leakage-neutral-particles-on-shocks/</guid>
		<description><![CDATA[The interstellar medium is not necessary fully ionized. When a shock propagates into the partially ionized medium, some neutral particles leak into the upstream region from the downstream region. In this paper, we investigate how leakage neutral particles affect the upstream structure of the shock and particle accelerations. By using four fluid approximations (upstream ions, [...]]]></description>
			<content:encoded><![CDATA[<p>The interstellar medium is not necessary fully ionized. When a shock propagates into the partially ionized medium, some neutral particles leak into the upstream region from the downstream region. In this paper, we investigate how leakage neutral particles affect the upstream structure of the shock and particle accelerations. By using four fluid approximations (upstream ions, upstream neutral particles, leakage neutral particles and pickup ions), we provide analytical solutions of the precursor structure due to leakage neutral particles. It is shown that the upstream flow is decelerated in the precursor and the shock compression ratio becomes smaller than that of the strong shock limit, but the total compression ratio is the same as that of the strong shock limit. Even if leakage of neutral particles is small (a few percents of upstream particles), this smaller compression ratio of the shock can explain steep gamma-ray spectra from young supernova remnants.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/effects-of-leakage-neutral-particles-on-shocks/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>MIPS 24-160 micron photometry for the Herschel-SPIRE Local Galaxies Guaranteed Time Programs</title>
		<link>http://voxcharta.org/2012/02/21/mips-24-160-micron-photometry-for-the-herschel-spire-local-galaxies-guaranteed-time-programs/</link>
		<comments>http://voxcharta.org/2012/02/21/mips-24-160-micron-photometry-for-the-herschel-spire-local-galaxies-guaranteed-time-programs/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:48:24 +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[cluster survey]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[herschel]]></category>
		<category><![CDATA[mip]]></category>
		<category><![CDATA[multiband imaging]]></category>
		<category><![CDATA[nearby galaxy]]></category>
		<category><![CDATA[photometer]]></category>
		<category><![CDATA[photometry data]]></category>
		<category><![CDATA[space observatory]]></category>
		<category><![CDATA[spectral energy distribution]]></category>
		<category><![CDATA[spire]]></category>
		<category><![CDATA[survey]]></category>
		<category><![CDATA[time program]]></category>
		<category><![CDATA[virgo cluster]]></category>
		<category><![CDATA[wave band]]></category>
		<category><![CDATA[wavelength]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/mips-24-160-micron-photometry-for-the-herschel-spire-local-galaxies-guaranteed-time-programs/</guid>
		<description><![CDATA[We provide an overview of ancillary 24, 70, and 160 micron data from the Multiband Imaging Photometer for Spitzer (MIPS) that are intended to complement the 70-500 micron Herschel Space Observatory photometry data for nearby galaxies obtained by the Herschel-SPIRE Local Galaxies Guaranteed Time Programs and the Herschel Virgo Cluster Survey. The MIPS data can [...]]]></description>
			<content:encoded><![CDATA[<p>We provide an overview of ancillary 24, 70, and 160 micron data from the Multiband Imaging Photometer for Spitzer (MIPS) that are intended to complement the 70-500 micron Herschel Space Observatory photometry data for nearby galaxies obtained by the Herschel-SPIRE Local Galaxies Guaranteed Time Programs and the Herschel Virgo Cluster Survey. The MIPS data can be used to extend the photometry to wave bands that are not observed in these Herschel surveys and to check the photometry in cases where Herschel performs observations at the same wavelengths. Additionally, we measured globally-integrated 24-160 micron flux densities for the galaxies in the sample that can be used for the construction of spectral energy distributions. Using MIPS photometry published by other references, we have confirmed that we are obtaining accurate photometry for these galaxies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/mips-24-160-micron-photometry-for-the-herschel-spire-local-galaxies-guaranteed-time-programs/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Observations and Analysis of High-Resolution Magnetic Field Structures in Molecular Clouds</title>
		<link>http://voxcharta.org/2012/02/21/observations-and-analysis-of-high-resolution-magnetic-field-structures-in-molecular-clouds/</link>
		<comments>http://voxcharta.org/2012/02/21/observations-and-analysis-of-high-resolution-magnetic-field-structures-in-molecular-clouds/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:48:06 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[dense structure]]></category>
		<category><![CDATA[evolutionary stage]]></category>
		<category><![CDATA[field structure]]></category>
		<category><![CDATA[high angular resolution]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[hourglass]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[millimeter array]]></category>
		<category><![CDATA[molecular cloud]]></category>
		<category><![CDATA[patches]]></category>
		<category><![CDATA[polarization observations]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[testbed]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/observations-and-analysis-of-high-resolution-magnetic-field-structures-in-molecular-clouds/</guid>
		<description><![CDATA[Recent high-angular-resolution (up to 0.7&#8243;) dust polarization observations toward star forming regions are summarized. With the Sub-Millimeter Array, the emission from the dense structures is traced and resolved. The detected magnetic field morphologies vary from hourglass-like structures to isolated patches depending on the evolutionary stage of the source. These observed features have also served as [...]]]></description>
			<content:encoded><![CDATA[<p>Recent high-angular-resolution (up to 0.7&#8243;) dust polarization observations toward star forming regions are summarized. With the Sub-Millimeter Array, the emission from the dense structures is traced and resolved. The detected magnetic field morphologies vary from hourglass-like structures to isolated patches depending on the evolutionary stage of the source. These observed features have also served as a testbed to develop new analysis methods, with a particular focus on quantifying the role of the magnetic field in the star formation process.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/observations-and-analysis-of-high-resolution-magnetic-field-structures-in-molecular-clouds/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Publication Trends in Astronomy: The Lone Author [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/21/publication-trends-in-astronomy-the-lone-author-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/21/publication-trends-in-astronomy-the-lone-author-cross-listing/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:47:50 +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[astronomy journals]]></category>
		<category><![CDATA[astrophysics data system]]></category>
		<category><![CDATA[author papers]]></category>
		<category><![CDATA[collaborators]]></category>
		<category><![CDATA[nasa]]></category>
		<category><![CDATA[nasa astrophysics data]]></category>
		<category><![CDATA[nasa astrophysics data system]]></category>
		<category><![CDATA[publication trends]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/publication-trends-in-astronomy-the-lone-author-cross-listing/</guid>
		<description><![CDATA[In this short communication I highlight how the number of collaborators on papers in the main astronomy journals has evolved over time. We see a trend of moving away from single-author papers. This communication is based on data in the holdings of the SAO/NASA Astrophysics Data System (ADS).   The ADS is funded by [...]]]></description>
			<content:encoded><![CDATA[<p>In this short communication I highlight how the number of collaborators on papers in the main astronomy journals has evolved over time. We see a trend of moving away from single-author papers. This communication is based on data in the holdings of the SAO/NASA Astrophysics Data System (ADS).   The ADS is funded by NASA Grant NNX09AB39G.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/publication-trends-in-astronomy-the-lone-author-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Symmetry energy effects on location of the inner edge of neutron star crusts [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/21/symmetry-energy-effects-on-location-of-the-inner-edge-of-neutron-star-crusts-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/21/symmetry-energy-effects-on-location-of-the-inner-edge-of-neutron-star-crusts-cross-listing/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:47:37 +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[accuracy]]></category>
		<category><![CDATA[approximation]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[energy effects]]></category>
		<category><![CDATA[equation of state]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[inner edge]]></category>
		<category><![CDATA[moment of inertia]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[nuclear matter]]></category>
		<category><![CDATA[phenomenological model]]></category>
		<category><![CDATA[related properties]]></category>
		<category><![CDATA[symmetry]]></category>
		<category><![CDATA[transition]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/symmetry-energy-effects-on-location-of-the-inner-edge-of-neutron-star-crusts-cross-listing/</guid>
		<description><![CDATA[The symmetry energy effects on the location of the inner edge of neutron star crusts are studied. Three phenomenological models are employed in order to check the accuracy of the well known parabolic approximation of the equation of state for asymmetric nuclear matter in the determination of the transition density $n_t$ and transition pressure $P_t$. [...]]]></description>
			<content:encoded><![CDATA[<p>The symmetry energy effects on the location of the inner edge of neutron star crusts are studied. Three phenomenological models are employed in order to check the accuracy of the well known parabolic approximation of the equation of state for asymmetric nuclear matter in the determination of the transition density $n_t$ and transition pressure $P_t$. The results corroborate the statement that the error due to the assumption that a priori the equation of state is parabolic may introduce a large error in the determination of related properties of a neutron star as the crustal fraction of the moment of inertia.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/symmetry-energy-effects-on-location-of-the-inner-edge-of-neutron-star-crusts-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Dipole Collapse and Dynamo Waves in Global Direct Numerical Simulations</title>
		<link>http://voxcharta.org/2012/02/21/dipole-collapse-and-dynamo-waves-in-global-direct-numerical-simulations/</link>
		<comments>http://voxcharta.org/2012/02/21/dipole-collapse-and-dynamo-waves-in-global-direct-numerical-simulations/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:47:19 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[aspect ratio]]></category>
		<category><![CDATA[collapse]]></category>
		<category><![CDATA[control parameter]]></category>
		<category><![CDATA[dynamo]]></category>
		<category><![CDATA[dynamo action]]></category>
		<category><![CDATA[dynamo models]]></category>
		<category><![CDATA[field topologies]]></category>
		<category><![CDATA[free boundary conditions]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[mass star]]></category>
		<category><![CDATA[numerical simulation]]></category>
		<category><![CDATA[order of magnitude]]></category>
		<category><![CDATA[overtone]]></category>
		<category><![CDATA[regime]]></category>
		<category><![CDATA[single mode]]></category>
		<category><![CDATA[stars and planets]]></category>
		<category><![CDATA[test field]]></category>
		<category><![CDATA[zonal flow]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/dipole-collapse-and-dynamo-waves-in-global-direct-numerical-simulations/</guid>
		<description><![CDATA[Magnetic fields of low-mass stars and planets are thought to originate from self-excited dynamo action in their convective interiors. Observations reveal a variety of field topologies ranging from large-scale, axial dipole to more structured magnetic fields. In this article, we investigate more than 70 three-dimensional, self-consistent dynamo models obtained by direct numerical simulations. The control [...]]]></description>
