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<channel>
	<title>Vox Charta &#187; Cosmology and Extragalactic</title>
	<atom:link href="http://voxcharta.org/category/astro-ph/cosmology-extragalactic-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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			<item>
		<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>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>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>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>
		</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>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>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>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/evolutionary-synthesis-models-as-a-tool-and-guide-towards-the-first-galaxies/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<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>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>
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		<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>
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		<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>
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		<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>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>
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		<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>
		</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>
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		<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>
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		<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>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>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>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/the-dust-scaling-relations-of-the-herschel-reference-survey-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<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>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>
		</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>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>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>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>
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		<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>
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		<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>
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		<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>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>
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		<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>
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		<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>
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		<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>
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		<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>
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		<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>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>
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		<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>
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		<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>
		</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>
		</item>
		<item>
		<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 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>
		</item>
		<item>
		<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>
		</item>
		<item>
		<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>Dirac equation in a de Sitter expansion for massive neutrinos from modern Kaluza-Klein theory [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/dirac-equation-in-a-de-sitter-expansion-for-massive-neutrinos-from-modern-kaluza-klein-theory-replacement-2/</link>
		<comments>http://voxcharta.org/2012/02/21/dirac-equation-in-a-de-sitter-expansion-for-massive-neutrinos-from-modern-kaluza-klein-theory-replacement-2/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:37:06 +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[de sitter]]></category>
		<category><![CDATA[dirac equation]]></category>
		<category><![CDATA[foliation]]></category>
		<category><![CDATA[kaluza klein theory]]></category>
		<category><![CDATA[massive neutrinos]]></category>
		<category><![CDATA[matter theory]]></category>
		<category><![CDATA[ricci]]></category>
		<category><![CDATA[theory of gravity]]></category>
		<category><![CDATA[vacuum]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/dirac-equation-in-a-de-sitter-expansion-for-massive-neutrinos-from-modern-kaluza-klein-theory-replacement-2/</guid>
		<description><![CDATA[Using the modern Kaluza-Klein theory of gravity (or the Induced Matter theory), we study the Dirac equation for massive neutrinos on a de Sitter background metric from a 5D Riemann-flat (and hence Ricci-flat) extended de Sitter metric, on which is defined the vacuum for test massless 1/2-neutral fields minimally coupled to gravity and free of [...]]]></description>
			<content:encoded><![CDATA[<p>Using the modern Kaluza-Klein theory of gravity (or the Induced Matter theory), we study the Dirac equation for massive neutrinos on a de Sitter background metric from a 5D Riemann-flat (and hence Ricci-flat) extended de Sitter metric, on which is defined the vacuum for test massless 1/2-neutral fields minimally coupled to gravity and free of any other interactions. We obtain that the effective 4D masses of the neutrinos can only take three possible values, which are related to the (static) foliation of the fifth and noncompact extra dimension.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/dirac-equation-in-a-de-sitter-expansion-for-massive-neutrinos-from-modern-kaluza-klein-theory-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Testing Different Formulations of MOND Using LISA Pathfinder [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/testing-different-formulations-of-mond-using-lisa-pathfinder-replacement/</link>
		<comments>http://voxcharta.org/2012/02/21/testing-different-formulations-of-mond-using-lisa-pathfinder-replacement/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:36:48 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[gravitational potential]]></category>
		<category><![CDATA[impact parameter]]></category>
		<category><![CDATA[lpf]]></category>
		<category><![CDATA[modified newtonian dynamics]]></category>
		<category><![CDATA[negative result]]></category>
		<category><![CDATA[pathfinder]]></category>
		<category><![CDATA[poisson equation]]></category>
		<category><![CDATA[quantitative and qualitative analysis]]></category>
		<category><![CDATA[saddle point]]></category>
		<category><![CDATA[signal to noise]]></category>
		<category><![CDATA[signal to noise ratio]]></category>
		<category><![CDATA[typical signal]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/testing-different-formulations-of-mond-using-lisa-pathfinder-replacement/</guid>
		<description><![CDATA[Previously it has been shown that MOdified Newtonian Dynamics (MOND) can be tested near the saddle points of the Newtonian gravitational potential using the forthcoming LISA Pathfinder (LPF) mission. These analysis focused on one particular formulation of the MONDian theory, which centered around a particular modified Poisson equation. We show that, in addition to the [...]]]></description>
			<content:encoded><![CDATA[<p>Previously it has been shown that MOdified Newtonian Dynamics (MOND) can be tested near the saddle points of the Newtonian gravitational potential using the forthcoming LISA Pathfinder (LPF) mission. These analysis focused on one particular formulation of the MONDian theory, which centered around a particular modified Poisson equation. We show that, in addition to the well known AQUAL formulation, another possibility exists in the form of a driven Poisson equation for the MONDian field. We consider similar quantitative and qualitative analysis for this formulation and also investigate typical Signal to Noise Ratios (SNR) resulting from these theories for a LPF test. We demonstrate that for a typical 50 km saddle flyby, the SNR is amplified by 25% between the two formulations. We also suggest that the SNR remains enhanced for impact parameters of 1000km or larger. Finally we show that constraints from a negative result remain as good, but no better between different formulations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/testing-different-formulations-of-mond-using-lisa-pathfinder-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Herschel-ATLAS/GAMA: a census of dust in optically selected galaxies from stacking at submillimetre wavelengths [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/herschel-atlasgama-a-census-of-dust-in-optically-selected-galaxies-from-stacking-at-submillimetre-wavelengths-replacement/</link>
		<comments>http://voxcharta.org/2012/02/21/herschel-atlasgama-a-census-of-dust-in-optically-selected-galaxies-from-stacking-at-submillimetre-wavelengths-replacement/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:36:31 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[atlas]]></category>
		<category><![CDATA[colours]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[deg]]></category>
		<category><![CDATA[dust emission]]></category>
		<category><![CDATA[emission properties]]></category>
		<category><![CDATA[galaxy population]]></category>
		<category><![CDATA[herschel]]></category>
		<category><![CDATA[mass ratio]]></category>
		<category><![CDATA[obscuration]]></category>
		<category><![CDATA[redshift galaxies]]></category>
		<category><![CDATA[rest frame]]></category>
		<category><![CDATA[stack]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[statistical study]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[submillimetre wavelengths]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/herschel-atlasgama-a-census-of-dust-in-optically-selected-galaxies-from-stacking-at-submillimetre-wavelengths-replacement/</guid>
		<description><![CDATA[We use the Herschel-ATLAS survey to conduct the first large-scale statistical study of the submm properties of optically selected galaxies. Using ~80,000 r-band selected galaxies from 126 deg^2 of the GAMA survey, we stack into submm imaging at 250, 350 and 500{\mu}m to gain unprecedented statistics on the dust emission from galaxies at z &#60; [...]]]></description>
			<content:encoded><![CDATA[<p>We use the Herschel-ATLAS survey to conduct the first large-scale statistical study of the submm properties of optically selected galaxies. Using ~80,000 r-band selected galaxies from 126 deg^2 of the GAMA survey, we stack into submm imaging at 250, 350 and 500{\mu}m to gain unprecedented statistics on the dust emission from galaxies at z &lt; 0.35. We find that low redshift galaxies account for 5% of the cosmic 250{\mu}m background (4% at 350{\mu}m; 3% at 500{\mu}m), of which approximately 60% comes from &#039;blue&#039; and 20% from &#039;red&#039; galaxies (rest-frame g &#8211; r). We compare the dust properties of different galaxy populations by dividing the sample into bins of optical luminosity, stellar mass, colour and redshift. In blue galaxies we find that dust temperature and luminosity correlate strongly with stellar mass at a fixed redshift, but red galaxies do not follow these correlations and overall have lower luminosities and temperatures. We make reasonable assumptions to account for the contaminating flux from lensing by red sequence galaxies and conclude that galaxies with different optical colours have fundamentally different dust emission properties. Results indicate that while blue galaxies are more luminous than red galaxies due to higher temperatures, the dust masses of the two samples are relatively similar. Dust mass is shown to correlate with stellar mass, although the dust/stellar mass ratio is much higher for low stellar mass galaxies, consistent with the lowest mass galaxies having the highest specific star formation rates. We stack the 250{\mu}m/NUV luminosity ratio, finding results consistent with greater obscuration of star formation at lower stellar mass and higher redshift. Submm luminosities and dust masses of all galaxies are shown to evolve strongly with redshift, indicating a fall in the amount of obscured star formation in ordinary galaxies over the last four billion years.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/herschel-atlasgama-a-census-of-dust-in-optically-selected-galaxies-from-stacking-at-submillimetre-wavelengths-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Local Simulations of Instabilities in Relativistic Jets I: Morphology and Energetics of the Current-Driven Instability [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/local-simulations-of-instabilities-in-relativistic-jets-i-morphology-and-energetics-of-the-current-driven-instability-replacement/</link>
		<comments>http://voxcharta.org/2012/02/21/local-simulations-of-instabilities-in-relativistic-jets-i-morphology-and-energetics-of-the-current-driven-instability-replacement/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:36:17 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[amplification]]></category>
		<category><![CDATA[analytic model]]></category>
		<category><![CDATA[deform]]></category>
		<category><![CDATA[driven instabilities]]></category>
		<category><![CDATA[energetics]]></category>
		<category><![CDATA[equipartition]]></category>
		<category><![CDATA[flow morphology]]></category>
		<category><![CDATA[force balance]]></category>
		<category><![CDATA[free model]]></category>
		<category><![CDATA[initial force]]></category>
		<category><![CDATA[kinetic energy]]></category>
		<category><![CDATA[linear growth]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetic force]]></category>
		<category><![CDATA[magnetic pressure]]></category>
		<category><![CDATA[numerical investigation]]></category>
		<category><![CDATA[physical parameter]]></category>
		<category><![CDATA[pressure gradient]]></category>
		<category><![CDATA[radial force]]></category>
		<category><![CDATA[relativistic jet]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/local-simulations-of-instabilities-in-relativistic-jets-i-morphology-and-energetics-of-the-current-driven-instability-replacement/</guid>
		<description><![CDATA[We present the results of a numerical investigation of current-driven instability in magnetized jets. Utilizing the well-tested, relativistic magnetohydrodynamic code Athena, we construct an ensemble of local, co-moving plasma columns in which initial radial force balance is achieved through various combinations of magnetic, pressure, and rotational forces. We then examine the resulting flow morphologies and [...]]]></description>