			<content:encoded><![CDATA[<p>Magnetic fields of low-mass stars and planets are thought to originate from self-excited dynamo action in their convective interiors. Observations reveal a variety of field topologies ranging from large-scale, axial dipole to more structured magnetic fields. In this article, we investigate more than 70 three-dimensional, self-consistent dynamo models obtained by direct numerical simulations. The control parameters, the aspect ratio and the mechanical boundary conditions have been varied to build up this sample of models. Both, strongly dipolar and multipolar models have been obtained. We show that these dynamo regimes can in general be distinguished by the ratio of a typical convective length scale to the Rossby radius. Models with a predominantly dipolar magnetic field were obtained, if the convective length scale is at least an order of magnitude larger than the Rossby radius. Moreover, we highlight the role of the strong shear associated with the geostrophic zonal flow for models with stress-free boundary conditions. In this case, the above transition disappears and is replaced by a region of bistability for which dipolar and multipolar dynamos co-exist. We interpret our results in terms of dynamo eigenmodes using the so-called test-field method. We can thus show that models in the dipolar regime are characterized by an isolated &#8217;single mode&#8217;. Competing overtones become significant as the boundary to multipolar dynamos is approached. We discuss how these findings relate to previous models and to observations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/dipole-collapse-and-dynamo-waves-in-global-direct-numerical-simulations/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Thermonuclear X-ray bursts from the 401 Hertz accreting pulsar IGR J17498-2921: indication of burning in confined regions</title>
		<link>http://voxcharta.org/2012/02/21/thermonuclear-x-ray-bursts-from-the-401-hertz-accreting-pulsar-igr-j17498-2921-indication-of-burning-in-confined-regions/</link>
		<comments>http://voxcharta.org/2012/02/21/thermonuclear-x-ray-bursts-from-the-401-hertz-accreting-pulsar-igr-j17498-2921-indication-of-burning-in-confined-regions/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:47:03 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[burst]]></category>
		<category><![CDATA[burster]]></category>
		<category><![CDATA[hertz]]></category>
		<category><![CDATA[igr]]></category>
		<category><![CDATA[magnetic axis]]></category>
		<category><![CDATA[oscillation]]></category>
		<category><![CDATA[proportional counter]]></category>
		<category><![CDATA[rate ratio]]></category>
		<category><![CDATA[Ray Bursts]]></category>
		<category><![CDATA[sigma]]></category>
		<category><![CDATA[spectral analysis]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[stellar surface]]></category>
		<category><![CDATA[to the best of our knowledge]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/thermonuclear-x-ray-bursts-from-the-401-hertz-accreting-pulsar-igr-j17498-2921-indication-of-burning-in-confined-regions/</guid>
		<description><![CDATA[We use the 2011 Rossi X-ray Timing Explorer (RXTE) proportional counter array (PCA) data of the 401 Hz accreting pulsar and burster IGR J17498-2921 to perform timing analysis and time-resolved spectroscopy of 12 thermonuclear X-ray bursts. We confirm previously reported burst oscillations from this source with a much higher significance (8.8\sigma). We notice that the [...]]]></description>
			<content:encoded><![CDATA[<p>We use the 2011 Rossi X-ray Timing Explorer (RXTE) proportional counter array (PCA) data of the 401 Hz accreting pulsar and burster IGR J17498-2921 to perform timing analysis and time-resolved spectroscopy of 12 thermonuclear X-ray bursts. We confirm previously reported burst oscillations from this source with a much higher significance (8.8\sigma). We notice that the bursts can be divided into three groups: big photospheric radius expansion (PRE) bursts are about ten times more luminous than medium bursts, while the latter are about ten times more luminous than small bursts. The PCA field-of-view of these observations contains several known bursters, and hence some of the observed bursts might not be from IGR J17498-2921. The oscillations during big bursts at the known pulsar frequency show that these bursts were definitely from IGR J17498-2921. We find that at least several of the other bursts were also likely originated from IGR J17498-2921. Spectral analysis reveals that the luminosity differences among various bursts are primarily due to differences in normalizations, and not temperatures, even when we consider the effects of colour factor. This shows burning on a fraction of the stellar surface for those small and medium bursts, which originated from IGR J17498-2921. The low values of the upper limits of burst oscillation amplitude for these bursts suggest a small angle between the spin axis and the magnetic axis. We find indications of the PRE nature of a medium burst, which likely originated from IGR J17498-2921. If true, then, to the best of our knowledge, this is the first time that two PRE bursts with a peak count rate ratio of as high as {\approx} 12 have been detected from the same source.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/thermonuclear-x-ray-bursts-from-the-401-hertz-accreting-pulsar-igr-j17498-2921-indication-of-burning-in-confined-regions/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The dominant role of mergers in the size evolution of massive early-type galaxies since z ~ 1</title>
		<link>http://voxcharta.org/2012/02/21/the-dominant-role-of-mergers-in-the-size-evolution-of-massive-early-type-galaxies-since-z-1/</link>
		<comments>http://voxcharta.org/2012/02/21/the-dominant-role-of-mergers-in-the-size-evolution-of-massive-early-type-galaxies-since-z-1/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:46:17 +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[cosmos field]]></category>
		<category><![CDATA[dominant role]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[merger]]></category>
		<category><![CDATA[pair]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[Sun]]></category>
		<category><![CDATA[type galaxy]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/the-dominant-role-of-mergers-in-the-size-evolution-of-massive-early-type-galaxies-since-z-1/</guid>
		<description><![CDATA[In this paper we measure the merger fraction and rate, both minor and major, of massive early-type galaxies (M_star &#62;= 10^11 M_Sun) in the COSMOS field, and study their role in mass and size evolution. We use the 30-band photometric catalogue in COSMOS, complemented with the spectroscopy of the zCOSMOS survey, to define close pairs [...]]]></description>
			<content:encoded><![CDATA[<p>In this paper we measure the merger fraction and rate, both minor and major, of massive early-type galaxies (M_star &gt;= 10^11 M_Sun) in the COSMOS field, and study their role in mass and size evolution. We use the 30-band photometric catalogue in COSMOS, complemented with the spectroscopy of the zCOSMOS survey, to define close pairs with a separation 10h^-1 kpc &lt;= r_p &lt;= 30h-1 kpc and a relative velocity Delta v = 1/4) and minor (1/10 &lt;= mu = 1/10 mergers can explain ~55% of the observed size evolution of these galaxies since z ~ 1. Another ~20% is due to the progenitor bias (younger galaxies are more extended) and we estimate that very minor mergers (mu &lt; 1/10) could contribute with an extra ~20%. The remaining ~5% should come from other processes (e.g., adiabatic expansion or observational effects). This picture also reproduces the mass growth and velocity dispersion evolution of these galaxies. We conclude from these results that merging is the main contributor to the size evolution of massive ETGs at z &lt;= 1, accounting for ~50-75% of that evolution in the last 8 Gyr. Nearly half of the evolution due to mergers is related to minor (mu &lt; 1/4) events.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/the-dominant-role-of-mergers-in-the-size-evolution-of-massive-early-type-galaxies-since-z-1/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Exploring the supernova remnant G308.4-1.4</title>
		<link>http://voxcharta.org/2012/02/21/exploring-the-supernova-remnant-g308-4-1-4/</link>
		<comments>http://voxcharta.org/2012/02/21/exploring-the-supernova-remnant-g308-4-1-4/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:46:03 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[australian telescope]]></category>
		<category><![CDATA[chandra x ray]]></category>
		<category><![CDATA[density variation]]></category>
		<category><![CDATA[emission characteristics]]></category>
		<category><![CDATA[geometrical center]]></category>
		<category><![CDATA[hydrogen density]]></category>
		<category><![CDATA[infrared observation]]></category>
		<category><![CDATA[infrared wavelength]]></category>
		<category><![CDATA[plasma temperature]]></category>
		<category><![CDATA[progenitor star]]></category>
		<category><![CDATA[radio wavelength]]></category>
		<category><![CDATA[ray observatory]]></category>
		<category><![CDATA[ray point]]></category>
		<category><![CDATA[shell type]]></category>
		<category><![CDATA[solar values]]></category>
		<category><![CDATA[spatial density]]></category>
		<category><![CDATA[spectral energy distribution]]></category>
		<category><![CDATA[supernova explosion]]></category>
		<category><![CDATA[supernova remnant catalogue]]></category>
		<category><![CDATA[telescope compact array]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/exploring-the-supernova-remnant-g308-4-1-4/</guid>
		<description><![CDATA[Aims: We present a detailed X-ray and radio wavelength study of G308.4-1.4, a candidate supernova remnant (SNR) in the ROSAT All Sky Survey and the MOST supernova remnant catalogue.   Methods: The SNR candidate and its central point sources were studied using observations from the Chandra X-ray Observatory, SWIFT, the Australian Telescope Compact Array [...]]]></description>
			<content:encoded><![CDATA[<p>Aims: We present a detailed X-ray and radio wavelength study of G308.4-1.4, a candidate supernova remnant (SNR) in the ROSAT All Sky Survey and the MOST supernova remnant catalogue.   Methods: The SNR candidate and its central point sources were studied using observations from the Chandra X-ray Observatory, SWIFT, the Australian Telescope Compact Array (ATCA) at 1.4 and 2.5 GHz and WISE infrared observation at 24 $\mu$m.   Results: We conclude that G308.4-1.4 is indeed a supernova remnant by means of its morphology matching at X-ray, radio and infrared wavelength, its spectral energy distribution in the X-ray band and its emission characteristics in the radio band. G308.4-1.4 is a shell-type SNR. X-ray, radio and infrared emission is seen only in the eastern part of the remnant due to a strong spatial density variation of the interstellar medium around the remnant. The X-ray emission can best be described by an absorbed non-equilibrium collisional plasma with a hydrogen density of $n_\text{H}=(1.02\pm 0.04)$ cm$^{-2}$, a plasma temperature of $6.3^{+1.2}_{-0.7}$ million Kelvin and an under-abundance of Iron, Neon and Magnesium, as well as an overabundance in Sulfur with respect to the solar values. A Sedov analysis revealed that the remnant is at a distance of $ \approx 10$ kpc and the progenitor star exploded $\sim 5000$ to 7500 years ago. Two faint X-ray point sources located near to the remnant&#8217;s geometrical center are detected. Both sources have no counterpart at other wavelengths, leaving them as candidates for the compact remnant of the supernova explosion.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/exploring-the-supernova-remnant-g308-4-1-4/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Assessing the Feasibility of Cosmic-Ray Acceleration by Magnetic Turbulence at the Galactic Center</title>
		<link>http://voxcharta.org/2012/02/21/assessing-the-feasibility-of-cosmic-ray-acceleration-by-magnetic-turbulence-at-the-galactic-center/</link>
		<comments>http://voxcharta.org/2012/02/21/assessing-the-feasibility-of-cosmic-ray-acceleration-by-magnetic-turbulence-at-the-galactic-center/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:44:23 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[conductive environment]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[cosmic ray acceleration]]></category>
		<category><![CDATA[decay]]></category>
		<category><![CDATA[feasibility]]></category>
		<category><![CDATA[galactic center]]></category>
		<category><![CDATA[galactic plane]]></category>
		<category><![CDATA[hadronic]]></category>
		<category><![CDATA[hes]]></category>
		<category><![CDATA[intensity distribution]]></category>
		<category><![CDATA[leptonic interactions]]></category>
		<category><![CDATA[magnetic turbulence]]></category>
		<category><![CDATA[photon]]></category>
		<category><![CDATA[point source]]></category>
		<category><![CDATA[proton]]></category>
		<category><![CDATA[relativistic particle]]></category>
		<category><![CDATA[source candidates]]></category>
		<category><![CDATA[supermassive black hole]]></category>
		<category><![CDATA[tev energies]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/assessing-the-feasibility-of-cosmic-ray-acceleration-by-magnetic-turbulence-at-the-galactic-center/</guid>
		<description><![CDATA[The presence of relativistic particles at the center of our galaxy is evidenced by the diffuse TeV emission detected from the inner $\sim$$2^\circ$ of the Galaxy. Although it is not yet entirely clear whether the origin of the TeV photons is due to hadronic or leptonic interactions, the tight correlation of the intensity distribution with [...]]]></description>
			<content:encoded><![CDATA[<p>The presence of relativistic particles at the center of our galaxy is evidenced by the diffuse TeV emission detected from the inner $\sim$$2^\circ$ of the Galaxy. Although it is not yet entirely clear whether the origin of the TeV photons is due to hadronic or leptonic interactions, the tight correlation of the intensity distribution with the distribution of molecular gas along the Galactic ridge strongly points to a pionic-decay process involving relativistic protons. In earlier work, we concluded that point-source candidates, such as the supermassive black hole Sagittarius A* (identified with the HESS source J1745-290), or the pulsar wind nebulae dispersed along the Galactic plane, could not account for the observed diffuse TeV emission from this region. Motivated by this result, we consider here the feasibility that the cosmic rays populating the Galactic Center (GC) region are accelerated in situ by magnetic turbulence. Our results indicate that even in a highly conductive environment, this mechanism is efficient enough to energize protons within the intercloud medium to the $\ga $ TeV energies required to produce the HESS emission.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/assessing-the-feasibility-of-cosmic-ray-acceleration-by-magnetic-turbulence-at-the-galactic-center/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Sweeping Away the Mysteries of Dusty Continuous Winds in AGN</title>
		<link>http://voxcharta.org/2012/02/21/sweeping-away-the-mysteries-of-dusty-continuous-winds-in-agn/</link>
		<comments>http://voxcharta.org/2012/02/21/sweeping-away-the-mysteries-of-dusty-continuous-winds-in-agn/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:44:01 +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[active galactic nuclei]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[digital sky survey]]></category>
		<category><![CDATA[disk winds]]></category>
		<category><![CDATA[dust grains]]></category>
		<category><![CDATA[dusty disk]]></category>
		<category><![CDATA[dynamical model]]></category>
		<category><![CDATA[fundamental physics]]></category>
		<category><![CDATA[hole mass]]></category>
		<category><![CDATA[input spectrum]]></category>
		<category><![CDATA[msun]]></category>
		<category><![CDATA[observational signature]]></category>
		<category><![CDATA[physical parameter]]></category>
		<category><![CDATA[radiation pressure]]></category>
		<category><![CDATA[relative power]]></category>
		<category><![CDATA[sdss]]></category>
		<category><![CDATA[sloan digital]]></category>
		<category><![CDATA[spectral energy distribution]]></category>
		<category><![CDATA[terminal velocity]]></category>
		<category><![CDATA[unified model]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/sweeping-away-the-mysteries-of-dusty-continuous-winds-in-agn/</guid>
		<description><![CDATA[An integral part of the Unified Model for Active Galactic Nuclei (AGNs) is an axisymmetric obscuring medium, which is commonly depicted as a torus of gas and dust surrounding the central engine. However, a robust, dynamical model of the torus is required in order to understand the fundamental physics of AGNs and interpret their observational [...]]]></description>
			<content:encoded><![CDATA[<p>An integral part of the Unified Model for Active Galactic Nuclei (AGNs) is an axisymmetric obscuring medium, which is commonly depicted as a torus of gas and dust surrounding the central engine. However, a robust, dynamical model of the torus is required in order to understand the fundamental physics of AGNs and interpret their observational signatures. Here we explore self-similar, dusty disk-winds, driven by both magnetocentrifugal forces and radiation pressure, as an explanation for the torus. Using these models, we make predictions of AGN infrared (IR) spectral energy distributions (SEDs) from 2-100 microns by varying parameters such as: the viewing angle; the base column density of the wind; the Eddington ratio; the black hole mass; and the amount of power in the input spectrum emitted in the X-ray relative to that emitted in the UV/optical. We find that models with N_H,0 = 10^25 cm^-2, L/L_Edd = 0.1, and M_BH &gt;= 10^8 Msun are able to adequately approximate the general shape and amount of power expected in the IR as observed in a composite of optically luminous Sloan Digital Sky Survey (SDSS) quasars. The effect of varying the relative power coming out in X-rays relative to the UV is a change in the emission below ~5 micron from the hottest dust grains; this arises from the differing contributions to heating and acceleration of UV and X-ray photons. We see mass outflows ranging from ~1-4 Msun/yr, terminal velocities ranging from ~1900-8000 km/s, and kinetic luminosities ranging from ~1&#215;10^42-8&#215;10^43 erg/s. Further development of this model holds promise for using specific features of observed IR spectra in AGNs to infer fundamental physical parameters of the systems.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/sweeping-away-the-mysteries-of-dusty-continuous-winds-in-agn/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Mergers and ejections of black holes in globular clusters</title>
		<link>http://voxcharta.org/2012/02/21/mergers-and-ejections-of-black-holes-in-globular-clusters/</link>
		<comments>http://voxcharta.org/2012/02/21/mergers-and-ejections-of-black-holes-in-globular-clusters/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:43:44 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[algorithmic]]></category>
		<category><![CDATA[body simulation]]></category>
		<category><![CDATA[characteristic feature]]></category>
		<category><![CDATA[cluster model]]></category>
		<category><![CDATA[coalescence]]></category>
		<category><![CDATA[dense core]]></category>
		<category><![CDATA[eccentricity]]></category>
		<category><![CDATA[ejections]]></category>
		<category><![CDATA[energy loss]]></category>
		<category><![CDATA[globular cluster]]></category>
		<category><![CDATA[hellstrom]]></category>
		<category><![CDATA[merger]]></category>
		<category><![CDATA[mikkola]]></category>
		<category><![CDATA[neutron stars and black holes]]></category>
		<category><![CDATA[radiation energy]]></category>
		<category><![CDATA[schwarzschild radii]]></category>
		<category><![CDATA[segregation]]></category>
		<category><![CDATA[shrinkage]]></category>
		<category><![CDATA[subsystems]]></category>
		<category><![CDATA[velocities]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/mergers-and-ejections-of-black-holes-in-globular-clusters/</guid>
		<description><![CDATA[We report on results of fully consistent N-body simulations of globular cluster models with N = 100 000 members containing neutron stars and black holes. Using the improved `algorithmic regularization&#8217; method of Hellstrom and Mikkola for compact subsystems, the new code NBODY7 enables for the first time general relativistic coalescence to be achieved for post-Newtonian [...]]]></description>
			<content:encoded><![CDATA[<p>We report on results of fully consistent N-body simulations of globular cluster models with N = 100 000 members containing neutron stars and black holes. Using the improved `algorithmic regularization&#8217; method of Hellstrom and Mikkola for compact subsystems, the new code NBODY7 enables for the first time general relativistic coalescence to be achieved for post-Newtonian terms and realistic parameters. Following an early stage of mass segregation, a few black holes form a small dense core which usually leads to the formation of one dominant binary. The subsequent evolution by dynamical shrinkage involves the competing processes of ejection and mergers by radiation energy loss. Unless the binary is ejected, long-lived triple systems often exhibit Kozai cycles with extremely high inner eccentricity (e &gt; 0.999) which may terminate in coalescence at a few Schwarzschild radii. A characteristic feature is that ordinary stars as well as black holes and even BH binaries are ejected with high velocities. On the basis of the models studied so far, the results suggest a limited growth of a few remaining stellar mass black holes in globular clusters.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/mergers-and-ejections-of-black-holes-in-globular-clusters/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Revisiting a model-independent dark energy reconstruction method</title>
		<link>http://voxcharta.org/2012/02/21/revisiting-a-model-independent-dark-energy-reconstruction-method/</link>
		<comments>http://voxcharta.org/2012/02/21/revisiting-a-model-independent-dark-energy-reconstruction-method/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:43:27 +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[complement]]></category>
		<category><![CDATA[conclusion]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[derivative]]></category>
		<category><![CDATA[energy evolution]]></category>
		<category><![CDATA[global trend]]></category>
		<category><![CDATA[grbs]]></category>
		<category><![CDATA[minimal assumptions]]></category>
		<category><![CDATA[new insights]]></category>
		<category><![CDATA[original works]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[polynomial]]></category>
		<category><![CDATA[poor performers]]></category>
		<category><![CDATA[probes]]></category>
		<category><![CDATA[quality basis]]></category>
		<category><![CDATA[reconstruction]]></category>
		<category><![CDATA[reconstruction method]]></category>
		<category><![CDATA[redshift range]]></category>
		<category><![CDATA[selection criteria]]></category>
		<category><![CDATA[state of the art]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/revisiting-a-model-independent-dark-energy-reconstruction-method/</guid>
		<description><![CDATA[Model independent reconstructions of dark energy have received some attention. The approach that addresses the reconstruction of the dimensionless coordinate distance and its two first derivatives using a polynomial fit in different redshift windows is well developed \cite{DalyDjorgovski1,DalyDjorgovski2,DalyDjorgovski3}. In this work we offer new insights into the problem by focusing on two types of observational [...]]]></description>
			<content:encoded><![CDATA[<p>Model independent reconstructions of dark energy have received some attention. The approach that addresses the reconstruction of the dimensionless coordinate distance and its two first derivatives using a polynomial fit in different redshift windows is well developed \cite{DalyDjorgovski1,DalyDjorgovski2,DalyDjorgovski3}. In this work we offer new insights into the problem by focusing on two types of observational probes: SNeIa and GRBs. Our results allow to highlight some of the intrinsic weaknesses of the method. One of the directions we follow is to consider updated observational samples. Our results indicate than conclusions on the main dark energy features as drawn from this method are intimately related to the features of the samples themselves (which are not quite ideal). This is particularly true of GRBs, which manifest themselves as poor performers in this context. In contrast to original works, we conclude they cannot be used for cosmological purposes, and the state of the art does not allow to regard them on the same quality basis as SNeIa. The next direction we contribute to is the question of how the adjusting of some parameters (window width, overlap, selection criteria) affect the results. We find again there is a considerable sensitivity to these features. Then, we try to establish what is the current redshift range for which one can make solid predictions on dark energy evolution. Finally, we strengthen the former view that this model is modest in the sense it provides only a picture of the global trend. But, on the other hand, we believe it offers an interesting complement to other approaches given that it works on minimal assumptions.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/revisiting-a-model-independent-dark-energy-reconstruction-method/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>A remarkable long-term light curve, and deep, low-state spectroscopy: Swift &amp; XMM-Newton monitoring of the NLS1 galaxy Mkn 335</title>
		<link>http://voxcharta.org/2012/02/21/a-remarkable-long-term-light-curve-and-deep-low-state-spectroscopy-swift-xmm-newton-monitoring-of-the-nls1-galaxy-mkn-335/</link>
		<comments>http://voxcharta.org/2012/02/21/a-remarkable-long-term-light-curve-and-deep-low-state-spectroscopy-swift-xmm-newton-monitoring-of-the-nls1-galaxy-mkn-335/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:42:53 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[AGN]]></category>