			<content:encoded><![CDATA[<p>We present the results of a numerical investigation of current-driven instability in magnetized jets. Utilizing the well-tested, relativistic magnetohydrodynamic code Athena, we construct an ensemble of local, co-moving plasma columns in which initial radial force balance is achieved through various combinations of magnetic, pressure, and rotational forces. We then examine the resulting flow morphologies and energetics to determine the degree to which these systems become disrupted, the amount of kinetic energy amplification attained, and the non-linear saturation behaviors. Our most significant finding is that the details of initial force balance have a pronounced effect on the resulting flow morphology. Models in which the initial magnetic field is force-free deform, but do not become disrupted. Systems that achieve initial equilibrium by balancing pressure gradients and/or rotation against magnetic forces, however, tend to shred, mix, and develop turbulence. In all cases, the linear growth of current-driven instabilities is well-represented by analytic models. CDI-driven kinetic energy amplification is slower and saturates at a lower value in force-free models than in those that feature pressure gradients and/or rotation. In rotating columns, we find that magnetized regions undergoing rotational shear are driven toward equipartition between kinetic and magnetic energies. We show that these results are applicable for a large variety of physical parameters, but we caution that algorithmic decisions (such as choice of Riemann solver) can affect the evolution of these systems more than physically motivated parameters.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/local-simulations-of-instabilities-in-relativistic-jets-i-morphology-and-energetics-of-the-current-driven-instability-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Gravity and Large-Scale Non-local Bias [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/gravity-and-large-scale-non-local-bias-replacement/</link>
		<comments>http://voxcharta.org/2012/02/21/gravity-and-large-scale-non-local-bias-replacement/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:36:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bia]]></category>
		<category><![CDATA[cosmological parameters]]></category>
		<category><![CDATA[deformation]]></category>
		<category><![CDATA[density measurement]]></category>
		<category><![CDATA[departures]]></category>
		<category><![CDATA[dependence]]></category>
		<category><![CDATA[dipole field]]></category>
		<category><![CDATA[formalism]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[invariant]]></category>
		<category><![CDATA[luminous galaxies]]></category>
		<category><![CDATA[matter density]]></category>
		<category><![CDATA[non locality]]></category>
		<category><![CDATA[number density]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[time evolution]]></category>
		<category><![CDATA[tracers]]></category>
		<category><![CDATA[triangle shape]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/gravity-and-large-scale-non-local-bias-replacement/</guid>
		<description><![CDATA[The relationship between galaxy and matter overdensities, bias, is most often assumed to be local. This is however unstable under time evolution, we provide proofs under several sets of assumptions. In the simplest model galaxies are created locally and linearly biased at a single time, and subsequently move with the matter (no velocity bias) conserving [...]]]></description>
			<content:encoded><![CDATA[<p>The relationship between galaxy and matter overdensities, bias, is most often assumed to be local. This is however unstable under time evolution, we provide proofs under several sets of assumptions. In the simplest model galaxies are created locally and linearly biased at a single time, and subsequently move with the matter (no velocity bias) conserving their comoving number density (no merging). We show that, after this formation time, the bias becomes unavoidably non-local and non-linear at large scales. We identify the non-local gravitationally induced fields in which the galaxy overdensity can be expanded, showing that they can be constructed out of the invariants of the deformation tensor (Galileons). In addition, we show that this result persists if we include an arbitrary evolution of the comoving number density of tracers. We then include velocity bias, and show that new contributions appear, a dipole field being the signature at second order. We test these predictions by studying the dependence of halo overdensities in cells of fixed matter density: measurements in simulations show that departures from the mean bias relation are strongly correlated with the non-local gravitationally induced fields identified by our formalism. The effects on non-local bias seen in the simulations are most important for the most biased halos, as expected from our predictions. The non-locality seen in the simulations is not fully captured by assuming local bias in Lagrangian space. Accounting for these effects when modeling galaxy bias is essential for correctly describing the dependence on triangle shape of the galaxy bispectrum, and hence constraining cosmological parameters and primordial non-Gaussianity. We show that using our formalism we remove an important systematic in the determination of bias parameters from the galaxy bispectrum, particularly for luminous galaxies. (abridged)</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/gravity-and-large-scale-non-local-bias-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Internal Stellar Kinematics of M32 from the SPLASH Survey: Dark Halo Constraints and the Formation of Compact Elliptical Galaxies [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/internal-stellar-kinematics-of-m32-from-the-splash-survey-dark-halo-constraints-and-the-formation-of-compact-elliptical-galaxies-replacement-2/</link>
		<comments>http://voxcharta.org/2012/02/21/internal-stellar-kinematics-of-m32-from-the-splash-survey-dark-halo-constraints-and-the-formation-of-compact-elliptical-galaxies-replacement-2/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:34:47 +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[andromeda galaxy m31]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[dark halo]]></category>
		<category><![CDATA[deimos]]></category>
		<category><![CDATA[elliptical galaxy]]></category>
		<category><![CDATA[keck]]></category>
		<category><![CDATA[m32]]></category>
		<category><![CDATA[neighbor]]></category>
		<category><![CDATA[satellite]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[stellar kinematics]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/internal-stellar-kinematics-of-m32-from-the-splash-survey-dark-halo-constraints-and-the-formation-of-compact-elliptical-galaxies-replacement-2/</guid>
		<description><![CDATA[As part of the SPLASH survey of the Andromeda galaxy (M31) and its neighbors, we have obtained Keck/DEIMOS spectra of the compact elliptical (cE) satellite M32. This is the first resolved-star kinematical study of any cE galaxy. In contrast to previous studies that extended out to r&#60;30&#34;~1Re~100pc, we measure the rotation curve and velocity dispersion [...]]]></description>
			<content:encoded><![CDATA[<p>As part of the SPLASH survey of the Andromeda galaxy (M31) and its neighbors, we have obtained Keck/DEIMOS spectra of the compact elliptical (cE) satellite M32. This is the first resolved-star kinematical study of any cE galaxy. In contrast to previous studies that extended out to r&lt;30&quot;~1Re~100pc, we measure the rotation curve and velocity dispersion profile out to r~250&quot; and higher order Gauss-Hermite moments out to r~70&quot;. We achieve this by combining integrated-light spectroscopy at small radii (where crowding/blending are severe) with resolved stellar spectroscopy at larger radii, using spatial and kinematical information to statistically account for M31 contamination. The rotation curve and velocity dispersion profile extend well beyond the radius (r~150&quot;) where the isophotes are distorted. Unlike NGC 205, another close dwarf companion of M31, M32&#039;s kinematic are regular and symmetric and do not show obvious sharp gradients across the region of isophotal elongation and twists. We interpret M32&#039;s kinematics using three-integral axisymmetric dynamical equilibrium models constructed using Schwarzschild&#039;s orbit superposition technique. Models with a constant M/L can fit the data remarkably well. However, since such a model requires an increasing tangential anisotropy with radius, invoking the presence of an extended dark halo may be more plausible. Such an extended dark halo is definitely required to bind a half-dozen fast-moving stars observed at the largest radii, but these stars may not be an equilibrium component of M32. The observed regularity of the stellar kinematics, as well as the possible detection of an extended dark halo, are unexpected if M31 tides are significant at large radii. While these findings by themselves do not rule out tidal models for cE formation, they suggest that tidal stripping may not be as significant for shaping cE galaxies as has often been argued.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/internal-stellar-kinematics-of-m32-from-the-splash-survey-dark-halo-constraints-and-the-formation-of-compact-elliptical-galaxies-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Cosmological Constraint and Analysis on Holographic Dark Energy Model Characterized by the Conformal-age-like Length [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/cosmological-constraint-and-analysis-on-holographic-dark-energy-model-characterized-by-the-conformal-age-like-length-replacement/</link>
		<comments>http://voxcharta.org/2012/02/21/cosmological-constraint-and-analysis-on-holographic-dark-energy-model-characterized-by-the-conformal-age-like-length-replacement/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:34:31 +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[best fit]]></category>
		<category><![CDATA[confidence level]]></category>
		<category><![CDATA[cosmic microwave background]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[deceleration parameter]]></category>
		<category><![CDATA[density of matter]]></category>
		<category><![CDATA[digital sky survey]]></category>
		<category><![CDATA[energy density]]></category>
		<category><![CDATA[energy model]]></category>
		<category><![CDATA[equation of state]]></category>
		<category><![CDATA[hubble space telescope]]></category>
		<category><![CDATA[microwave anisotropy probe]]></category>
		<category><![CDATA[microwave background radiation]]></category>
		<category><![CDATA[radiation data]]></category>
		<category><![CDATA[sky survey data]]></category>
		<category><![CDATA[sloan digital]]></category>
		<category><![CDATA[systematic analysis]]></category>
		<category><![CDATA[wide field camera]]></category>
		<category><![CDATA[wilkinson microwave anisotropy]]></category>
		<category><![CDATA[wilkinson microwave anisotropy probe]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/cosmological-constraint-and-analysis-on-holographic-dark-energy-model-characterized-by-the-conformal-age-like-length-replacement/</guid>
		<description><![CDATA[We present a best-fit analysis on the holographic dark energy model characterized by the conformal-age-like length. Based on the Union2 compilation of 557 supernova Ia data, the baryon acoustic oscillation results from the Sloan Digital Sky Survey data release 7, the cosmic microwave background radiation data from the 7-yr Wilkinson Microwave Anisotropy Probe and the [...]]]></description>
			<content:encoded><![CDATA[<p>We present a best-fit analysis on the holographic dark energy model characterized by the conformal-age-like length. Based on the Union2 compilation of 557 supernova Ia data, the baryon acoustic oscillation results from the Sloan Digital Sky Survey data release 7, the cosmic microwave background radiation data from the 7-yr Wilkinson Microwave Anisotropy Probe and the Hubble constant measurement from the Wide Field Camera 3 on the Hubble Space Telescope, we show that the model gives the minimal $\chi^2_{min}=549.428$, which is comparable to $\chi^2_{\Lambda {\rm CDM}}=546.478$ for the $\Lambda$CDM model. The single parameter $d$ concerned in the model is found to be $d=0.235^{+0.005}_{-0.005} ^{+0.008}_{-0.009}$ at 1 $\sigma$ and 2 $\sigma$ confidence levels. The resulting constraints on the present fractional energy density of matter and the equation of state are $\Omega_{m}=0.278^{+0.017}_{-0.016} ^{+0.028}_{-0.026}$ and $w_{de}=-1.252^{+0.025}_{-0.025} ^{+0.042}_{-0.041}$ respectively. The model leads to a slightly larger fraction of matter comparing to the $\Lambda$CDM model. We also provide a systematic analysis on the cosmic evolutions of the fractional energy density of dark energy, the equation of state of dark energy, the deceleration parameter and the statefinder. It is noticed that the equation of state crosses from $w_{de}&gt;-1$ to $w_{de}0$) to accelerated expansion ($q&lt;0$) recently, and the statefinder may serve as a sensitive diagnostic to distinguish the CHDE model with the $\Lambda$CDM model.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/cosmological-constraint-and-analysis-on-holographic-dark-energy-model-characterized-by-the-conformal-age-like-length-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Measuring X-ray variability in faint/sparsely-sampled AGN [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/measuring-x-ray-variability-in-faintsparsely-sampled-agn-replacement/</link>
		<comments>http://voxcharta.org/2012/02/21/measuring-x-ray-variability-in-faintsparsely-sampled-agn-replacement/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:33:47 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[biases]]></category>
		<category><![CDATA[cdf]]></category>
		<category><![CDATA[Chandra]]></category>
		<category><![CDATA[future x]]></category>
		<category><![CDATA[lightcurve]]></category>
		<category><![CDATA[maximum likelihood]]></category>
		<category><![CDATA[measurement error]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[monte carlo simulation]]></category>
		<category><![CDATA[population]]></category>
		<category><![CDATA[sampling pattern]]></category>
		<category><![CDATA[statistic]]></category>
		<category><![CDATA[uncertainty]]></category>
		<category><![CDATA[uniform sampling]]></category>
		<category><![CDATA[variability]]></category>
		<category><![CDATA[variance]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xmm newton]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/measuring-x-ray-variability-in-faintsparsely-sampled-agn-replacement/</guid>
		<description><![CDATA[We discuss some practical aspects of measuring the variability amplitude of faint and distant active galactic nuclei (AGN), characterized by sparsely sampled lightcurves and low statistic. In such cases the excess variance, commonly used to estimate the intrinsic lightcurve variance, is affected by strong biases and uncertainties since it represents a maximum likelihood variability estimator [...]]]></description>
			<content:encoded><![CDATA[<p>We discuss some practical aspects of measuring the variability amplitude of faint and distant active galactic nuclei (AGN), characterized by sparsely sampled lightcurves and low statistic. In such cases the excess variance, commonly used to estimate the intrinsic lightcurve variance, is affected by strong biases and uncertainties since it represents a maximum likelihood variability estimator only for identical/normal distributed measurements errors and uniform sampling. We performed realistic Monte Carlo simulations of AGN lightcurves, reproducing both the sampling pattern and measurement errors typical of multi-epoch deep surveys, such as the XMM-Newton observations of the Chandra Deep Field South (CDFS), or assuming different sampling patterns that may characterize long surveys with sub-optimal observing conditions. We used the results to estimate our ability to measure the intrinsic source variability as well as to constrain the observing strategy of future X-ray missions studying distant and/or faint AGN populations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/measuring-x-ray-variability-in-faintsparsely-sampled-agn-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Holographic Dark Energy Characterized by the Total Comoving Horizon and Insights to Cosmological Constant and Coincidence Problem [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/holographic-dark-energy-characterized-by-the-total-comoving-horizon-and-insights-to-cosmological-constant-and-coincidence-problem-replacement/</link>
		<comments>http://voxcharta.org/2012/02/21/holographic-dark-energy-characterized-by-the-total-comoving-horizon-and-insights-to-cosmological-constant-and-coincidence-problem-replacement/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:32:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration]]></category>
		<category><![CDATA[best fit]]></category>
		<category><![CDATA[coincidence]]></category>
		<category><![CDATA[consequence]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[cosmological constant]]></category>
		<category><![CDATA[cosmological observations]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[early universe]]></category>
		<category><![CDATA[horizon]]></category>
		<category><![CDATA[inflation]]></category>
		<category><![CDATA[inflationary universe]]></category>
		<category><![CDATA[insight]]></category>
		<category><![CDATA[principle]]></category>
		<category><![CDATA[systematic analysis]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/holographic-dark-energy-characterized-by-the-total-comoving-horizon-and-insights-to-cosmological-constant-and-coincidence-problem-replacement/</guid>
		<description><![CDATA[The observed acceleration of the present universe is shown to be well explained by the holographic dark energy characterized by the total comoving horizon of the universe ($\eta$HDE). It is of interest to notice that the very large primordial part of the comoving horizon generated by the inflation of early universe makes the $\eta$HDE behave [...]]]></description>
			<content:encoded><![CDATA[<p>The observed acceleration of the present universe is shown to be well explained by the holographic dark energy characterized by the total comoving horizon of the universe ($\eta$HDE). It is of interest to notice that the very large primordial part of the comoving horizon generated by the inflation of early universe makes the $\eta$HDE behave like a cosmological constant. As a consequence, both the fine-tuning problem and the coincidence problem can reasonably be understood with the inflationary universe and holographical principle. We present a systematic analysis and obtain a consistent cosmological constraint on the $\eta$HDE model based on the recent cosmological observations. It is found that the $\eta$HDE model gives the best-fit result $\Omega_{m0}=0.270$ ($\Omega_{de0}=0.730$) and the minimal $\chi^2_{min}=542.915$ which is compatible with $\chi^2_{\Lambda {\rm CDM}}=542.919$ for the $\Lambda$CDM model.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/holographic-dark-energy-characterized-by-the-total-comoving-horizon-and-insights-to-cosmological-constant-and-coincidence-problem-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A Density Independent Formulation of Smoothed Particle Hydrodynamics [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/a-density-independent-formulation-of-smoothed-particle-hydrodynamics-replacement/</link>
		<comments>http://voxcharta.org/2012/02/21/a-density-independent-formulation-of-smoothed-particle-hydrodynamics-replacement/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:31:25 +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[astronomical object]]></category>
		<category><![CDATA[blob]]></category>
		<category><![CDATA[density distribution]]></category>
		<category><![CDATA[differentiability]]></category>
		<category><![CDATA[discontinuity]]></category>
		<category><![CDATA[energy conservation]]></category>
		<category><![CDATA[helmholtz]]></category>
		<category><![CDATA[high density]]></category>
		<category><![CDATA[kelvin]]></category>
		<category><![CDATA[low density]]></category>
		<category><![CDATA[numerical diffusion]]></category>
		<category><![CDATA[numerical problem]]></category>
		<category><![CDATA[particle hydrodynamics]]></category>
		<category><![CDATA[rayleigh]]></category>
		<category><![CDATA[repulsive force]]></category>
		<category><![CDATA[shock tube]]></category>
		<category><![CDATA[spatial derivatives]]></category>
		<category><![CDATA[sph]]></category>
		<category><![CDATA[surface tension]]></category>
		<category><![CDATA[symmetry]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/a-density-independent-formulation-of-smoothed-particle-hydrodynamics-replacement/</guid>
		<description><![CDATA[In the standard formulation of the smoothed particle hydrodynamics (SPH), it is assumed that the local density distribution is differentiable. This assumption is used to derive the spatial derivatives of other quantities. However, this assumption breaks down at the contact discontinuity, which appears often in simulations of astronomical objects. At the contact discontinuity, the density [...]]]></description>
			<content:encoded><![CDATA[<p>In the standard formulation of the smoothed particle hydrodynamics (SPH), it is assumed that the local density distribution is differentiable. This assumption is used to derive the spatial derivatives of other quantities. However, this assumption breaks down at the contact discontinuity, which appears often in simulations of astronomical objects. At the contact discontinuity, the density of the low-density side is overestimated while that of the high-density side is underestimated. As a result, the pressure of the low (high) density side is over (under) estimated. Thus, unphysical repulsive force appears at the contact discontinuity, resulting in the effective surface tension. This effective surface tension suppresses instabilities such as the Kelvin-Helmholtz and Rayleigh-Taylor instabilities. In this paper, we present a new formulation of SPH, which does not require the differentiability of density and thus can handle contact discontinuity without numerical problems. The results of standard tests such as the shock tube, Kelvin-Helmholtz and Rayleigh-Taylor instabilities, and the blob tests are all very favorable to our new formulation. We conclude that our new formulation solved practically all known difficulties of the standard SPH, without introducing additional numerical diffusion or breaking the exact force symmetry or energy conservation.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/a-density-independent-formulation-of-smoothed-particle-hydrodynamics-replacement/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/2012/02/21/future-constraints-on-variations-of-the-fine-structure-constant-from-combined-cmb-and-weak-lensing-measurements-replacement/</link>
		<comments>http://voxcharta.org/2012/02/21/future-constraints-on-variations-of-the-fine-structure-constant-from-combined-cmb-and-weak-lensing-measurements-replacement/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:31:06 +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/2012/02/21/future-constraints-on-variations-of-the-fine-structure-constant-from-combined-cmb-and-weak-lensing-measurements-replacement/</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/2012/02/21/future-constraints-on-variations-of-the-fine-structure-constant-from-combined-cmb-and-weak-lensing-measurements-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Prospects for early localization of gravitational-wave signals from compact binary coalescences with advanced detectors [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/20/prospects-for-early-localization-of-gravitational-wave-signals-from-compact-binary-coalescences-with-advanced-detectors-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/20/prospects-for-early-localization-of-gravitational-wave-signals-from-compact-binary-coalescences-with-advanced-detectors-cross-listing/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 02:08:10 +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[aligo]]></category>
		<category><![CDATA[candidate source]]></category>
		<category><![CDATA[coalescence]]></category>
		<category><![CDATA[compact object]]></category>
		<category><![CDATA[earlier times]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[inspiral]]></category>
		<category><![CDATA[interferometer]]></category>
		<category><![CDATA[ligo]]></category>
		<category><![CDATA[localization]]></category>
		<category><![CDATA[massive system]]></category>
		<category><![CDATA[monte carlo technique]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[prospects]]></category>
		<category><![CDATA[sky area]]></category>
		<category><![CDATA[source location]]></category>
		<category><![CDATA[timing accuracy]]></category>
		<category><![CDATA[triangulation]]></category>
		<category><![CDATA[wave signals]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/prospects-for-early-localization-of-gravitational-wave-signals-from-compact-binary-coalescences-with-advanced-detectors-cross-listing/</guid>
		<description><![CDATA[A leading candidate source of detectable gravitational waves is the inspiral and merger of pairs of stellar-mass compact objects. The advanced LIGO and advanced Virgo detectors will allow scientists to detect inspiral signals from more massive systems and at earlier times in the detector band, than with first generation detectors. The signal from a coalescence [...]]]></description>
			<content:encoded><![CDATA[<p>A leading candidate source of detectable gravitational waves is the inspiral and merger of pairs of stellar-mass compact objects. The advanced LIGO and advanced Virgo detectors will allow scientists to detect inspiral signals from more massive systems and at earlier times in the detector band, than with first generation detectors. The signal from a coalescence of two neutron stars is expected to stay in the sensitive band of advanced detectors for several minutes, thus allowing detection before the final coalescence of the system. In this work, the prospects of detecting inspiral signals prior to coalescence, and the possibility to derive a suitable sky area for source locations are investigated. As a large fraction of the signal is accumulated in the last ~10 seconds prior to coalescence, bandwidth and timing accuracy are largely accrued in the very last moments prior to coalescence. We use Monte Carlo techniques to estimate the accuracy of sky localization through networks of ground-based interferometers such as aLIGO and aVirgo. With the addition of the Japanese KAGRA detector, it is shown that the detection and triangulation before coalescence may be feasible.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/prospects-for-early-localization-of-gravitational-wave-signals-from-compact-binary-coalescences-with-advanced-detectors-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Brightness and Fluctuation of the Mid-Infrared Sky from AKARI Observations towards the North Ecliptic Pole</title>
		<link>http://voxcharta.org/2012/02/20/brightness-and-fluctuation-of-the-mid-infrared-sky-from-akari-observations-towards-the-north-ecliptic-pole/</link>
		<comments>http://voxcharta.org/2012/02/20/brightness-and-fluctuation-of-the-mid-infrared-sky-from-akari-observations-towards-the-north-ecliptic-pole/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 02:06:21 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[arcsecond]]></category>
		<category><![CDATA[cold phase]]></category>
		<category><![CDATA[dominant source]]></category>
		<category><![CDATA[faint source]]></category>
		<category><![CDATA[infrared astronomical satellite]]></category>
		<category><![CDATA[infrared band]]></category>
		<category><![CDATA[infrared brightness]]></category>
		<category><![CDATA[infrared sky]]></category>
		<category><![CDATA[infrared wavelength]]></category>
		<category><![CDATA[interplanetary dust]]></category>
		<category><![CDATA[interstellar dust]]></category>
		<category><![CDATA[north ecliptic pole]]></category>
		<category><![CDATA[photon noise]]></category>
		<category><![CDATA[power spectrum]]></category>
		<category><![CDATA[scale features]]></category>
		<category><![CDATA[seasonal variation]]></category>
		<category><![CDATA[shot noise]]></category>
		<category><![CDATA[sky brightness]]></category>
		<category><![CDATA[spectrum analysis]]></category>
		<category><![CDATA[zodiacal light]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/brightness-and-fluctuation-of-the-mid-infrared-sky-from-akari-observations-towards-the-north-ecliptic-pole/</guid>
		<description><![CDATA[We present the smoothness of the mid-infrared sky from observations by the Japanese infrared astronomical satellite AKARI. AKARI monitored the north ecliptic pole (NEP) during its cold phase with nine wavebands covering from 2.4 to 24 \mu m, out of which six mid-infrared bands were used in this study. A simple sinusoidal fit to the [...]]]></description>
			<content:encoded><![CDATA[<p>We present the smoothness of the mid-infrared sky from observations by the Japanese infrared astronomical satellite AKARI. AKARI monitored the north ecliptic pole (NEP) during its cold phase with nine wavebands covering from 2.4 to 24 \mu m, out of which six mid-infrared bands were used in this study. A simple sinusoidal fit to the seasonal variation of the sky brightness shows that the mid-infrared brightness towards the NEP is not affected by small-scale features of the interplanetary dust cloud. We applied power spectrum analysis to the images in order to search for the fluctuation of the sky brightness. Observed fluctuation is explained by fluctuation of photon noise, shot noise of faint sources, and Galactic cirrus. The fluctuations at a few arcminutes scales at short mid-infrared wavelengths (7, 9, and 11 \mum) are largely caused by the diffuse Galactic light of the interstellar dust cirrus. At long mid-infrared wavelengths (15, 18, and 24 \mum), photon noise is the dominant source of fluctuation over the scale from arcseconds to a few arcminutes. The residual fluctuation power at 200&#8243; after removing these contributions is at most 1.08 \pm 0.22 nW m^-2 sr^-1 or 0.05% of the brightness at 24 \mum and at least 0.52 \pm 0.13 nW m^-2 sr^-1 or 0.02% at 18 \mum. We conclude that the upper limit of the fluctuation in the zodiacal light is 0.02% of the sky brightness.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/brightness-and-fluctuation-of-the-mid-infrared-sky-from-akari-observations-towards-the-north-ecliptic-pole/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Extending the M_(bh)-sigma diagram with dense nuclear star clusters</title>