		<category><![CDATA[broad band]]></category>
		<category><![CDATA[ccd spectrum]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[distinct trends]]></category>
		<category><![CDATA[galactic nucleus]]></category>
		<category><![CDATA[hardness ratio]]></category>
		<category><![CDATA[light curve]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[phenomenological model]]></category>
		<category><![CDATA[reflection model]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectral variability]]></category>
		<category><![CDATA[state spectroscopy]]></category>
		<category><![CDATA[time scale]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xmm newton]]></category>
		<category><![CDATA[xmm observation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/a-remarkable-long-term-light-curve-and-deep-low-state-spectroscopy-swift-xmm-newton-monitoring-of-the-nls1-galaxy-mkn-335/</guid>
		<description><![CDATA[The Narrow-line Seyfert 1 galaxy (NLS1) Mkn 335 is remarkable because it has repeatedly shown deep, long X-ray low-states which show pronounced spectral structure. It has become one of the prototype AGN in deep minimum X-ray states. Here we report on the continuation of our ongoing monitoring campaign with Swift and the examination of the [...]]]></description>
			<content:encoded><![CDATA[<p>The Narrow-line Seyfert 1 galaxy (NLS1) Mkn 335 is remarkable because it has repeatedly shown deep, long X-ray low-states which show pronounced spectral structure. It has become one of the prototype AGN in deep minimum X-ray states. Here we report on the continuation of our ongoing monitoring campaign with Swift and the examination of the low state X-ray spectra based on a 200 ks triggered observation with XMM in June 2009. Swift has continuously monitored Mkn 335 since May 2007 typically on a monthly basis. This is one of the longest simultaneous UV/X-ray light curves so far obtained for an active galactic nucleus (AGN). Mkn 335 has shown strong X-ray variability even on time scales of hours. In the UV, it turns out to be one of the most variable among NLS1s. Long-term Swift monitoring allow us to examine correlations between the UV, X-rays and X-ray hardness ratios. We find no significant correlation or lag between the UV and X-ray variability; however, we do find distinct trends in the behavior of the hardness ratio variability. The hardness ratio and count rate are correlated in the low-flux state, but no correlation is seen in the high-state. The X-ray low-state spectra of the 2007 and 2009 XMM observations display significant spectral variability. We fit the X-ray spectra with a suite of phenomenological models in order to characterize the data. The broad band CCD spectrum can be fitted equally well with partial absorption and blurred reflection models. These more complicated models are explored in further detail in upcoming work.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/a-remarkable-long-term-light-curve-and-deep-low-state-spectroscopy-swift-xmm-newton-monitoring-of-the-nls1-galaxy-mkn-335/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>The Lesser Role of Shear in Star Formation: Insight from the Galactic Ring Survey</title>
		<link>http://voxcharta.org/2012/02/21/the-lesser-role-of-shear-in-star-formation-insight-from-the-galactic-ring-survey/</link>
		<comments>http://voxcharta.org/2012/02/21/the-lesser-role-of-shear-in-star-formation-insight-from-the-galactic-ring-survey/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:42:22 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[clouds the clouds]]></category>
		<category><![CDATA[co line]]></category>
		<category><![CDATA[correlates]]></category>
		<category><![CDATA[critical surface]]></category>
		<category><![CDATA[dense core]]></category>
		<category><![CDATA[fragmentation]]></category>
		<category><![CDATA[galactic ring]]></category>
		<category><![CDATA[galactic star]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gravity]]></category>
		<category><![CDATA[insight]]></category>
		<category><![CDATA[molecular cloud]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[profile]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[surface density]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/the-lesser-role-of-shear-in-star-formation-insight-from-the-galactic-ring-survey/</guid>
		<description><![CDATA[We analyse the role played by shear in regulating star formation in the Galaxy on the scale of individual molecular clouds. The clouds are selected from the $^{13}$CO $J=1-0$ line of the Galactic Ring Survey. We estimate the shear parameter which is the ratio of a critical surface density for the clouds to be disrupted [...]]]></description>
			<content:encoded><![CDATA[<p>We analyse the role played by shear in regulating star formation in the Galaxy on the scale of individual molecular clouds. The clouds are selected from the $^{13}$CO $J=1-0$ line of the Galactic Ring Survey. We estimate the shear parameter which is the ratio of a critical surface density for the clouds to be disrupted by shear to their actual surface density. We find that for almost all molecular clouds considered in the sample, there is no evidence that shear is playing a significant role in opposing the effects of self-gravity. Furthermore, we find that the shear parameter of the clouds does not depend on their position in the Galaxy, which implies that shear can not explain the radial profiles of the Galactic star formation rates. We also find that for gravitationally bound clouds, higher shear parameters do not imply lower masses nor that the shear parameter correlates with the clouds level of fragmentation. Our results suggest that shear is playing only a minor role in affecting the rates at which gravitationally bound molecular clouds convert their gas into dense cores and thereafter into stars.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/the-lesser-role-of-shear-in-star-formation-insight-from-the-galactic-ring-survey/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Temperature-Pressure Profile of the hot Jupiter HD 189733b from HST Sodium Observations: Detection of Upper Atmospheric Heating</title>
		<link>http://voxcharta.org/2012/02/21/temperature-pressure-profile-of-the-hot-jupiter-hd-189733b-from-hst-sodium-observations-detection-of-upper-atmospheric-heating/</link>
		<comments>http://voxcharta.org/2012/02/21/temperature-pressure-profile-of-the-hot-jupiter-hd-189733b-from-hst-sodium-observations-detection-of-upper-atmospheric-heating/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:42:11 +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[absolute pressure]]></category>
		<category><![CDATA[atmospheric regions]]></category>
		<category><![CDATA[atmospheric temperature]]></category>
		<category><![CDATA[confidence level]]></category>
		<category><![CDATA[doublet]]></category>
		<category><![CDATA[exoplanet]]></category>
		<category><![CDATA[hd 189733b]]></category>
		<category><![CDATA[high altitude temperature]]></category>
		<category><![CDATA[light radius]]></category>
		<category><![CDATA[plausible scenario]]></category>
		<category><![CDATA[pressure profile]]></category>
		<category><![CDATA[resolving power]]></category>
		<category><![CDATA[rstar]]></category>
		<category><![CDATA[space telescope imaging]]></category>
		<category><![CDATA[spectral absorption]]></category>
		<category><![CDATA[temperature regimes]]></category>
		<category><![CDATA[thermosphere]]></category>
		<category><![CDATA[vertical temperature profile]]></category>
		<category><![CDATA[wavelength range]]></category>
		<category><![CDATA[zero altitude]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/temperature-pressure-profile-of-the-hot-jupiter-hd-189733b-from-hst-sodium-observations-detection-of-upper-atmospheric-heating/</guid>
		<description><![CDATA[We present transmission spectra of the hot Jupiter HD 189733b taken with the Space Telescope Imaging Spectrograph aboard HST. The spectra cover the wavelength range 5808-6380 Ang with a resolving power of R=5000. We detect absorption from the NaI doublet within the exoplanet&#8217;s atmosphere at the 9 sigma confidence level within a 5 Ang band [...]]]></description>
			<content:encoded><![CDATA[<p>We present transmission spectra of the hot Jupiter HD 189733b taken with the Space Telescope Imaging Spectrograph aboard HST. The spectra cover the wavelength range 5808-6380 Ang with a resolving power of R=5000. We detect absorption from the NaI doublet within the exoplanet&#8217;s atmosphere at the 9 sigma confidence level within a 5 Ang band (absorption depth 0.09 +/- 0.01%) and use the data to measure the doublet&#8217;s spectral absorption profile. We detect only the narrow cores of the doublet. The narrowness of the feature could be due to an obscuring high-altitude haze of an unknown composition or a significantly sub-solar NaI abundance hiding the line wings beneath a H2 Rayleigh signature. We compare the spectral absorption profile over 5.5 scale heights with model spectral absorption profiles and constrain the temperature at different atmospheric regions, allowing us to construct a vertical temperature profile. We identify two temperature regimes; a 1280 +/- 240 K region derived from the NaI doublet line wings corresponding to altitudes below ~ 500 km, and a 2800 +/- 400 K region derived from the NaI doublet line cores corresponding to altitudes from ~ 500-4000 km. The zero altitude is defined by the white-light radius of Rp/Rstar=0.15628 +/- 0.00009. The temperature rises with altitude, which is likely evidence of a thermosphere. The absolute pressure scale depends on the species responsible for the Rayleigh signature and its abundance. We discuss a plausible scenario for this species, a high-altitude silicate haze, and the atmospheric temperature-pressure profile that results. In this case, the high altitude temperature rise for HD 189733b occurs at pressures of 10^-5 to 10^-8 bar.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/temperature-pressure-profile-of-the-hot-jupiter-hd-189733b-from-hst-sodium-observations-detection-of-upper-atmospheric-heating/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Modelling supermassive black hole growth: towards an improved sub-grid prescription</title>
		<link>http://voxcharta.org/2012/02/21/modelling-supermassive-black-hole-growth-towards-an-improved-sub-grid-prescription/</link>
		<comments>http://voxcharta.org/2012/02/21/modelling-supermassive-black-hole-growth-towards-an-improved-sub-grid-prescription/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:41:53 +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[accretion]]></category>
		<category><![CDATA[angular momentum]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[bondi]]></category>
		<category><![CDATA[cosmological simulations]]></category>
		<category><![CDATA[expression]]></category>
		<category><![CDATA[formalism]]></category>
		<category><![CDATA[galaxy formation]]></category>
		<category><![CDATA[gas dynamics]]></category>
		<category><![CDATA[gravity]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[hoyle]]></category>
		<category><![CDATA[orders of magnitude]]></category>
		<category><![CDATA[radius]]></category>
		<category><![CDATA[regime]]></category>
		<category><![CDATA[supermassive black hole]]></category>
		<category><![CDATA[validity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/modelling-supermassive-black-hole-growth-towards-an-improved-sub-grid-prescription/</guid>
		<description><![CDATA[Accretion onto supermassive black holes (SMBHs) in galaxy formation simulations is frequently modelled by the Bondi-Hoyle formalism. Here we examine the validity of this approach analytically and numerically. We argue that the character of the flow where one evaluates the gas properties is unlikely to satisfy the simple Bondi-Hoyle model. Only in the specific case [...]]]></description>
			<content:encoded><![CDATA[<p>Accretion onto supermassive black holes (SMBHs) in galaxy formation simulations is frequently modelled by the Bondi-Hoyle formalism. Here we examine the validity of this approach analytically and numerically. We argue that the character of the flow where one evaluates the gas properties is unlikely to satisfy the simple Bondi-Hoyle model. Only in the specific case of hot virialised gas with zero angular momentum and negligible radiative cooling is the Bondi-Hoyle solution relevant. In the opposite extreme, where the gas is in a state of free-fall at the evaluation radius due to efficient cooling and the dominant gravity of the surrounding halo, the Bondi-Hoyle formalism can be erroneous by orders of magnitude in either direction. This may impose artificial trends with halo mass in cosmological simulations by being wrong by different factors for different halo masses. We propose an expression for the sub-grid accretion rate which interpolates between the free-fall regime and the Bondi-Hoyle regime, therefore taking account of the contribution of the halo to the gas dynamics.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/modelling-supermassive-black-hole-growth-towards-an-improved-sub-grid-prescription/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Search for High-Mass X-ray Binaries in the Phoenix Dwarf Galaxy</title>