		<link>http://voxcharta.org/2012/02/20/extending-the-m_bh-sigma-diagram-with-dense-nuclear-star-clusters/</link>
		<comments>http://voxcharta.org/2012/02/20/extending-the-m_bh-sigma-diagram-with-dense-nuclear-star-clusters/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 02:05:21 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[dwarf galaxy]]></category>
		<category><![CDATA[elliptical galaxy]]></category>
		<category><![CDATA[expectation]]></category>
		<category><![CDATA[exponent]]></category>
		<category><![CDATA[feedback mechanism]]></category>
		<category><![CDATA[galaxy merger]]></category>
		<category><![CDATA[luminous galaxies]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[observation]]></category>
		<category><![CDATA[observational result]]></category>
		<category><![CDATA[sigma 1]]></category>
		<category><![CDATA[sigma 2]]></category>
		<category><![CDATA[sigma 5]]></category>
		<category><![CDATA[star cluster]]></category>
		<category><![CDATA[stellar wind]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/extending-the-m_bh-sigma-diagram-with-dense-nuclear-star-clusters/</guid>
		<description><![CDATA[Abridged: Four new nuclear star cluster masses, M_nc, plus seven upper limits, are provided for galaxies with previously determined black hole masses, M_bh. Together with a sample of 64 galaxies with direct M_bh measurements, 13 of which additionally now have M_nc measurements rather than only upper limits, plus an additional 29 dwarf galaxies with available [...]]]></description>
			<content:encoded><![CDATA[<p>Abridged: Four new nuclear star cluster masses, M_nc, plus seven upper limits, are provided for galaxies with previously determined black hole masses, M_bh. Together with a sample of 64 galaxies with direct M_bh measurements, 13 of which additionally now have M_nc measurements rather than only upper limits, plus an additional 29 dwarf galaxies with available M_nc measurements and velocity dispersions sigma, an (M_bh + M_nc)-sigma diagram is constructed. Given that major dry galaxy merger events preserve the M_bh/L ratio, and given that L ~ sigma^5 for luminous galaxies, it is first noted that the observation M_bh ~ sigma^5 is consistent with expectations. For the fainter elliptical galaxies it is known that L ~ sigma^2, and assuming a constant M_nc/L ratio (Ferrarese et al.), the expectation that M_nc ~ sigma^2 is in broad agreement with our new observational result that M_nc ~ sigma^{1.57\pm0.24}. This exponent is however in contrast to the value of ~4 which has been reported previously and interpreted in terms of a regulating feedback mechanism from stellar winds.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/extending-the-m_bh-sigma-diagram-with-dense-nuclear-star-clusters/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Dark Energy and Fate of the Universe</title>
		<link>http://voxcharta.org/2012/02/20/dark-energy-and-fate-of-the-universe/</link>
		<comments>http://voxcharta.org/2012/02/20/dark-energy-and-fate-of-the-universe/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 02:05:02 +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[circular orbit]]></category>
		<category><![CDATA[confidence level]]></category>
		<category><![CDATA[cosmological observations]]></category>
		<category><![CDATA[cpl]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[divergence]]></category>
		<category><![CDATA[energy model]]></category>
		<category><![CDATA[fate of the universe]]></category>
		<category><![CDATA[gyr]]></category>
		<category><![CDATA[parameter space]]></category>
		<category><![CDATA[parametrization]]></category>
		<category><![CDATA[redshift]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/dark-energy-and-fate-of-the-universe/</guid>
		<description><![CDATA[We explore the ultimate fate of the Universe by using a divergence-free parametrization for dark energy $w(z)=w_0+w_a({\ln (2+z)\over 1+z}-\ln2)$. Unlike the CPL parametrization, this parametrization has well behaved, bounded behavior for both high redshifts and negative redshifts, and thus can genuinely cover many theoretical dark energy models. After constraining the parameter space of this parametrization [...]]]></description>
			<content:encoded><![CDATA[<p>We explore the ultimate fate of the Universe by using a divergence-free parametrization for dark energy $w(z)=w_0+w_a({\ln (2+z)\over 1+z}-\ln2)$. Unlike the CPL parametrization, this parametrization has well behaved, bounded behavior for both high redshifts and negative redshifts, and thus can genuinely cover many theoretical dark energy models. After constraining the parameter space of this parametrization by using the current cosmological observations, we find that, at the 95.4% confidence level, our Universe can still exist at least 16.7 Gyr before it ends in a big rip. Moreover, for the phantom energy dominated Universe, we find that a gravitationally bound system will be destroyed at a time $t \simeq P\sqrt{2|1+3w(-1)|}/[6\pi |1+w(-1)|]$, where $P$ is the period of a circular orbit around this system, before the big rip.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/dark-energy-and-fate-of-the-universe/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Axino dark matter and baryon number asymmetry from Q-ball decay in gauge mediation [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/20/axino-dark-matter-and-baryon-number-asymmetry-from-q-ball-decay-in-gauge-mediation-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/20/axino-dark-matter-and-baryon-number-asymmetry-from-q-ball-decay-in-gauge-mediation-cross-listing/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 02:04:41 +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[baryon asymmetry]]></category>
		<category><![CDATA[big bang]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[decay]]></category>
		<category><![CDATA[gauge]]></category>
		<category><![CDATA[mediation]]></category>
		<category><![CDATA[model parameter]]></category>
		<category><![CDATA[nucleon]]></category>
		<category><![CDATA[standard model]]></category>
		<category><![CDATA[supersymmetric particle]]></category>
		<category><![CDATA[universe]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/axino-dark-matter-and-baryon-number-asymmetry-from-q-ball-decay-in-gauge-mediation-cross-listing/</guid>
		<description><![CDATA[We investigate the Q-ball decay into the axino dark matter in the gauge-mediated supersymmetry breaking. In our scenario, the Q ball decays mainly into nucleons and partially into axinos to account for the baryon asymmetry and the dark matter of the universe simultaneously. The Q ball decays well before the big bang nucleosynthesis so that [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate the Q-ball decay into the axino dark matter in the gauge-mediated supersymmetry breaking. In our scenario, the Q ball decays mainly into nucleons and partially into axinos to account for the baryon asymmetry and the dark matter of the universe simultaneously. The Q ball decays well before the big bang nucleosynthesis so that it is not affected by the decay. The decay into the supersymmetric particles of the minimal supersymmetric standard model is kinematically prohibited until the very end of the decay, and we could safely make their abundances small enough for the successful big bang nucleosynthesis. We show the regions of axino model parameters and the Q-ball parameters which realize this scenario.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/axino-dark-matter-and-baryon-number-asymmetry-from-q-ball-decay-in-gauge-mediation-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Constraining dynamical dark energy with a divergence-free parametrization in the presence of spatial curvature and massive neutrinos</title>
		<link>http://voxcharta.org/2012/02/20/constraining-dynamical-dark-energy-with-a-divergence-free-parametrization-in-the-presence-of-spatial-curvature-and-massive-neutrinos/</link>
		<comments>http://voxcharta.org/2012/02/20/constraining-dynamical-dark-energy-with-a-divergence-free-parametrization-in-the-presence-of-spatial-curvature-and-massive-neutrinos/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 02:04:25 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[curvature]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[determinations]]></category>
		<category><![CDATA[divergence]]></category>
		<category><![CDATA[energy parameters]]></category>
		<category><![CDATA[flat universe]]></category>
		<category><![CDATA[hst]]></category>
		<category><![CDATA[lrg]]></category>
		<category><![CDATA[massive neutrinos]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[neutrino mass]]></category>
		<category><![CDATA[parameterization]]></category>
		<category><![CDATA[parametrization]]></category>
		<category><![CDATA[polarization data]]></category>
		<category><![CDATA[power spectrum]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[sdss]]></category>
		<category><![CDATA[type ia]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/constraining-dynamical-dark-energy-with-a-divergence-free-parametrization-in-the-presence-of-spatial-curvature-and-massive-neutrinos/</guid>
		<description><![CDATA[In this paper, we report the results of constraining the dynamical dark energy with a divergence-free parameterization, $w(z) = w_{0} + w_{a}(\frac{\ln(2+z)}{1+z}-\ln2)$, in the presence of spatial curvature and massive neutrinos, with the 7-yr WMAP temperature and polarization data, the power spectrum of LRGs derived from SDSS DR7, the Type Ia supernova data from Union2 [...]]]></description>
			<content:encoded><![CDATA[<p>In this paper, we report the results of constraining the dynamical dark energy with a divergence-free parameterization, $w(z) = w_{0} + w_{a}(\frac{\ln(2+z)}{1+z}-\ln2)$, in the presence of spatial curvature and massive neutrinos, with the 7-yr WMAP temperature and polarization data, the power spectrum of LRGs derived from SDSS DR7, the Type Ia supernova data from Union2 sample, and the new measurements of $H_0$ from HST, by using a MCMC global fit method. Our focus is on the determinations of the spatial curvature, $\Omega_k$, and the total mass of neutrinos, $\sum m_{\nu}$, in such a dynamical dark energy scenario, and the influence of these factors to the constraints on the dark energy parameters, $w_0$ and $w_a$. We show that $\Omega_k$ and $\sum m_{\nu}$ can be well constrained in this model; the 95% CL limits are: $-0.0153&lt;\Omega_k&lt;0.0167$ and $\sum m_{\nu}&lt;0.56$ eV. Comparing to the case in a flat universe, we find that the error in $w_0$ is amplified by 25.51%, and the error in $w_a$ is amplified by 0.14%; comparing to the case with a zero neutrino mass, we find that the error in $w_0$ is amplified by 12.24%, and the error in $w_a$ is amplified by 1.63%.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/constraining-dynamical-dark-energy-with-a-divergence-free-parametrization-in-the-presence-of-spatial-curvature-and-massive-neutrinos/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Gaia: a Window to Large Scale Flows</title>
		<link>http://voxcharta.org/2012/02/20/gaia-a-window-to-large-scale-flows/</link>
		<comments>http://voxcharta.org/2012/02/20/gaia-a-window-to-large-scale-flows/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 02:03:36 +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[catalog]]></category>
		<category><![CDATA[distant galaxy]]></category>
		<category><![CDATA[estimates]]></category>
		<category><![CDATA[gaia]]></category>
		<category><![CDATA[galaxy distances]]></category>
		<category><![CDATA[galaxy properties]]></category>
		<category><![CDATA[large scale]]></category>
		<category><![CDATA[line of sight]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[number of galaxies]]></category>
		<category><![CDATA[peculiar velocity]]></category>
		<category><![CDATA[probes]]></category>
		<category><![CDATA[proper motion]]></category>
		<category><![CDATA[proxy]]></category>
		<category><![CDATA[scale motions]]></category>
		<category><![CDATA[selection biases]]></category>
		<category><![CDATA[velocity field]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/gaia-a-window-to-large-scale-flows/</guid>
		<description><![CDATA[Using redshifts as proxy for galaxy distances, estimates of the 2D transverse peculiar velocities of distant galaxies ($cz\ltsim 2\times 10^4 \kms$) can be obtained from Gaia&#8217;s measurements of proper motions. Owing to the large number of galaxies expected to be observed by Gaia, these transverse velocities are likely to supersede traditional probes of the large [...]]]></description>
			<content:encoded><![CDATA[<p>Using redshifts as proxy for galaxy distances, estimates of the 2D transverse peculiar velocities of distant galaxies ($cz\ltsim 2\times 10^4 \kms$) can be obtained from Gaia&#8217;s measurements of proper motions. Owing to the large number of galaxies expected to be observed by Gaia, these transverse velocities are likely to supersede traditional probes of the large scale velocity field based on current and future distance indicator measurements. This Gaia probe of large scale motions is completely independent of any intrinsic relations between galaxy properties, hence it is essentially free of selection biases. It is also free from {homogeneous and} inhomogeneous Malmquist biases that typically plague distance indicator catalogs. Further, it provides additional information to traditional probes which yield line-of-sight peculiar velocities.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/gaia-a-window-to-large-scale-flows/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Environmental Effects on the Metal Enrichment of Low Mass Galaxies in Nearby Clusters</title>
		<link>http://voxcharta.org/2012/02/20/environmental-effects-on-the-metal-enrichment-of-low-mass-galaxies-in-nearby-clusters/</link>
		<comments>http://voxcharta.org/2012/02/20/environmental-effects-on-the-metal-enrichment-of-low-mass-galaxies-in-nearby-clusters/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 02:03:03 +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[chemical evolution]]></category>
		<category><![CDATA[chemical history]]></category>
		<category><![CDATA[cluster environment]]></category>
		<category><![CDATA[cluster galaxy]]></category>
		<category><![CDATA[cluster mass]]></category>
		<category><![CDATA[environmental processes]]></category>
		<category><![CDATA[gas content]]></category>
		<category><![CDATA[hi gas]]></category>
		<category><![CDATA[hydrodynamic model]]></category>
		<category><![CDATA[interchange]]></category>
		<category><![CDATA[mass star]]></category>
		<category><![CDATA[massive cluster]]></category>
		<category><![CDATA[metal content]]></category>
		<category><![CDATA[metal enrichment]]></category>
		<category><![CDATA[nearby cluster]]></category>
		<category><![CDATA[sdss]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[star formation history]]></category>
		<category><![CDATA[truncation]]></category>
		<category><![CDATA[vulnerable systems]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/environmental-effects-on-the-metal-enrichment-of-low-mass-galaxies-in-nearby-clusters/</guid>
		<description><![CDATA[In this paper we study the chemical history of low-mass star-forming (SF) galaxies in the local Universe clusters Coma, A1367, A779, and A634. The aim of this work is to search for the imprint of the environment on the chemical evolution of these galaxies. Galaxy chemical evolution is linked to the star formation history (SFH), [...]]]></description>
			<content:encoded><![CDATA[<p>In this paper we study the chemical history of low-mass star-forming (SF) galaxies in the local Universe clusters Coma, A1367, A779, and A634. The aim of this work is to search for the imprint of the environment on the chemical evolution of these galaxies. Galaxy chemical evolution is linked to the star formation history (SFH), as well as to the gas interchange with the environment, and low-mass galaxies are well known to be vulnerable systems to environmental processes affecting both these parameters. For our study we have used spectra from the SDSS-III DR8. We have examined the mass-metallicity relation of cluster galaxies finding well defined sequences. The slope of these sequences, for galaxies in low-mass clusters and galaxies at large cluster-centric distances, follows the predictions of recent hydrodynamic models. A flattening of this slope has been observed for galaxies located in the core of the two more massive clusters of the sample, principally in Coma, suggesting that the imprint of the cluster environment on the chemical evolution of SF galaxies should be sensitive to both the galaxy mass and the host cluster mass. The HI gas content of Coma and A1367 galaxies indicate that low-mass SF galaxies, located at the core of these clusters, have been severely affected by ram-pressure stripping. The observed mass-dependent enhancement of the metal content of low-mass galaxies in dense environments seems plausible, according to hydrodynamic simulations. This enhanced metal enrichment could be produced by the combination of effects such as wind reaccretion, due to pressure cofinement by the intra-cluster medium (ICM), and the truncation of gas infall, as a result of the ram-pressure stripping. Thus, the properties of the ICM should play an important role in the chemical evolution of low-mass galaxies in clusters.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/environmental-effects-on-the-metal-enrichment-of-low-mass-galaxies-in-nearby-clusters/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>The first IRAM/PdBI polarimetric millimeter survey of active galactic nuclei. II. Activity and properties of individual sources</title>
		<link>http://voxcharta.org/2012/02/20/the-first-irampdbi-polarimetric-millimeter-survey-of-active-galactic-nuclei-ii-activity-and-properties-of-individual-sources/</link>
		<comments>http://voxcharta.org/2012/02/20/the-first-irampdbi-polarimetric-millimeter-survey-of-active-galactic-nuclei-ii-activity-and-properties-of-individual-sources/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:58:58 +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[active galactic nuclei]]></category>
		<category><![CDATA[AGN]]></category>
		<category><![CDATA[compression factor]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[emission region]]></category>
		<category><![CDATA[frame frequency]]></category>
		<category><![CDATA[frequency range]]></category>
		<category><![CDATA[iram]]></category>
		<category><![CDATA[linear polarization]]></category>
		<category><![CDATA[magnetic field strength]]></category>
		<category><![CDATA[millimeter]]></category>
		<category><![CDATA[oblique shock]]></category>
		<category><![CDATA[observatory]]></category>
		<category><![CDATA[outflow]]></category>
		<category><![CDATA[predominant component]]></category>
		<category><![CDATA[rest frame]]></category>
		<category><![CDATA[scenarios]]></category>
		<category><![CDATA[shock]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/the-first-irampdbi-polarimetric-millimeter-survey-of-active-galactic-nuclei-ii-activity-and-properties-of-individual-sources/</guid>
		<description><![CDATA[We present an analysis of the linear polarization of six active galactic nuclei &#8211; 0415+379 (3C~111), 0507+179, 0528+134 (OG+134), 0954+658, 1418+546 (OQ+530), and 1637+574 (OS+562). Our targets were monitored from 2007 to 2011 in the observatory-frame frequency range 80-253 GHz, corresponding to a rest-frame frequency range 88-705 GHz. We find average degrees of polarization m_L [...]]]></description>
			<content:encoded><![CDATA[<p>We present an analysis of the linear polarization of six active galactic nuclei &#8211; 0415+379 (3C~111), 0507+179, 0528+134 (OG+134), 0954+658, 1418+546 (OQ+530), and 1637+574 (OS+562). Our targets were monitored from 2007 to 2011 in the observatory-frame frequency range 80-253 GHz, corresponding to a rest-frame frequency range 88-705 GHz. We find average degrees of polarization m_L ~ 2-7%; this indicates that the polarization signals are effectively averaged out by the emitter geometries. We see indication for fairly strong shocks and/or complex, variable emission region geometries in our sources, with compression factors 10 deg. An analysis of correlations between source fluxes and polarization parameter points out special cases: the presence of (at least) two distinct emission regions with different levels of polarization (for 0415+379) as well as emission from a single, predominant component (for 0507+179 and 1418+546). Regarding the evolution of flux and polarization, we find good agreement between observations and the signal predicted by &#8220;oblique shock in jet&#8221; scenarios in one source (1418+546). We attempt to derive rotation measures for all sources, leading to actual measurements for two AGN and upper limits for three sources. We derive values of RM = -39,000 +/- 1,000 (stat) +/- 13,000 (sys) rad/m^2 and RM = 420,000 +/- 10,000 (stat) +/- 110,000 (sys) rad/m^2 for 1418+546 and 1637+574, respectively; these are the highest values reported to date for AGN. These values indicate magnetic field strengths of the order ~0.0001 G. For 0415+379, 0507+179, and 0954+658 we derive upper limits |RM| &lt; 17,000 rad/m^2. From the relation |RM| ~ \nu^a we find a = 1.9 +/- 0.3 for 1418+546, in good agreement with a = 2 as expected for a spherical or conical outflow.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/the-first-irampdbi-polarimetric-millimeter-survey-of-active-galactic-nuclei-ii-activity-and-properties-of-individual-sources/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Holographic Dark Energy Characterized by the Total Comoving Horizon and Insights to Cosmological Constant and Coincidence Problem [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/20/holographic-dark-energy-characterized-by-the-total-comoving-horizon-and-insights-to-cosmological-constant-and-coincidence-problem-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/20/holographic-dark-energy-characterized-by-the-total-comoving-horizon-and-insights-to-cosmological-constant-and-coincidence-problem-cross-listing/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:56:45 +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[acceleration]]></category>
		<category><![CDATA[best fit]]></category>
		<category><![CDATA[coincidence]]></category>
		<category><![CDATA[consequence]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[cosmological constant]]></category>
		<category><![CDATA[cosmological observations]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[early universe]]></category>
		<category><![CDATA[horizon]]></category>
		<category><![CDATA[inflation]]></category>
		<category><![CDATA[inflationary universe]]></category>
		<category><![CDATA[insight]]></category>
		<category><![CDATA[principle]]></category>
		<category><![CDATA[systematic analysis]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/holographic-dark-energy-characterized-by-the-total-comoving-horizon-and-insights-to-cosmological-constant-and-coincidence-problem-cross-listing/</guid>
		<description><![CDATA[The observed acceleration of the present universe is shown to be well explained by the holographic dark energy characterized by the total comoving horizon of the universe ($\eta$HDE). It is of interest to notice that the very large primordial part of the comoving horizon generated by the inflation of early universe makes the $\eta$HDE behave [...]]]></description>
			<content:encoded><![CDATA[<p>The observed acceleration of the present universe is shown to be well explained by the holographic dark energy characterized by the total comoving horizon of the universe ($\eta$HDE). It is of interest to notice that the very large primordial part of the comoving horizon generated by the inflation of early universe makes the $\eta$HDE behave like a cosmological constant. As a consequence, both the fine-tuning problem and the coincidence problem can reasonably be understood with the inflationary universe and holographical principle. We present a systematic analysis and obtain a consistent cosmological constraint on the $\eta$HDE model based on the recent cosmological observations. It is found that the $\eta$HDE model gives the best-fit result $\Omega_{m0}=0.270$ ($\Omega_{de0}=0.730$) and the minimal $\chi^2_{min}=542.915$ which is compatible with $\chi^2_{\Lambda {\rm CDM}}=542.919$ for the $\Lambda$CDM model.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/holographic-dark-energy-characterized-by-the-total-comoving-horizon-and-insights-to-cosmological-constant-and-coincidence-problem-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>F-GAMMA: On the phenomenological classification of continuum radio spectra variability patterns of Fermi blazars</title>
		<link>http://voxcharta.org/2012/02/20/f-gamma-on-the-phenomenological-classification-of-continuum-radio-spectra-variability-patterns-of-fermi-blazars/</link>
		<comments>http://voxcharta.org/2012/02/20/f-gamma-on-the-phenomenological-classification-of-continuum-radio-spectra-variability-patterns-of-fermi-blazars/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:56:10 +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[active galactic nuclei]]></category>
		<category><![CDATA[band radio]]></category>
		<category><![CDATA[band spectrum]]></category>
		<category><![CDATA[blazar]]></category>
		<category><![CDATA[broad band]]></category>
		<category><![CDATA[component system]]></category>
		<category><![CDATA[continuum]]></category>
		<category><![CDATA[differential]]></category>
		<category><![CDATA[doppler]]></category>
		<category><![CDATA[Fermi]]></category>
		<category><![CDATA[flare]]></category>
		<category><![CDATA[gamma]]></category>
		<category><![CDATA[large scale]]></category>
		<category><![CDATA[mechanisms]]></category>
		<category><![CDATA[phenomenological classification]]></category>
		<category><![CDATA[radio spectra]]></category>
		<category><![CDATA[spectral evolution]]></category>
		<category><![CDATA[telescopes]]></category>
		<category><![CDATA[variability]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/f-gamma-on-the-phenomenological-classification-of-continuum-radio-spectra-variability-patterns-of-fermi-blazars/</guid>
		<description><![CDATA[The F-GAMMA program is a coordinated effort to investigate the physics of Active Galactic Nuclei (AGNs) via multi-frequency monitoring of Fermi blazars. In the current study we show and discuss the evolution of broad-band radio spectra, which are measured at ten frequencies between 2.64 and 142 GHz using the Effelsberg 100-m and the IRAM 30-m [...]]]></description>
			<content:encoded><![CDATA[<p>The F-GAMMA program is a coordinated effort to investigate the physics of Active Galactic Nuclei (AGNs) via multi-frequency monitoring of Fermi blazars. In the current study we show and discuss the evolution of broad-band radio spectra, which are measured at ten frequencies between 2.64 and 142 GHz using the Effelsberg 100-m and the IRAM 30-m telescopes. It is shown that any of the 78 sources studied can be classified in terms of their variability characteristics in merely 5 types of variability. It is argued that these can be attributed to only two classes of variability mechanisms. The first four types are dominated by spectral evolution and can be described by a simple two-component system composed of: (a) a steep quiescent spectral component from a large scale jet and (b) a time evolving flare component following the &#8220;Shock-in-Jet&#8221; evolutionary path. The fifth type is characterised by an achromatic change of the broad band spectrum, which could be attributed to a different mechanism, likely involving differential Doppler boosting caused by geometrical effects. Here we present the classification, the assumed physical scenario and the results of calculations that have been performed for the spectral evolution of flares.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/f-gamma-on-the-phenomenological-classification-of-continuum-radio-spectra-variability-patterns-of-fermi-blazars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The contribution from blazar cascade emission to the extragalactic gamma-ray background: What a role does the extragalactic magnetic field play?</title>
		<link>http://voxcharta.org/2012/02/20/the-contribution-from-blazar-cascade-emission-to-the-extragalactic-gamma-ray-background-what-a-role-does-the-extragalactic-magnetic-field-play/</link>
		<comments>http://voxcharta.org/2012/02/20/the-contribution-from-blazar-cascade-emission-to-the-extragalactic-gamma-ray-background-what-a-role-does-the-extragalactic-magnetic-field-play/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:55:42 +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[blazar]]></category>
		<category><![CDATA[cascade]]></category>
		<category><![CDATA[emission]]></category>
		<category><![CDATA[emission angle]]></category>
		<category><![CDATA[Fermi]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[glf]]></category>
		<category><![CDATA[luminosity function]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[point spread function]]></category>
		<category><![CDATA[saturation]]></category>
		<category><![CDATA[spectrum]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/the-contribution-from-blazar-cascade-emission-to-the-extragalactic-gamma-ray-background-what-a-role-does-the-extragalactic-magnetic-field-play/</guid>
		<description><![CDATA[We estimate the contribution to the extragalactic gamma-ray background (EGRB) from both intrinsic and cascade emissions produced by blazars using a simple semi- analysis method for two models of the blazar gamma-ray luminosity function (GLF). For the cascade emission, we consider two possible contributions: one is due to that the flux of the cascade emission [...]]]></description>