		<link>http://voxcharta.org/2012/02/21/the-search-for-high-mass-x-ray-binaries-in-the-phoenix-dwarf-galaxy/</link>
		<comments>http://voxcharta.org/2012/02/21/the-search-for-high-mass-x-ray-binaries-in-the-phoenix-dwarf-galaxy/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:41:35 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[background galaxy]]></category>
		<category><![CDATA[dwarf galaxy]]></category>
		<category><![CDATA[european photon imaging]]></category>
		<category><![CDATA[foreground star]]></category>
		<category><![CDATA[gas cloud]]></category>
		<category><![CDATA[hardness ratio]]></category>
		<category><![CDATA[high mass]]></category>
		<category><![CDATA[local group]]></category>
		<category><![CDATA[mass x]]></category>
		<category><![CDATA[metallicity]]></category>
		<category><![CDATA[myr]]></category>
		<category><![CDATA[optical counterpart]]></category>
		<category><![CDATA[ray binaries]]></category>
		<category><![CDATA[ray sources]]></category>
		<category><![CDATA[small magellanic cloud]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[supernova remnant]]></category>
		<category><![CDATA[transient nature]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xmm newton]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/the-search-for-high-mass-x-ray-binaries-in-the-phoenix-dwarf-galaxy/</guid>
		<description><![CDATA[We report on the first X-ray images of the Phoenix dwarf galaxy, taken with \emph{XMM-Newton} in July 2009. This local group dwarf galaxy shares similarities with the Small Magellanic Cloud (SMC) including a burst of star formation $\sim$50 Myr ago. The SMC has an abundance of High Mass X-ray Binaries (HMXBs) and so we have [...]]]></description>
			<content:encoded><![CDATA[<p>We report on the first X-ray images of the Phoenix dwarf galaxy, taken with \emph{XMM-Newton} in July 2009. This local group dwarf galaxy shares similarities with the Small Magellanic Cloud (SMC) including a burst of star formation $\sim$50 Myr ago. The SMC has an abundance of High Mass X-ray Binaries (HMXBs) and so we have investigated the possibility of an HMXB population in Phoenix with the intention of furthering the understanding of the HMXB-star formation rate relation. The data from the combined European Photon Imaging Cameras (EPIC) were used to distinguish between different source classes (foreground stars, background galaxies, AGN and supernova remnants) using EPIC hardness ratios and correlations with optical and radio catalogues. Of the 81 X-ray sources in the field of view, six are foreground stars, four are galaxies and one is an AGN. The remaining sources with optical counterparts have log($\frac{f_X}{f_{opt}}$) consistent with AGN in the local universe. Further investigation of five sources in the field of view suggests they are all background AGN. Their position behind the gas cloud associated with Phoenix makes them a possible tool for further probing the metallicity of this region. We find no evidence for any HMXBs in Phoenix at this time. This rules out the existence of the X-ray persistent supergiant X-ray binary systems. However the transient nature of the Be/X-ray binaries means we cannot rule out a population of these sources but can conclude that it is not extensive.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/the-search-for-high-mass-x-ray-binaries-in-the-phoenix-dwarf-galaxy/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Southern Africa CTA Site Proposal</title>
		<link>http://voxcharta.org/2012/02/21/southern-africa-cta-site-proposal/</link>
		<comments>http://voxcharta.org/2012/02/21/southern-africa-cta-site-proposal/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:41:21 +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[background level]]></category>
		<category><![CDATA[cherenkov telescopes]]></category>
		<category><![CDATA[cloud coverage]]></category>
		<category><![CDATA[cloudless sky]]></category>
		<category><![CDATA[cta]]></category>
		<category><![CDATA[fiber line]]></category>
		<category><![CDATA[keetmanshoop]]></category>
		<category><![CDATA[luderitz]]></category>
		<category><![CDATA[maximum wind speeds]]></category>
		<category><![CDATA[namibia]]></category>
		<category><![CDATA[national airports]]></category>
		<category><![CDATA[night sky]]></category>
		<category><![CDATA[night time]]></category>
		<category><![CDATA[railway line]]></category>
		<category><![CDATA[sky background]]></category>
		<category><![CDATA[sky brightness]]></category>
		<category><![CDATA[southern africa]]></category>
		<category><![CDATA[sutherland]]></category>
		<category><![CDATA[Telescope]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/southern-africa-cta-site-proposal/</guid>
		<description><![CDATA[Southern Africa has some of the world&#8217;s best sites for air Cherenkov telescopes. South Africa has only one viable site, which is south of Sutherland and also close to the Southern African Large Telescope (SALT). This site has very good infrastructure and is easy to access, but only 47% of the night-time has a cloudless [...]]]></description>
			<content:encoded><![CDATA[<p>Southern Africa has some of the world&#8217;s best sites for air Cherenkov telescopes. South Africa has only one viable site, which is south of Sutherland and also close to the Southern African Large Telescope (SALT). This site has very good infrastructure and is easy to access, but only 47% of the night-time has a cloudless sky usable for observations.   Namibia, which already hosts the H.E.S.S telescope, has a number of potential sites with much less cloud coverage. The H.E.S.S. site is one of the highest of these sites at 1840 m a.s.l. with about 64% of the night-time cloudless. It also has very low night sky background levels and is relatively close (about 100 km) to Windhoek. Moving further away from Windhoek to the south, the cloud coverage and artificial night sky brightness becomes even less, with the site at Kuibis (between Keetmanshoop and Luderitz) at 1640 m a.s.l. having clear night skies 73% of the time. Even though this site seems remote (being 660 km from Windhoek by road), it is close to the national B4 highway, a railway line, a power line and an optical fiber line. It is also less than two hours drive away from a harbour and national airports. The Namibian sites also receive very little snow, if any, and the wind speeds are less than 50 km/h for more than 90% of the time with maximum wind speeds of around 100 km/h. Seismically the whole Southern African region is very stable.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/southern-africa-cta-site-proposal/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The negative effective magnetic pressure in stratified forced turbulence [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/the-negative-effective-magnetic-pressure-in-stratified-forced-turbulence-replacement-2/</link>
		<comments>http://voxcharta.org/2012/02/21/the-negative-effective-magnetic-pressure-in-stratified-forced-turbulence-replacement-2/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:40:52 +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[coefficients]]></category>
		<category><![CDATA[diffusivity]]></category>
		<category><![CDATA[dynamo action]]></category>
		<category><![CDATA[energy density]]></category>
		<category><![CDATA[field model]]></category>
		<category><![CDATA[gradient]]></category>
		<category><![CDATA[intensity increase]]></category>
		<category><![CDATA[isothermal layer]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetic flux]]></category>
		<category><![CDATA[magnetic pressure]]></category>
		<category><![CDATA[numerical experiment]]></category>
		<category><![CDATA[numerical simulation]]></category>
		<category><![CDATA[prandtl number]]></category>
		<category><![CDATA[reynolds number]]></category>
		<category><![CDATA[test field]]></category>
		<category><![CDATA[Turbulence]]></category>
		<category><![CDATA[turbulent intensity]]></category>
		<category><![CDATA[turbulent kinetic energy]]></category>
		<category><![CDATA[vertical profile]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/the-negative-effective-magnetic-pressure-in-stratified-forced-turbulence-replacement-2/</guid>
		<description><![CDATA[To understand the basic mechanism of the formation of magnetic flux concentrations, we determine by direct numerical simulations the turbulence contributions to the mean magnetic pressure in a strongly stratified isothermal layer with large plasma beta, where a weak uniform horizontal mean magnetic field is applied. The negative contribution of turbulence to the effective mean [...]]]></description>
			<content:encoded><![CDATA[<p>To understand the basic mechanism of the formation of magnetic flux concentrations, we determine by direct numerical simulations the turbulence contributions to the mean magnetic pressure in a strongly stratified isothermal layer with large plasma beta, where a weak uniform horizontal mean magnetic field is applied. The negative contribution of turbulence to the effective mean magnetic pressure is determined for strongly stratified forced turbulence over a range of values of magnetic Reynolds and Prandtl numbers. Small-scale dynamo action is shown to reduce the negative effect of turbulence on the effective mean magnetic pressure. However, the turbulence coefficients describing the negative effective magnetic pressure phenomenon are found to be converged for magnetic Reynolds numbers between 60 and 600, which is the largest value considered here. In all these models the turbulent intensity is arranged to be nearly independent of height, so the kinetic energy density decreases with height due to the decrease in density. In a second series of numerical experiments, the turbulent intensity increases with height such that the turbulent kinetic energy density is nearly independent of height. Turbulent magnetic diffusivity and turbulent pumping velocity are determined with the test-field method for both cases. The vertical profile of the turbulent magnetic diffusivity is found to agree with what is expected based on simple mixing length expressions. Turbulent pumping is shown to be down the gradient of turbulent magnetic diffusivity, but it is twice as large as expected. Corresponding numerical mean-field models are used to show that a large-scale instability can occur in both cases, provided the degree of scale separation is large enough and hence the turbulent magnetic diffusivity small enough.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/the-negative-effective-magnetic-pressure-in-stratified-forced-turbulence-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Probing eV-mass scale axions with a Micromegas detector in the CAST experiment [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/probing-ev-mass-scale-axions-with-a-micromegas-detector-in-the-cast-experiment-replacement/</link>
		<comments>http://voxcharta.org/2012/02/21/probing-ev-mass-scale-axions-with-a-micromegas-detector-in-the-cast-experiment-replacement/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:40:39 +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[axion]]></category>
		<category><![CDATA[bore]]></category>
		<category><![CDATA[cern]]></category>
		<category><![CDATA[characterization]]></category>
		<category><![CDATA[coupling]]></category>
		<category><![CDATA[decommissioned]]></category>
		<category><![CDATA[dipole magnet]]></category>
		<category><![CDATA[hypothetical particle]]></category>
		<category><![CDATA[mass range]]></category>
		<category><![CDATA[mass scale]]></category>
		<category><![CDATA[possible solution]]></category>
		<category><![CDATA[solar telescope]]></category>
		<category><![CDATA[strong interaction]]></category>
		<category><![CDATA[Sun]]></category>
		<category><![CDATA[thesis]]></category>
		<category><![CDATA[working principle]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/probing-ev-mass-scale-axions-with-a-micromegas-detector-in-the-cast-experiment-replacement/</guid>
		<description><![CDATA[The CAST (CERN Axion Solar Telescope) experiment is searching for axions, an hypothetical particle that emerges as a possible solution to the well known CP violation problem in strong interactions. CAST is using a decommissioned LHC dipole magnet able to track the Sun as a possible source of solar axions, and to convert them to [...]]]></description>