			<content:encoded><![CDATA[<p>We estimate the contribution to the extragalactic gamma-ray background (EGRB) from both intrinsic and cascade emissions produced by blazars using a simple semi- analysis method for two models of the blazar gamma-ray luminosity function (GLF). For the cascade emission, we consider two possible contributions: one is due to that the flux of the cascade emission is lower than the Fermi LAT sensitivity (case I), which is independent on the extragalactic magnetic field (EGMF), another is due to the fact that the flux of the cascade emission is larger than the Fermi LAT sensitivity but the emission angle is larger than LAT point-spread-function (PSF) angle (case II), which depends on the EGMF. Our results indicate that (1) blazar contribution to the EGRB is dominant although it depends on the GLF model and the EGMF; (2) the EGMF plays an important role in estimating the contribution from the cascade emission produced by blazars, the contribution from the cascade emission will significantly alter the EGRB spectrum when the strength of the EGMF is large enough (say BEGMF &gt; 10-12 G); and (3) since the cascade emission in case II reaches a saturation when the strength of the EGMF is ? 10-11 G, it is very possible that the contribution from the cascade emission produced by blazars can be considered as another method to probe the upper limit of the strength of the EGMF.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/the-contribution-from-blazar-cascade-emission-to-the-extragalactic-gamma-ray-background-what-a-role-does-the-extragalactic-magnetic-field-play/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The effect of feedback on the emission properties of the Warm-Hot Intergalactic Medium</title>
		<link>http://voxcharta.org/2012/02/20/the-effect-of-feedback-on-the-emission-properties-of-the-warm-hot-intergalactic-medium/</link>
		<comments>http://voxcharta.org/2012/02/20/the-effect-of-feedback-on-the-emission-properties-of-the-warm-hot-intergalactic-medium/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:53:52 +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[baryon]]></category>
		<category><![CDATA[chemical enrichment]]></category>
		<category><![CDATA[consistent treatment]]></category>
		<category><![CDATA[emission properties]]></category>
		<category><![CDATA[free interaction]]></category>
		<category><![CDATA[galactic wind]]></category>
		<category><![CDATA[galaxy cluster]]></category>
		<category><![CDATA[hydrodynamical simulations]]></category>
		<category><![CDATA[intergalactic medium]]></category>
		<category><![CDATA[light cone]]></category>
		<category><![CDATA[line emission]]></category>
		<category><![CDATA[metal species]]></category>
		<category><![CDATA[observational constraints]]></category>
		<category><![CDATA[physical mechanism]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[ray energies]]></category>
		<category><![CDATA[scale structure]]></category>
		<category><![CDATA[soft x]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[theoretical prediction]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/the-effect-of-feedback-on-the-emission-properties-of-the-warm-hot-intergalactic-medium/</guid>
		<description><![CDATA[At present, 30-40 per cent of the baryons in the local Universe is still undetected. According to theoretical predictions, this gas should reside in filaments filling the large-scale structure (LSS) in the form of a Warm-Hot Intergalactic Medium (WHIM), at temperatures of 10^5 &#8211; 10^7 K, thus emitting in the soft X-ray energies via free-free [...]]]></description>
			<content:encoded><![CDATA[<p>At present, 30-40 per cent of the baryons in the local Universe is still undetected. According to theoretical predictions, this gas should reside in filaments filling the large-scale structure (LSS) in the form of a Warm-Hot Intergalactic Medium (WHIM), at temperatures of 10^5 &#8211; 10^7 K, thus emitting in the soft X-ray energies via free-free interaction and line emission from heavy elements. In this work we characterize the properties of the X-ray emission of the WHIM, and the LSS in general, focusing on the influence of different physical mechanisms, namely galactic winds (GWs), black-hole feedback and star-formation, and providing estimates of possible observational constraints. To this purpose we use a set of cosmological hydrodynamical simulations that include a self-consistent treatment of star-formation and chemical enrichment of the intergalactic medium, that allows us to follow the evolution of different metal species. We construct a set of simulated light-cones to make predictions of the emission in the 0.3-10 keV energy range. We obtain that GWs increase by a factor of 2 the emission of both galaxy clusters and WHIM. The amount of oxygen at average temperature and, consequently, the amount of expected bright Ovii and Oviii lines is increased by a factor of 3 due to GWs and by 20 per cent when assuming a top-heavy IMF. We compare our results with current observational constraints and find that the emission from faint groups and WHIM should account from half to all of the unresolved X-ray background in the 1-2 keV band.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/the-effect-of-feedback-on-the-emission-properties-of-the-warm-hot-intergalactic-medium/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A Density Independent Formulation of Smoothed Particle Hydrodynamics</title>
		<link>http://voxcharta.org/2012/02/20/a-density-independent-formulation-of-smoothed-particle-hydrodynamics/</link>
		<comments>http://voxcharta.org/2012/02/20/a-density-independent-formulation-of-smoothed-particle-hydrodynamics/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:52:57 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astronomical object]]></category>
		<category><![CDATA[blob]]></category>
		<category><![CDATA[density distribution]]></category>
		<category><![CDATA[differentiability]]></category>
		<category><![CDATA[discontinuity]]></category>
		<category><![CDATA[energy conservation]]></category>
		<category><![CDATA[helmholtz]]></category>
		<category><![CDATA[high density]]></category>
		<category><![CDATA[kelvin]]></category>
		<category><![CDATA[low density]]></category>
		<category><![CDATA[numerical diffusion]]></category>
		<category><![CDATA[numerical problem]]></category>
		<category><![CDATA[particle hydrodynamics]]></category>
		<category><![CDATA[rayleigh]]></category>
		<category><![CDATA[repulsive force]]></category>
		<category><![CDATA[shock tube]]></category>
		<category><![CDATA[spatial derivatives]]></category>
		<category><![CDATA[sph]]></category>
		<category><![CDATA[surface tension]]></category>
		<category><![CDATA[symmetry]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/a-density-independent-formulation-of-smoothed-particle-hydrodynamics/</guid>
		<description><![CDATA[In the standard formulation of the smoothed particle hydrodynamics (SPH), it is assumed that the local density distribution is differentiable. This assumption is used to derive the spatial derivatives of other quantities. However, this assumption breaks down at the contact discontinuity, which appears often in simulations of astronomical objects. At the contact discontinuity, the density [...]]]></description>
			<content:encoded><![CDATA[<p>In the standard formulation of the smoothed particle hydrodynamics (SPH), it is assumed that the local density distribution is differentiable. This assumption is used to derive the spatial derivatives of other quantities. However, this assumption breaks down at the contact discontinuity, which appears often in simulations of astronomical objects. At the contact discontinuity, the density of the low-density side is overestimated while that of the high-density side is underestimated. As a result, the pressure of the low (high) density side is over (under) estimated. Thus, unphysical repulsive force appears at the contact discontinuity, resulting in the effective surface tension. This effective surface tension suppresses instabilities such as the Kelvin-Helmholtz and Rayleigh-Taylor instabilities. In this paper, we present a new formulation of SPH, which does not require the differentiability of density and thus can handle contact discontinuity without numerical problems. The results of standard tests such as the shock tube, Kelvin-Helmholtz and Rayleigh-Taylor instabilities, and the blob tests are all very favorable to our new formulation. We conclude that our new formulation solved practically all known difficulties of the standard SPH, without introducing additional numerical diffusion or breaking the exact force symmetry or energy conservation.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/a-density-independent-formulation-of-smoothed-particle-hydrodynamics/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Time dependent embedding of spherically symmetric Rindler spacetime [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/20/time-dependent-embedding-of-spherically-symmetric-rindler-spacetime-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/20/time-dependent-embedding-of-spherically-symmetric-rindler-spacetime-cross-listing/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:51:58 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[congruence]]></category>
		<category><![CDATA[energy density]]></category>
		<category><![CDATA[geometry]]></category>
		<category><![CDATA[heat flux]]></category>
		<category><![CDATA[observers]]></category>
		<category><![CDATA[rindler]]></category>
		<category><![CDATA[sharp energy]]></category>
		<category><![CDATA[strong energy]]></category>
		<category><![CDATA[universe]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/time-dependent-embedding-of-spherically-symmetric-rindler-spacetime-cross-listing/</guid>
		<description><![CDATA[An anisotropic cosmic fluid with radial heat flux which sources a time dependent Rindler geometry is investigated. Even though its energy density $\rho$ is positive, the radial and transversal pressures are negative and the strong energy condition is not satisfied. The congruence of &#8220;static&#8221; observers is not geodesic and the heat flux is oriented outward. [...]]]></description>
			<content:encoded><![CDATA[<p>An anisotropic cosmic fluid with radial heat flux which sources a time dependent Rindler geometry is investigated. Even though its energy density $\rho$ is positive, the radial and transversal pressures are negative and the strong energy condition is not satisfied. The congruence of &#8220;static&#8221; observers is not geodesic and the heat flux is oriented outward. We computed the Misner-Sharp energy associated to the curved Rindler metric embedded in a spatially flat FLRW universe and found that the Weyl energy is vanishing thanks to the conformally flat form of the spacetime.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/time-dependent-embedding-of-spherically-symmetric-rindler-spacetime-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Equation of State for Dark Energy in Modified Gravity Theories [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/20/equation-of-state-for-dark-energy-in-modified-gravity-theories-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/20/equation-of-state-for-dark-energy-in-modified-gravity-theories-cross-listing/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:51:48 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[crossings]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[eos]]></category>
		<category><![CDATA[equation of state]]></category>
		<category><![CDATA[expansion of the universe]]></category>
		<category><![CDATA[finite time]]></category>
		<category><![CDATA[gravitational theory]]></category>
		<category><![CDATA[gravity model]]></category>
		<category><![CDATA[gravity theory]]></category>
		<category><![CDATA[time future]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/equation-of-state-for-dark-energy-in-modified-gravity-theories-cross-listing/</guid>
		<description><![CDATA[We explore the equation of state (EoS) for dark energy $w_{\mathrm{DE}}$ in modified gravitational theories to explain the current accelerated expansion of the universe. We explicitly demonstrate that the future crossings of the phantom divide line of $w_{\mathrm{DE}}=-1$ are the generic feature in the existing viable $f(R)$ gravity models. Furthermore, we show that the crossing [...]]]></description>
			<content:encoded><![CDATA[<p>We explore the equation of state (EoS) for dark energy $w_{\mathrm{DE}}$ in modified gravitational theories to explain the current accelerated expansion of the universe. We explicitly demonstrate that the future crossings of the phantom divide line of $w_{\mathrm{DE}}=-1$ are the generic feature in the existing viable $f(R)$ gravity models. Furthermore, we show that the crossing of the phantom divide can be realized in the combined $f(T)$ theory constructed with the exponential and logarithmic terms. In addition, we investigate the effective EoS for the universe when the finite-time future singularities occur in non-local gravity.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/equation-of-state-for-dark-energy-in-modified-gravity-theories-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A Study of Optical Observing Techniques for Extra-Galactic Supernova Remnants: Case of NGC 300</title>
		<link>http://voxcharta.org/2012/02/20/a-study-of-optical-observing-techniques-for-extra-galactic-supernova-remnants-case-of-ngc-300/</link>
		<comments>http://voxcharta.org/2012/02/20/a-study-of-optical-observing-techniques-for-extra-galactic-supernova-remnants-case-of-ngc-300/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:51:33 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[archival data]]></category>
		<category><![CDATA[criterion]]></category>
		<category><![CDATA[galactic snrs]]></category>
		<category><![CDATA[galactic supernova remnants]]></category>
		<category><![CDATA[galaxy ngc]]></category>
		<category><![CDATA[high resolution image]]></category>
		<category><![CDATA[hubble space telescope]]></category>
		<category><![CDATA[ngc 300]]></category>
		<category><![CDATA[reliability]]></category>
		<category><![CDATA[sculptor group]]></category>
		<category><![CDATA[sii]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectral technique]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[survey]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/a-study-of-optical-observing-techniques-for-extra-galactic-supernova-remnants-case-of-ngc-300/</guid>
		<description><![CDATA[We present the results of a study of observational and identification techniques used for surveys and spectroscopy of candidate supernova remnants (SNRs) in the Sculptor Group galaxy NGC 300. The goal of this study was to investigate the reliability of using [Sii]/Halpha &#62; 0.4 in optical SNR surveys and spectra as an identifying feature of [...]]]></description>
			<content:encoded><![CDATA[<p>We present the results of a study of observational and identification techniques used for surveys and spectroscopy of candidate supernova remnants (SNRs) in the Sculptor Group galaxy NGC 300. The goal of this study was to investigate the reliability of using [Sii]/Halpha &gt; 0.4 in optical SNR surveys and spectra as an identifying feature of extra-galactic SNRs (egSNRs) and also to investigate the effectiveness of the observing techniques (which are hampered by seeing conditions and telescope pointing errors) using this criterion in egSNR surveys and spectrographs. This study is based on original observations of these objects and archival data obtained from the Hubble Space Telescope which contained images of some of the candidate SNRs in NGC 300. We found that the reliability of spectral techniques may be questionable and very high-resolution images may be needed to confirm a valid identification of some egSNRs.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/a-study-of-optical-observing-techniques-for-extra-galactic-supernova-remnants-case-of-ngc-300/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Ultra deep sub-kpc view of nearby massive compact galaxies</title>
		<link>http://voxcharta.org/2012/02/20/ultra-deep-sub-kpc-view-of-nearby-massive-compact-galaxies/</link>
		<comments>http://voxcharta.org/2012/02/20/ultra-deep-sub-kpc-view-of-nearby-massive-compact-galaxies/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:51:15 +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[adaptive optics]]></category>
		<category><![CDATA[compact galaxies]]></category>
		<category><![CDATA[gemini north telescope]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[k band]]></category>
		<category><![CDATA[Sun]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/ultra-deep-sub-kpc-view-of-nearby-massive-compact-galaxies/</guid>
		<description><![CDATA[Using Gemini North telescope ultra deep and high resolution (sub-kpc) K-band adaptive optics imaging of a sample of 4 nearby (z~0.15) massive (~10^{11}M_{sun}) compact (R&#60;1.5 kpc) galaxies, we have explored the structural properties of these rare objects with an unprecedented detail. Our surface brightness profiles expand over 12 magnitudes in range, allowing us to explore [...]]]></description>
			<content:encoded><![CDATA[<p>Using Gemini North telescope ultra deep and high resolution (sub-kpc) K-band adaptive optics imaging of a sample of 4 nearby (z~0.15) massive (~10^{11}M_{sun}) compact (R&lt;1.5 kpc) galaxies, we have explored the structural properties of these rare objects with an unprecedented detail. Our surface brightness profiles expand over 12 magnitudes in range, allowing us to explore the presence of any faint extended envelope on these objects down to stellar mass densities ~10^{6} M_{sun}/kpc^{2} at radial distances of ~15 kpc. We find no evidence for any extended faint tail altering the compactness of these galaxies. Our objects are elongated, resembling visually S0 galaxies and have a central stellar mass density well above the stellar mass densities of objects with similar stellar mass but normal size in the present universe. If these massive compact objects will eventually transform into normal size galaxies, the processes driving this size growth will have to migrate around 2-3&#215;10^{10}M_{sun} stellar mass from their inner (R&lt;1.7 kpc) region towards their outskirts. Nearby massive compact galaxies share with high-z compact massive galaxies not only their stellar mass, size and velocity dispersion but also the shape of their profiles and age of their stellar populations. This makes these singular galaxies unique laboratories to explore the early stages of the formation of massive galaxies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/ultra-deep-sub-kpc-view-of-nearby-massive-compact-galaxies/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Statistical anisotropy of CMB as a probe of conformal rolling scenario</title>
		<link>http://voxcharta.org/2012/02/20/statistical-anisotropy-of-cmb-as-a-probe-of-conformal-rolling-scenario/</link>
		<comments>http://voxcharta.org/2012/02/20/statistical-anisotropy-of-cmb-as-a-probe-of-conformal-rolling-scenario/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:48:18 +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[anisotropy]]></category>
		<category><![CDATA[cmb data]]></category>
		<category><![CDATA[confidence level]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[early universe]]></category>
		<category><![CDATA[hanson]]></category>
		<category><![CDATA[intermediate stage]]></category>
		<category><![CDATA[maximum likelihood method]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[perturbation]]></category>
		<category><![CDATA[power spectra]]></category>
		<category><![CDATA[quadrupole]]></category>
		<category><![CDATA[scenarios]]></category>
		<category><![CDATA[signature]]></category>
		<category><![CDATA[systematic effects]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/statistical-anisotropy-of-cmb-as-a-probe-of-conformal-rolling-scenario/</guid>
		<description><![CDATA[Search for the statistical anisotropy in the CMB data is a powerful tool for constraining models of the early Universe. In this paper we focus on the recently proposed cosmological scenario with conformal rolling. We consider two sub-scenarios, one of which involves a long intermediate stage between conformal rolling and conventional hot epoch. Primordial scalar [...]]]></description>
			<content:encoded><![CDATA[<p>Search for the statistical anisotropy in the CMB data is a powerful tool for constraining models of the early Universe. In this paper we focus on the recently proposed cosmological scenario with conformal rolling. We consider two sub-scenarios, one of which involves a long intermediate stage between conformal rolling and conventional hot epoch. Primordial scalar perturbations generated within these sub-scenarios have different direction-dependent power spectra, both characterized by a single parameter h^2. We search for the signatures of this anisotropy in the seven-year WMAP data using quadratic maximum likelihood method, first applied for similar purposes by Hanson and Lewis. We confirm the large quadrupole anisotropy detected in V and W bands, which has been argued to originate from systematic effects rather than from cosmology. We construct an estimator for the parameter h^2. In the case of the sub-scenario with the intermediate stage we set an upper limit h^2 &lt; 0.045 at the 95% confidence level. The constraint on h^2 is much weaker in the case of another sub-scenario, where the intermediate stage is absent.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/statistical-anisotropy-of-cmb-as-a-probe-of-conformal-rolling-scenario/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Defending The Fallacy of Fine-Tuning [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/20/defending-the-fallacy-of-fine-tuning-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/20/defending-the-fallacy-of-fine-tuning-cross-listing/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:48:06 +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[barnes]]></category>
		<category><![CDATA[conclusion]]></category>
		<category><![CDATA[cosmologist]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[disagreement]]></category>
		<category><![CDATA[earth]]></category>
		<category><![CDATA[fallacy]]></category>
		<category><![CDATA[fellow]]></category>
		<category><![CDATA[life in the universe]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[parameter range]]></category>
		<category><![CDATA[physicist]]></category>
		<category><![CDATA[physics]]></category>
		<category><![CDATA[religious literature]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/defending-the-fallacy-of-fine-tuning-cross-listing/</guid>
		<description><![CDATA[In 2011, I published a popular-level book, The Fallacy of Fine-Tuning: Why the Universe is Not Designed for Us. It investigated a common claim found in contemporary religious literature that the parameters of physics and cosmology are so delicately balanced, so &#8220;fine-tuned,&#8221; that any slight change and life in the universe would have been impossible. [...]]]></description>
			<content:encoded><![CDATA[<p>In 2011, I published a popular-level book, The Fallacy of Fine-Tuning: Why the Universe is Not Designed for Us. It investigated a common claim found in contemporary religious literature that the parameters of physics and cosmology are so delicately balanced, so &#8220;fine-tuned,&#8221; that any slight change and life in the universe would have been impossible. I concluded that while the precise form of life we find on Earth would not exist with slight changes in these parameters, some form of life could have evolved over a parameter range that is not infinitesimal, as often claimed. Postdoctoral fellow Luke Barnes has written a lengthy, highly technical review [arXiv:1112.4647] of the scientific literature on the fine-tuning problem. I have no significant disagreement with that literature and no prominent physicist or cosmologist has disputed my basic conclusions. Barnes does not invalidate these conclusions and misunderstands and misrepresents much of what is in the book.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/defending-the-fallacy-of-fine-tuning-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Probing dark energy beyond $z=2$ with CODEX</title>
		<link>http://voxcharta.org/2012/02/20/probing-dark-energy-beyond-z2-with-codex/</link>
		<comments>http://voxcharta.org/2012/02/20/probing-dark-energy-beyond-z2-with-codex/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:47:21 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[case study]]></category>
		<category><![CDATA[coupling]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[drift]]></category>
		<category><![CDATA[energy model]]></category>
		<category><![CDATA[equation of state]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[Measurement]]></category>
		<category><![CDATA[paradigm]]></category>
		<category><![CDATA[precision measurement]]></category>
		<category><![CDATA[spectrograph]]></category>
		<category><![CDATA[target]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/probing-dark-energy-beyond-z2-with-codex/</guid>
		<description><![CDATA[Precision measurements of nature&#8217;s fundamental couplings and a first measurement of the cosmological redshift drift are two of the key targets for future high-resolution ultra-stable spectrographs such as CODEX. Being able to do both gives CODEX a unique advantage, allowing it to probe dynamical dark energy models (by measuring the behavior of their equation of [...]]]></description>
			<content:encoded><![CDATA[<p>Precision measurements of nature&#8217;s fundamental couplings and a first measurement of the cosmological redshift drift are two of the key targets for future high-resolution ultra-stable spectrographs such as CODEX. Being able to do both gives CODEX a unique advantage, allowing it to probe dynamical dark energy models (by measuring the behavior of their equation of state) deep in the matter era and thereby testing classes of models that would otherwise be difficult to distinguish from the standard $\Lambda$CDM paradigm. We illustrate this point with two simple case studies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/probing-dark-energy-beyond-z2-with-codex/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</title>
		<link>http://voxcharta.org/2012/02/20/future-constraints-on-variations-of-the-fine-structure-constant-from-combined-cmb-and-weak-lensing-measurements/</link>
		<comments>http://voxcharta.org/2012/02/20/future-constraints-on-variations-of-the-fine-structure-constant-from-combined-cmb-and-weak-lensing-measurements/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:46:34 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[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/2012/02/20/future-constraints-on-variations-of-the-fine-structure-constant-from-combined-cmb-and-weak-lensing-measurements/</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/2012/02/20/future-constraints-on-variations-of-the-fine-structure-constant-from-combined-cmb-and-weak-lensing-measurements/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>An Anomaly in the Angular Distribution of Quasar Magnitudes: Evidence for a Bubble Universe with a Mass ~10^21 M\odot</title>
		<link>http://voxcharta.org/2012/02/20/an-anomaly-in-the-angular-distribution-of-quasar-magnitudes-evidence-for-a-bubble-universe-with-a-mass-1021-modot/</link>
		<comments>http://voxcharta.org/2012/02/20/an-anomaly-in-the-angular-distribution-of-quasar-magnitudes-evidence-for-a-bubble-universe-with-a-mass-1021-modot/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:43:36 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[alpha delta]]></category>
		<category><![CDATA[angular distribution]]></category>
		<category><![CDATA[anomaly]]></category>
		<category><![CDATA[bulls eye]]></category>
		<category><![CDATA[CMB]]></category>
		<category><![CDATA[discrepancy]]></category>
		<category><![CDATA[doppler shift]]></category>
		<category><![CDATA[enhancement]]></category>
		<category><![CDATA[eye pattern]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gravitational lensing]]></category>
		<category><![CDATA[intensity]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[mpc]]></category>
		<category><![CDATA[peculiar velocity]]></category>
		<category><![CDATA[sloan survey]]></category>
		<category><![CDATA[systematic error]]></category>
		<category><![CDATA[view of the universe]]></category>
		<category><![CDATA[wavelength]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/an-anomaly-in-the-angular-distribution-of-quasar-magnitudes-evidence-for-a-bubble-universe-with-a-mass-1021-modot/</guid>
		<description><![CDATA[Quasars provide our farthest-reaching view of the Universe. The Sloan Survey now contains over 100,000 quasar candidates. A careful look at the angular distribution of quasar magnitudes shows a surprising intensity enhancement with a &#8220;bulls eye&#8221; pattern toward (alpha,delta) ~ (195{\deg}, 0{\deg}) for all wavelengths from UV through infrared. The angular pattern and size of [...]]]></description>
			<content:encoded><![CDATA[<p>Quasars provide our farthest-reaching view of the Universe. The Sloan Survey now contains over 100,000 quasar candidates. A careful look at the angular distribution of quasar magnitudes shows a surprising intensity enhancement with a &#8220;bulls eye&#8221; pattern toward (alpha,delta) ~ (195{\deg}, 0{\deg}) for all wavelengths from UV through infrared. The angular pattern and size of the enhancement is very similar for all wavelengths, which is inconsistent with a Doppler shift due to a large peculiar velocity toward that direction. The shift is also too large to explain as a systematic error in the quasar magnitudes. The general features of the anomaly can be explained by the gravitational lensing of a massive bubble with Mlens ~ 10^21 M\odot, a lens radius ~350 Mpc, and with the lens subtending an angle of \pm15{\deg} on the sky. It is remarkable that the presence of such a massive bubble universe can explain not only the anomalies in the angular distribution of quasar intensities, but also anomalies in the distribution of luminous red galaxies, anomalies in the CMB, and bulk flow discrepancies, all of which appear in roughly the same direction.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/an-anomaly-in-the-angular-distribution-of-quasar-magnitudes-evidence-for-a-bubble-universe-with-a-mass-1021-modot/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Faint Extended OH Emission from the Local Interstellar Medium in the Direction l \approx 108\circ, b \approx 5\circ</title>