			<content:encoded><![CDATA[<p>The CAST (CERN Axion Solar Telescope) experiment is searching for axions, an hypothetical particle that emerges as a possible solution to the well known CP violation problem in strong interactions. CAST is using a decommissioned LHC dipole magnet able to track the Sun as a possible source of solar axions, and to convert them to X-rays photons detectable with low background X-ray detectors. CAST continues its data taking period scanning masses up to 1eV. This thesis presents the data obtained with a Micromegas detector for the scanned axion mass range up to 0.64eV. The working principle, characterization and analysis of the Micromegas detectors operating in CAST are detailed in this work. Moreover, the last detector data corresponding to the new data taking period, with 3He gas inside the bores, was used to obtain a preliminar and conservative upper limit on the axion-photon coupling for the new axion mass range explored, g_{a\gamma} &lt; 2.44 10^{-10} GeV^{-1}.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/probing-ev-mass-scale-axions-with-a-micromegas-detector-in-the-cast-experiment-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Phase diagram of dilute cosmic matter [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/phase-diagram-of-dilute-cosmic-matter-replacement-3/</link>
		<comments>http://voxcharta.org/2012/02/21/phase-diagram-of-dilute-cosmic-matter-replacement-3/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:40:29 +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[collisions]]></category>
		<category><![CDATA[cosmic matter]]></category>
		<category><![CDATA[dependent density]]></category>
		<category><![CDATA[enhancement]]></category>
		<category><![CDATA[existence]]></category>
		<category><![CDATA[functional calculations]]></category>
		<category><![CDATA[low density]]></category>
		<category><![CDATA[mean free path]]></category>
		<category><![CDATA[monte carlo calculation]]></category>
		<category><![CDATA[nucleus]]></category>
		<category><![CDATA[pasta]]></category>
		<category><![CDATA[periodic boundary condition]]></category>
		<category><![CDATA[phase diagram]]></category>
		<category><![CDATA[simultaneous collision]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/phase-diagram-of-dilute-cosmic-matter-replacement-3/</guid>
		<description><![CDATA[Enhancement of nuclear pasta formation due to multi-nucleus simultaneous collision is presented based on time-dependent density functional calculations with periodic boundary condition. This calculation corresponds to the situation with density lower than the known low-density existence limit of the nuclear pasta phase. In order to evaluate the contribution from three-nucleus simultaneous collisions inside the cosmic [...]]]></description>
			<content:encoded><![CDATA[<p>Enhancement of nuclear pasta formation due to multi-nucleus simultaneous collision is presented based on time-dependent density functional calculations with periodic boundary condition. This calculation corresponds to the situation with density lower than the known low-density existence limit of the nuclear pasta phase. In order to evaluate the contribution from three-nucleus simultaneous collisions inside the cosmic matter, the possibility of multi-nucleus simultaneous collisions is examined by a systematic Monte-Carlo calculation, and the mean free path of a nucleus is obtained. Consequently the low-density existence limit of the nuclear pasta phase is formed to be lower than believed up to now.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/phase-diagram-of-dilute-cosmic-matter-replacement-3/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The outskirts of globular clusters as modified gravity probes [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/the-outskirts-of-globular-clusters-as-modified-gravity-probes-replacement-2/</link>
		<comments>http://voxcharta.org/2012/02/21/the-outskirts-of-globular-clusters-as-modified-gravity-probes-replacement-2/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:40:12 +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[dark matter]]></category>
		<category><![CDATA[dynamical model]]></category>
		<category><![CDATA[galactic globular cluster]]></category>
		<category><![CDATA[galactic system]]></category>
		<category><![CDATA[gravitational anomaly]]></category>
		<category><![CDATA[gravitational equilibrium]]></category>
		<category><![CDATA[gravity]]></category>
		<category><![CDATA[line of sight]]></category>
		<category><![CDATA[observational constraints]]></category>
		<category><![CDATA[outskirt]]></category>
		<category><![CDATA[phenomenology]]></category>
		<category><![CDATA[population model]]></category>
		<category><![CDATA[probes]]></category>
		<category><![CDATA[radii]]></category>
		<category><![CDATA[rotation curves]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[surface brightness]]></category>
		<category><![CDATA[tully]]></category>
		<category><![CDATA[velocities]]></category>
		<category><![CDATA[velocity dispersion]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/the-outskirts-of-globular-clusters-as-modified-gravity-probes-replacement-2/</guid>
		<description><![CDATA[In the context of theories of gravity modified to account for the observed dynamics of galactic systems without the need to invoke the existence of dark matter, a prediction often appears regarding low acceleration systems: wherever $a$ falls below $a_{0}$ one should expect a transition from the classical to the modified gravity regime.This modified gravity [...]]]></description>
			<content:encoded><![CDATA[<p>In the context of theories of gravity modified to account for the observed dynamics of galactic systems without the need to invoke the existence of dark matter, a prediction often appears regarding low acceleration systems: wherever $a$ falls below $a_{0}$ one should expect a transition from the classical to the modified gravity regime.This modified gravity regime will be characterised by equilibrium velocities which become independent of distance, and which scale with the fourth root of the total baryonic mass, $V^{4} \propto M$. The two above conditions are the well known flat rotation curves and Tully-Fisher relations of the galactic regime. Recently however, a similar phenomenology has been hinted at, at the outskirts of Galactic globular clusters, precisely in the region where $a&lt;a_{0}$. Radial profiles of the projected velocity dispersion have been observed to stop decreasing along Keplerian expectations, and to level off at constant values beyond the radii where $a&lt;a_{0}$. We have constructed gravitational equilibrium dynamical models for a number of globular clusters for which the above gravitational anomaly has been reported, using a modified Newtonian force law which yields equilibrium velocities equivalent to MOND. We find models can be easily constructed having an inner Newtonian region and an outer modified gravity regime, which reproduce all observational constraints, surface brightness profiles, total masses and line of sight velocity dispersion profiles. Through the use of detailed single stellar population models tuned individually to each of the globular clusters in question, we derive estimates of the total masses for these systems. Interestingly, we find that the asymptotic values of the velocity dispersion profiles are consistent with scaling with the fourth root of the total masses, as expected under modified gravity scenarios.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/the-outskirts-of-globular-clusters-as-modified-gravity-probes-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Evolution and Environments of X-ray Emitting Active Galactic Nuclei in High-Redshift Large-Scale Structures [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/the-evolution-and-environments-of-x-ray-emitting-active-galactic-nuclei-in-high-redshift-large-scale-structures-replacement/</link>
		<comments>http://voxcharta.org/2012/02/21/the-evolution-and-environments-of-x-ray-emitting-active-galactic-nuclei-in-high-redshift-large-scale-structures-replacement/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:39:55 +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[active galactic nuclei]]></category>
		<category><![CDATA[AGN]]></category>
		<category><![CDATA[composite spectra]]></category>
		<category><![CDATA[cumulative source]]></category>
		<category><![CDATA[dense cluster]]></category>
		<category><![CDATA[evolutionary state]]></category>
		<category><![CDATA[host galaxy]]></category>
		<category><![CDATA[line strength]]></category>
		<category><![CDATA[nuclear activity]]></category>
		<category><![CDATA[optical spectroscopy]]></category>
		<category><![CDATA[parent population]]></category>
		<category><![CDATA[point source]]></category>
		<category><![CDATA[ray point]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[rest frame]]></category>
		<category><![CDATA[scale structure]]></category>
		<category><![CDATA[spectral property]]></category>
		<category><![CDATA[statistical measure]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/the-evolution-and-environments-of-x-ray-emitting-active-galactic-nuclei-in-high-redshift-large-scale-structures-replacement/</guid>
		<description><![CDATA[We use deep Chandra imaging and an extensive optical spectroscopy campaign on the Keck 10-m telescopes to study the properties of X-ray point sources in five large-scale structures at redshifts of z ~ 0.7-0.9. We first study X-ray point sources using the statistical measure of cumulative source counts, finding that the measured overdensities are consistent [...]]]></description>
			<content:encoded><![CDATA[<p>We use deep Chandra imaging and an extensive optical spectroscopy campaign on the Keck 10-m telescopes to study the properties of X-ray point sources in five large-scale structures at redshifts of z ~ 0.7-0.9. We first study X-ray point sources using the statistical measure of cumulative source counts, finding that the measured overdensities are consistent with previous results, but we recommend caution in overestimating the precision of the technique. Optical spectroscopy of objects matched to X-ray point sources confirms a total of 27 AGN within the five structures, and we find that their host galaxies tend to be located away from dense cluster cores. More than 36% of host galaxies are located in the `green valley&#8217;, which suggests they are a transitional population. Based on analysis of OII and Hd line strengths, the average spectral properties of the AGN host galaxies in all structures indicate either on-going star formation or a starburst within ~ 1 Gyr, and the host galaxies are younger than the average galaxy in the parent population. These results indicate a clear connection between starburst and nuclear activity. We use composite spectra of the spectroscopically confirmed members in each structure to separate them based on a measure of the overall evolutionary state of their constituent galaxies. We define structures as having more evolved populations if their average galaxy has lower EW(OII) and EW(Hd). The AGN in the more evolved structures have lower rest-frame 0.5-8 keV X-ray luminosities (all below 10^43.3 erg s^-1) and longer times since a starburst than those in the less evolved structures, suggesting that the peak of both star formation and AGN activity has occurred at earlier times. With the wide range of evolutionary states and timeframes in the structures, we use our results to analyze the evolution of X-ray AGN and evaluate potential triggering mechanisms.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/the-evolution-and-environments-of-x-ray-emitting-active-galactic-nuclei-in-high-redshift-large-scale-structures-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The CoDECS project: a publicly available suite of cosmological N-body simulations for interacting dark energy models [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/the-codecs-project-a-publicly-available-suite-of-cosmological-n-body-simulations-for-interacting-dark-energy-models-replacement/</link>
		<comments>http://voxcharta.org/2012/02/21/the-codecs-project-a-publicly-available-suite-of-cosmological-n-body-simulations-for-interacting-dark-energy-models-replacement/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:39:30 +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[background data]]></category>
		<category><![CDATA[baryon]]></category>
		<category><![CDATA[body simulation]]></category>
		<category><![CDATA[cold dark matter]]></category>
		<category><![CDATA[cosmic microwave background]]></category>
		<category><![CDATA[cosmological model]]></category>
		<category><![CDATA[cosmological parameters]]></category>
		<category><![CDATA[cosmological simulations]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[degeneracy]]></category>
		<category><![CDATA[density perturbations]]></category>
		<category><![CDATA[energy model]]></category>
		<category><![CDATA[hydrodynamical simulations]]></category>
		<category><![CDATA[power spectrum]]></category>
		<category><![CDATA[previous works]]></category>
		<category><![CDATA[realistic determination]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[scalar field]]></category>
		<category><![CDATA[scale dependence]]></category>
		<category><![CDATA[statistical significance]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/the-codecs-project-a-publicly-available-suite-of-cosmological-n-body-simulations-for-interacting-dark-energy-models-replacement/</guid>
		<description><![CDATA[We present the largest set of N-body and hydrodynamical simulations to date for cosmological models featuring a direct interaction between the Dark Energy (DE) scalar field, responsible of the observed cosmic acceleration, and the Cold Dark Matter (CDM) fluid. With respect to previous works, our simulations considerably extend the statistical significance of the simulated volume [...]]]></description>
			<content:encoded><![CDATA[<p>We present the largest set of N-body and hydrodynamical simulations to date for cosmological models featuring a direct interaction between the Dark Energy (DE) scalar field, responsible of the observed cosmic acceleration, and the Cold Dark Matter (CDM) fluid. With respect to previous works, our simulations considerably extend the statistical significance of the simulated volume and cover a wider range of different realizations of the interacting DE scenario, including the recently proposed bouncing coupled DE model. Furthermore, all the simulations are normalized in order to be consistent with the present bounds on the amplitude of density perturbations at last scattering, thereby providing the first realistic determination of the effects of a DE coupling for cosmological growth histories fully compatible with the latest Cosmic Microwave Background data. As a first basic analysis, we have studied the impact of the coupling on the nonlinear matter power spectrum and on the bias between the CDM and baryon distributions, as a function of redshift and scale. For the former, we have addressed the issue of the degeneracy between the effects of the coupling and other standard cosmological parameters, as e.g sigma_8, showing how the redshift evolution of the linear amplitude or the scale dependence of the nonlinear power spectrum might provide a way to break the degeneracy. For the latter, instead, we have computed the redshift and scale dependence of the bias in all our different models showing how a growing coupling or a bouncing coupled DE scenario provide much stronger effects with respect to constant coupling models. We refer to this vast numerical initiative as the COupled Dark Energy Cosmological Simulations project, or CoDECS, and we hereby release all the CoDECS outputs for public use through a dedicated web database, providing information on how to access and interpret the data.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/the-codecs-project-a-publicly-available-suite-of-cosmological-n-body-simulations-for-interacting-dark-energy-models-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Clustering and redshift-space distortions in interacting dark energy cosmologies [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/clustering-and-redshift-space-distortions-in-interacting-dark-energy-cosmologies-replacement/</link>
		<comments>http://voxcharta.org/2012/02/21/clustering-and-redshift-space-distortions-in-interacting-dark-energy-cosmologies-replacement/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:39:15 +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[bia]]></category>
		<category><![CDATA[catalogues]]></category>
		<category><![CDATA[cdm]]></category>
		<category><![CDATA[cold dark matter]]></category>
		<category><![CDATA[concordance]]></category>
		<category><![CDATA[cosmic microwave background]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[distortions]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[large scale]]></category>
		<category><![CDATA[lss]]></category>
		<category><![CDATA[redshift space]]></category>
		<category><![CDATA[scale structure]]></category>
		<category><![CDATA[scales]]></category>
		<category><![CDATA[scenarios]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[spatial properties]]></category>
		<category><![CDATA[suppression]]></category>
		<category><![CDATA[universe]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/clustering-and-redshift-space-distortions-in-interacting-dark-energy-cosmologies-replacement/</guid>
		<description><![CDATA[We investigate the spatial properties of the large scale structure (LSS) of the Universe in the framework of coupled dark energy (cDE) cosmologies. Using the public halo catalogues from the CoDECS simulations &#8212; the largest set of N-body experiments to date for such cosmological scenarios &#8212; we estimate the clustering and bias functions of cold [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate the spatial properties of the large scale structure (LSS) of the Universe in the framework of coupled dark energy (cDE) cosmologies. Using the public halo catalogues from the CoDECS simulations &#8212; the largest set of N-body experiments to date for such cosmological scenarios &#8212; we estimate the clustering and bias functions of cold dark matter (CDM) haloes, both in real- and redshift-space. Moreover, we investigate the effects of the dark energy (DE) coupling on the geometric and dynamic redshift-space distortions, quantifying the difference with respect to the concordance LambdaCDM model. At z~0, the spatial properties of CDM haloes in cDE models appear very similar to the LambdaCDM case, even if the cDE models are normalized at last scattering in order to be consistent with the latest Cosmic Microwave Background (CMB) data. At higher redshifts, we find that the DE coupling produces a significant scale-dependent suppression of the halo clustering and bias function. This effect, that strongly depends on the coupling strength, is not degenerate with sigma8 at scales r&lt;5-10 Mpc/h. Moreover, we find that the coupled DE strongly affects both the linear distortion parameter, beta, and the pairwise peculiar velocity dispersion, sigma12. Although the models considered in this work are found to be all in agreement with presently available observational data, the next generation of galaxy surveys will be able to put strong constraints on the level of coupling between DE and CDM exploiting the shape of redshift-space clustering anisotropies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/clustering-and-redshift-space-distortions-in-interacting-dark-energy-cosmologies-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Evidence for a compact Wolf-Rayet progenitor for the Type Ic supernova PTF 10vgv [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/evidence-for-a-compact-wolf-rayet-progenitor-for-the-type-ic-supernova-ptf-10vgv-replacement/</link>
		<comments>http://voxcharta.org/2012/02/21/evidence-for-a-compact-wolf-rayet-progenitor-for-the-type-ic-supernova-ptf-10vgv-replacement/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:39:03 +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[discovery]]></category>
		<category><![CDATA[inch telescope]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[palomar]]></category>
		<category><![CDATA[progenitor star]]></category>
		<category><![CDATA[ptf]]></category>
		<category><![CDATA[radius]]></category>
		<category><![CDATA[rsun]]></category>
		<category><![CDATA[shock]]></category>
		<category><![CDATA[type ic]]></category>
		<category><![CDATA[wolf]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/evidence-for-a-compact-wolf-rayet-progenitor-for-the-type-ic-supernova-ptf-10vgv-replacement/</guid>
		<description><![CDATA[We present the discovery of PTF 10vgv, a Type Ic supernova detected by the Palomar Transient Factory, using the Palomar 48-inch telescope (P48). R-band observations of the PTF 10vgv field with P48 probe the supernova emission from its very early phases (about two weeks before R-band maximum), and set limits on its flux in the [...]]]></description>
			<content:encoded><![CDATA[<p>We present the discovery of PTF 10vgv, a Type Ic supernova detected by the Palomar Transient Factory, using the Palomar 48-inch telescope (P48). R-band observations of the PTF 10vgv field with P48 probe the supernova emission from its very early phases (about two weeks before R-band maximum), and set limits on its flux in the week prior to the discovery. Our sensitive upper limits and early detections constrain the post-shock-breakout luminosity of this event. Via comparison to numerical (analytical) models, we derive an upper-limit of R \lesssim 4.5 Rsun (R \lesssim 1 Rsun) on the radius of the progenitor star, a direct indication in favor of a compact Wolf-Rayet star. Applying a similar analysis to the historical observations of SN 1994I, yields R \lesssim 1/4 Rsun for the progenitor radius of this supernova.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/evidence-for-a-compact-wolf-rayet-progenitor-for-the-type-ic-supernova-ptf-10vgv-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>3DEX: a code for fast spherical Fourier-Bessel decomposition of 3D surveys [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/3dex-a-code-for-fast-spherical-fourier-bessel-decomposition-of-3d-surveys-replacement-2/</link>
		<comments>http://voxcharta.org/2012/02/21/3dex-a-code-for-fast-spherical-fourier-bessel-decomposition-of-3d-surveys-replacement-2/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:38:47 +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[aim]]></category>
		<category><![CDATA[computation time]]></category>
		<category><![CDATA[cosmological data]]></category>
		<category><![CDATA[decomposition]]></category>
		<category><![CDATA[discipline]]></category>
		<category><![CDATA[equivalent formulation]]></category>
		<category><![CDATA[expansion]]></category>
		<category><![CDATA[external storage]]></category>
		<category><![CDATA[fourier]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[missing data]]></category>
		<category><![CDATA[precision cosmology]]></category>
		<category><![CDATA[rapid calculation]]></category>
		<category><![CDATA[scale survey]]></category>
		<category><![CDATA[scales]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[sky survey]]></category>
		<category><![CDATA[speed improvements]]></category>
		<category><![CDATA[spherical coordinates]]></category>
		<category><![CDATA[spherical harmonics]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/3dex-a-code-for-fast-spherical-fourier-bessel-decomposition-of-3d-surveys-replacement-2/</guid>
		<description><![CDATA[High-precision cosmology requires the analysis of large-scale surveys in 3D spherical coordinates, i.e. spherical Fourier-Bessel decomposition. Current methods are insufficient for future data-sets from wide-field cosmology surveys. The aim of this paper is to present a public code for fast spherical Fourier-Bessel decomposition that can be applied to cosmological data or 3D data in spherical [...]]]></description>
			<content:encoded><![CDATA[<p>High-precision cosmology requires the analysis of large-scale surveys in 3D spherical coordinates, i.e. spherical Fourier-Bessel decomposition. Current methods are insufficient for future data-sets from wide-field cosmology surveys. The aim of this paper is to present a public code for fast spherical Fourier-Bessel decomposition that can be applied to cosmological data or 3D data in spherical coordinates in other scientific fields. We present an equivalent formulation of the spherical Fourier-Bessel decomposition that separates radial and tangential calculations. We propose the use of the existing pixelisation scheme HEALPix for a rapid calculation of the tangential modes. 3DEX (3D EXpansions) is a public code for fast spherical Fourier-Bessel decomposition of 3D all-sky surveys that takes advantage of HEALPix for the calculation of tangential modes. We perform tests on very large simulations and we compare the precision and computation time of our method with an optimised implementation of the spherical Fourier-Bessel original formulation. For surveys with millions of galaxies, computation time is reduced by a factor 4-12 depending on the desired scales and accuracy. The formulation is also suitable for pre-calculations and external storage of the spherical harmonics, which allows for additional speed improvements. The 3DEX code can accommodate data with masked regions of missing data. 3DEX can also be used in other disciplines, where 3D data are to be analysed in spherical coordinates. The code and documentation can be downloaded at <a href="http://ixkael.com/blog/3dex.">http://ixkael.com/blog/3dex.</a></p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/3dex-a-code-for-fast-spherical-fourier-bessel-decomposition-of-3d-surveys-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Constraints on interacting dark energy models from galaxy Rotation Curves [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/constraints-on-interacting-dark-energy-models-from-galaxy-rotation-curves-replacement/</link>
		<comments>http://voxcharta.org/2012/02/21/constraints-on-interacting-dark-energy-models-from-galaxy-rotation-curves-replacement/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:38:21 +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[body simulation]]></category>
		<category><![CDATA[cdm]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[cosmic structure]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[coupling]]></category>
		<category><![CDATA[cusp]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[density profile]]></category>
		<category><![CDATA[dynamical properties]]></category>
		<category><![CDATA[energy model]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[interaction strength]]></category>
		<category><![CDATA[observational data]]></category>
		<category><![CDATA[pilot investigation]]></category>
		<category><![CDATA[rotation curves]]></category>
		<category><![CDATA[scale structure]]></category>
		<category><![CDATA[spiral galaxy]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/constraints-on-interacting-dark-energy-models-from-galaxy-rotation-curves-replacement/</guid>
		<description><![CDATA[[Abridged] High-resolution N-body simulations have recently shown that the structural properties of highly nonlinear cosmic structures, as e.g. their average concentration at a given mass, could be significantly modified in the presence of an interaction between Dark Energy and Dark Matter. While a constant interaction strength leads to less concentrated density profiles, a steep growth [...]]]></description>
			<content:encoded><![CDATA[<p>[Abridged] High-resolution N-body simulations have recently shown that the structural properties of highly nonlinear cosmic structures, as e.g. their average concentration at a given mass, could be significantly modified in the presence of an interaction between Dark Energy and Dark Matter. While a constant interaction strength leads to less concentrated density profiles, a steep growth in time of the coupling function has been shown to determine a large increase of halo concentrations over a wide range of masses, including the typical halos hosting luminous spiral galaxies. This determines a substantial worsening of the &#8220;cusp-core&#8221; tension arising in the standard $\Lambda $CDM model and provides a direct way to constrain the form of the Dark Energy interaction. In the present paper we make use of the outcomes of some high-resolution N-body simulations of a specific class of interacting Dark Energy models to compare the predicted rotation curves of luminous spiral galaxies forming in these cosmologies against real observational data. Our results show how some specific interacting Dark Energy scenarios featuring a steep growth in time of the coupling function &#8212; which are virtually indistinguishable from LCDM in the background &#8212; cannot fit the observed rotation curves of luminous spiral galaxies and can therefore be ruled out only on the basis of dynamical properties of small-scale structures. Our study is a pilot investigation of the effects of a Dark Energy interaction at small scales, and demonstrates how the dynamical properties of visible galaxies can in some cases provide direct constraints on the nature of Dark Energy.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/constraints-on-interacting-dark-energy-models-from-galaxy-rotation-curves-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Statistical Tests of Noise and Harmony in Dark Matter Modulation Signals [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/statistical-tests-of-noise-and-harmony-in-dark-matter-modulation-signals-replacement/</link>
		<comments>http://voxcharta.org/2012/02/21/statistical-tests-of-noise-and-harmony-in-dark-matter-modulation-signals-replacement/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:38:06 +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[aim]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[collaboration]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[dataset]]></category>
		<category><![CDATA[earth]]></category>
		<category><![CDATA[harmonics]]></category>
		<category><![CDATA[harmony]]></category>
		<category><![CDATA[modulation]]></category>
		<category><![CDATA[phenomena]]></category>
		<category><![CDATA[power spectrum]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[statistical test]]></category>
		<category><![CDATA[Sun]]></category>
		<category><![CDATA[time dependence]]></category>
		<category><![CDATA[time series analysis]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/statistical-tests-of-noise-and-harmony-in-dark-matter-modulation-signals-replacement/</guid>
		<description><![CDATA[The aim of the current work is a detailed time-series analysis of the data from Dark Matter direct detection experiments as well as related datasets. We examine recent claims that the cosmic ray muon flux can be responsible for generating the modulation signals seen by DAMA and, more recently, by the CoGeNT collaboration. We find [...]]]></description>
			<content:encoded><![CDATA[<p>The aim of the current work is a detailed time-series analysis of the data from Dark Matter direct detection experiments as well as related datasets. We examine recent claims that the cosmic ray muon flux can be responsible for generating the modulation signals seen by DAMA and, more recently, by the CoGeNT collaboration. We find no evidence for such a strong correlation and show that the two phenomena differ in their power spectrum, phase, and possibly in amplitude. In addition, we investigate in more detail, the time dependence of Dark Matter scattering. Since the signal is periodic with period of a year (due to the Earth&#8217;s motion around the Sun), the presence of higher harmonics can be expected. We show that the higher harmonics generically have similar phase to the annual modulation and the biannual mode in particular could provide another handle in searching for Dark Matter in the laboratory.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/statistical-tests-of-noise-and-harmony-in-dark-matter-modulation-signals-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Investigation of the Progenitors of Nova Explosions [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/investigation-of-the-progenitors-of-nova-explosions-replacement/</link>
		<comments>http://voxcharta.org/2012/02/21/investigation-of-the-progenitors-of-nova-explosions-replacement/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:37:51 +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[binary system]]></category>
		<category><![CDATA[cne]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[explosion]]></category>
		<category><![CDATA[initial targets]]></category>
		<category><![CDATA[liverpool telescope]]></category>
		<category><![CDATA[outburst]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[photometric observations]]></category>
		<category><![CDATA[population]]></category>
		<category><![CDATA[preliminary investigation]]></category>
		<category><![CDATA[preliminary results]]></category>
		<category><![CDATA[progenitor]]></category>
		<category><![CDATA[recurrent novae]]></category>
		<category><![CDATA[rs oph]]></category>
		<category><![CDATA[sco]]></category>
		<category><![CDATA[SNe]]></category>
		<category><![CDATA[type ia]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/investigation-of-the-progenitors-of-nova-explosions-replacement/</guid>
		<description><![CDATA[Recurrent novae (RNe) play an important role as one of the suspected progenitor systems of Type Ia supernovae (SNe) which are used as primary distance indicators in cosmology. Thus, it is important to investigate the nature of their central binary systems to determine the relation between the parameters of the central system and outburst type, [...]]]></description>
			<content:encoded><![CDATA[<p>Recurrent novae (RNe) play an important role as one of the suspected progenitor systems of Type Ia supernovae (SNe) which are used as primary distance indicators in cosmology. Thus, it is important to investigate the nature of their central binary systems to determine the relation between the parameters of the central system and outburst type, and finally ascertain the population of novae that might be available to give rise to the progenitors of Type Ia SNe. The details of the preliminary investigation looking for characteristics that may distinguish recurrent and classical novae (CNe) systems, the selection of initial targets for detailed study, and preliminary results are presented. We identified 10 suspected RNe among the Galactic CNe for investigation with the Liverpool Telescope population and our initial photometric observations of their quiescent systems suggest 2 may belong to the RS Oph type and 2 to the U Sco type RNe. Spectroscopic follow-up is now underway.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/investigation-of-the-progenitors-of-nova-explosions-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Application of cross correlations between CMB and large scale structure to constraints on the primordial non-Gaussianity [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/application-of-cross-correlations-between-cmb-and-large-scale-structure-to-constraints-on-the-primordial-non-gaussianity-replacement/</link>
		<comments>http://voxcharta.org/2012/02/21/application-of-cross-correlations-between-cmb-and-large-scale-structure-to-constraints-on-the-primordial-non-gaussianity-replacement/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:37:37 +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[angular distribution]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[cross correlation]]></category>
		<category><![CDATA[dark matter halo]]></category>
		<category><![CDATA[Delta]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[fisher]]></category>
		<category><![CDATA[fNL]]></category>
		<category><![CDATA[galaxy galaxy]]></category>
		<category><![CDATA[hsc]]></category>
		<category><![CDATA[hyper]]></category>
		<category><![CDATA[matrix method]]></category>
		<category><![CDATA[planck]]></category>
		<category><![CDATA[power spectra]]></category>
		<category><![CDATA[scale structure]]></category>
		<category><![CDATA[survey]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/application-of-cross-correlations-between-cmb-and-large-scale-structure-to-constraints-on-the-primordial-non-gaussianity-replacement/</guid>
		<description><![CDATA[The primordial non-Gaussianity of local type affects the clustering of dark matter halos, and the planned deep and wide photometric surveys are suitable for examining this class of non-Gaussianity. In our previous paper, we investigated the constraint from the cross correlation between CMB lensing potential and galaxy angular distribution on the primordial non-Gaussianity, without taking [...]]]></description>
			<content:encoded><![CDATA[<p>The primordial non-Gaussianity of local type affects the clustering of dark matter halos, and the planned deep and wide photometric surveys are suitable for examining this class of non-Gaussianity. In our previous paper, we investigated the constraint from the cross correlation between CMB lensing potential and galaxy angular distribution on the primordial non-Gaussianity, without taking into account redshift slicing. To improve our previous analysis, in this paper, we add the galaxy lensing shear into our analysis and take into account redshift slicing to follow the redshift evolution of the clustering. By calculating 81 power spectra and using the Fisher matrix method, we find that the constraint on the primordial non-Gaussianity can be improved from {\Delta}fNL \sim 5.4 to 5.1 by including the galaxy-galaxy lensing shear cross correlations expected from the Hyper Suprime-Cam survey (HSC), in comparison with the constraint without any cross correlations. Moreover, the constraint can go down to {\Delta}fNL \sim 4.8 by including the galaxy-CMB lensing cross correlations from the ACTPol and Planck experiments.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/application-of-cross-correlations-between-cmb-and-large-scale-structure-to-constraints-on-the-primordial-non-gaussianity-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Detection of very-high energy \gamma-ray emission from NGC 1275 by the MAGIC telescopes [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/detection-of-very-high-energy-gamma-ray-emission-from-ngc-1275-by-the-magic-telescopes-replacement-2/</link>
		<comments>http://voxcharta.org/2012/02/21/detection-of-very-high-energy-gamma-ray-emission-from-ngc-1275-by-the-magic-telescopes-replacement-2/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:37:24 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[6 sigma]]></category>
		<category><![CDATA[central radio]]></category>
		<category><![CDATA[cluster of galaxies]]></category>
		<category><![CDATA[cm 2]]></category>
		<category><![CDATA[differential]]></category>
		<category><![CDATA[energy spectrum]]></category>
		<category><![CDATA[factor 3]]></category>
		<category><![CDATA[galaxy ic]]></category>
		<category><![CDATA[gamma ray emission]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[light curve]]></category>
		<category><![CDATA[mev]]></category>
		<category><![CDATA[perseus cluster]]></category>
		<category><![CDATA[radio galaxy]]></category>
		<category><![CDATA[scale variability