		<link>http://voxcharta.org/2012/02/20/faint-extended-oh-emission-from-the-local-interstellar-medium-in-the-direction-l-approx-108circ-b-approx-5circ/</link>
		<comments>http://voxcharta.org/2012/02/20/faint-extended-oh-emission-from-the-local-interstellar-medium-in-the-direction-l-approx-108circ-b-approx-5circ/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:43:22 +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[circ]]></category>
		<category><![CDATA[extent]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[line emission]]></category>
		<category><![CDATA[local interstellar medium]]></category>
		<category><![CDATA[oh emission]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/faint-extended-oh-emission-from-the-local-interstellar-medium-in-the-direction-l-approx-108circ-b-approx-5circ/</guid>
		<description><![CDATA[We have mapped faint 1667 OH line emission (TA \approx 20 &#8211; 40 mK in our \approx 30&#8242; beam) along many lines of sight in the Galaxy covering an area of \approx 4\circ \times 4\circ in the general direction of l \approx 108\circ, b \approx 5\circ. The OH emission is widespread, similar in extent to [...]]]></description>
			<content:encoded><![CDATA[<p>We have mapped faint 1667 OH line emission (TA \approx 20 &#8211; 40 mK in our \approx 30&#8242; beam) along many lines of sight in the Galaxy covering an area of \approx 4\circ \times 4\circ in the general direction of l \approx 108\circ, b \approx 5\circ. The OH emission is widespread, similar in extent to the local HI (r &lt;/= 2 kpc) both in space and in velocity. The OH profile amplitudes show a good general correlation with those of HI in spectral channels of \approx 1 km/s; this relation is described by TA(OH) \approx 1.50 \times 10^{-4} TB(HI) for values of TB(HI) &lt;/\approx 60 &#8211; 70 K. Beyond this the HI line appears to &quot;saturate&quot;, and few values are recorded above \approx 90 K. However, the OH brightness continues to rise, by a further factor \approx 3. The OH velocity profiles show multiple features with widths typically 2 &#8211; 3 km/s, but less than 10% of these features are associated with CO(1-0) emission in existing surveys of the area smoothed to comparable resolution.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/faint-extended-oh-emission-from-the-local-interstellar-medium-in-the-direction-l-approx-108circ-b-approx-5circ/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The XMM Cluster Survey: The Stellar Mass Assembly of Fossil Galaxies</title>
		<link>http://voxcharta.org/2012/02/20/the-xmm-cluster-survey-the-stellar-mass-assembly-of-fossil-galaxies/</link>
		<comments>http://voxcharta.org/2012/02/20/the-xmm-cluster-survey-the-stellar-mass-assembly-of-fossil-galaxies/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:42:20 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cluster]]></category>
		<category><![CDATA[cluster galaxy]]></category>
		<category><![CDATA[cluster mass]]></category>
		<category><![CDATA[cluster survey]]></category>
		<category><![CDATA[density region]]></category>
		<category><![CDATA[digital sky survey]]></category>
		<category><![CDATA[fossil]]></category>
		<category><![CDATA[fossil systems]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[galaxy merger]]></category>
		<category><![CDATA[gap]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[sloan digital]]></category>
		<category><![CDATA[star formation history]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[universe]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/the-xmm-cluster-survey-the-stellar-mass-assembly-of-fossil-galaxies/</guid>
		<description><![CDATA[This paper presents both the result of a search for fossil systems within the XMM Cluster Survey and the Sloan Digital Sky Survey and the results of a study of the stellar mass assembly and stellar populations of their fossil galaxies. In total, 17 groups and clusters are identified at z &#60; 0.25 with large [...]]]></description>
			<content:encoded><![CDATA[<p>This paper presents both the result of a search for fossil systems within the XMM Cluster Survey and the Sloan Digital Sky Survey and the results of a study of the stellar mass assembly and stellar populations of their fossil galaxies. In total, 17 groups and clusters are identified at z &lt; 0.25 with large magnitude gaps between the first and fourth brightest galaxies. All the information necessary to classify these systems as fossils is provided. For both groups and clusters, the total and fractional luminosity of the brightest galaxy are positively correlated with the magnitude gap. The brightest galaxies in fossil systems (called fossil galaxies) have stellar populations and star-formation histories which are similar to normal brightest cluster galaxies. However, at fixed group/cluster mass, the stellar masses of the fossil galaxies are larger compared to normal brightest cluster galaxies, a fact that holds true over a wide range of group/cluster masses. Moreover, the fossil galaxies are found to contain a significant fraction of the the total optical luminosity of the group/cluster within 0.5R200, as much as 85%, compared to the non-fossils, which can have as little as 10%. Our results suggest that fossil systems formed early and in the highest density regions of the Universe and that fossil galaxies represent the end products of galaxy mergers in groups and clusters.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/the-xmm-cluster-survey-the-stellar-mass-assembly-of-fossil-galaxies/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The mass function of black holes at 1&lt;z&lt;4.5: comparison of models with observations [Replacement]</title>
		<link>http://voxcharta.org/2012/02/20/the-mass-function-of-black-holes-at-1z4-5-comparison-of-models-with-observations-replacement-2/</link>
		<comments>http://voxcharta.org/2012/02/20/the-mass-function-of-black-holes-at-1z4-5-comparison-of-models-with-observations-replacement-2/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:40:35 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[mass function]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/the-mass-function-of-black-holes-at-1z4-5-comparison-of-models-with-observations-replacement-2/</guid>
		<description><![CDATA[In this paper, we compare the observationally derived black hole mass function (BHMF) of luminous broad-line quasars (BLQSOs) at 1&#60;z&#60;4.5 drawn from the Sloan Digital Sky Survey (SDSS) presented in Kelly et al. (2010), with models of merger driven BH growth in the context of standard hierarchical structure formation models. In the models, we explore [...]]]></description>
			<content:encoded><![CDATA[<p>In this paper, we compare the observationally derived black hole mass function (BHMF) of luminous broad-line quasars (BLQSOs) at 1&lt;z&lt;4.5 drawn from the Sloan Digital Sky Survey (SDSS) presented in Kelly et al. (2010), with models of merger driven BH growth in the context of standard hierarchical structure formation models. In the models, we explore two distinct black hole seeding prescriptions at the highest redshifts: &quot;light seeds&quot; &#8211; remnants of Population III stars and &quot;massive seeds&quot; that form from the direct collapse of pre-galactic disks. The subsequent merger triggered mass build-up of the black hole population is tracked over cosmic time under the assumption of a fixed accretion rate as well as rates drawn from the distribution derived by Merloni &amp; Heinz. Our model snapshots are compared to the SDSS derived BHMFs of BLQSOs. Our key findings are that the duty cycle of SMBHs powering BLQSOs increases with increasing redshift for all models and models with Pop III remnants as black hole seeds are unable to fit the observationally derived BHMFs for BLQSOs, lending strong support for the massive seeding model (abridged).</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/the-mass-function-of-black-holes-at-1z4-5-comparison-of-models-with-observations-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Unification models with reheating via primordial black holes [Replacement]</title>
		<link>http://voxcharta.org/2012/02/20/unification-models-with-reheating-via-primordial-black-holes-replacement/</link>
		<comments>http://voxcharta.org/2012/02/20/unification-models-with-reheating-via-primordial-black-holes-replacement/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:39:41 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[big bang]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[evaporation]]></category>
		<category><![CDATA[inflation]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[necessary condition]]></category>
		<category><![CDATA[nucleosynthesis]]></category>
		<category><![CDATA[scalar field]]></category>
		<category><![CDATA[unification]]></category>
		<category><![CDATA[universe]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/unification-models-with-reheating-via-primordial-black-holes-replacement/</guid>
		<description><![CDATA[We study the possibility of reheating the universe through the evaporation of primordial black holes created at the end of inflation. This is shown to allow for the unification of inflation and dark matter under the dynamics of a single scalar field. We determine the necessary conditions to recover the standard Big Bang by the [...]]]></description>
			<content:encoded><![CDATA[<p>We study the possibility of reheating the universe through the evaporation of primordial black holes created at the end of inflation. This is shown to allow for the unification of inflation and dark matter under the dynamics of a single scalar field. We determine the necessary conditions to recover the standard Big Bang by the time of nucleosynthesis after reheating through black holes.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/unification-models-with-reheating-via-primordial-black-holes-replacement/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/2012/02/20/the-outskirts-of-globular-clusters-as-modified-gravity-probes-replacement/</link>
		<comments>http://voxcharta.org/2012/02/20/the-outskirts-of-globular-clusters-as-modified-gravity-probes-replacement/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:39:23 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[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/2012/02/20/the-outskirts-of-globular-clusters-as-modified-gravity-probes-replacement/</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/2012/02/20/the-outskirts-of-globular-clusters-as-modified-gravity-probes-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The CFHTLS-Strong Lensing Legacy Survey (SL2S): Investigating the group-scale lenses with the SARCS sample [Replacement]</title>
		<link>http://voxcharta.org/2012/02/20/the-cfhtls-strong-lensing-legacy-survey-sl2s-investigating-the-group-scale-lenses-with-the-sarcs-sample-replacement/</link>
		<comments>http://voxcharta.org/2012/02/20/the-cfhtls-strong-lensing-legacy-survey-sl2s-investigating-the-group-scale-lenses-with-the-sarcs-sample-replacement/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:38:57 +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[arc]]></category>
		<category><![CDATA[canada france]]></category>
		<category><![CDATA[central galaxy]]></category>
		<category><![CDATA[component density]]></category>
		<category><![CDATA[concordance]]></category>
		<category><![CDATA[contraction]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[deg]]></category>
		<category><![CDATA[density profile]]></category>
		<category><![CDATA[ellipticity]]></category>
		<category><![CDATA[gravitational arcs]]></category>
		<category><![CDATA[hawaii telescope]]></category>
		<category><![CDATA[image separation]]></category>
		<category><![CDATA[lens candidate]]></category>
		<category><![CDATA[luminosity function]]></category>
		<category><![CDATA[radii]]></category>
		<category><![CDATA[sarcs]]></category>
		<category><![CDATA[scale lenses]]></category>
		<category><![CDATA[serendipitously]]></category>
		<category><![CDATA[theoretical model]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/the-cfhtls-strong-lensing-legacy-survey-sl2s-investigating-the-group-scale-lenses-with-the-sarcs-sample-replacement/</guid>
		<description><![CDATA[We present the Strong Lensing Legacy Survey &#8211; ARCS (SARCS) sample compiled from the final T0006 data release of the Canada-France-Hawaii Telescope Legacy Survey (CFHTLS) covering a total non-overlapping area of 159 sq.deg. We adopt a semi-automatic method to find gravitational arcs in the survey that makes use of an arc-finding algorithm. The candidate list [...]]]></description>
			<content:encoded><![CDATA[<p>We present the Strong Lensing Legacy Survey &#8211; ARCS (SARCS) sample compiled from the final T0006 data release of the Canada-France-Hawaii Telescope Legacy Survey (CFHTLS) covering a total non-overlapping area of 159 sq.deg. We adopt a semi-automatic method to find gravitational arcs in the survey that makes use of an arc-finding algorithm. The candidate list is pruned by visual inspection and ranking to form the SARCS sample. This list also includes some serendipitously discovered lens candidates. The SARCS sample consists of 127 lens candidates which span arc radii~2&#8243;-18&#8243; within the unmasked area of ~ 150 sq. deg. Within the sample, 54 systems are promising lenses amongst which, we find 12 giant arcs and 2 radial arc candidates. From our sample, we detect a systematic alignment of giant arcs with the ellipticity of the baryonic component of the lens in concordance with previous studies. The lens redshift distribution corresponding to both the giant arcs and all arcs, estimated from photometric catalogs, peaks at z~0.6. Owing to the large area and depth of the CFHTLS, we find the largest lens sample probing group-scales for the first time. We compare the observed image separation distribution (ISD) of our arcs with theoretical models. A two-component density profile for the lenses which accounts for both the central galaxy and dark matter component is required by the data to explain the observed ISD. Unfortunately, current levels of uncertainties and degeneracies accommodate models both with and without adiabatic contraction. We also show the effects of changing parameters of the model that predict the ISD and that a larger lens sample might constrain relations such as the concentration-mass relation, mass-luminosity relation and slope of the luminosity function. (abridged)</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/the-cfhtls-strong-lensing-legacy-survey-sl2s-investigating-the-group-scale-lenses-with-the-sarcs-sample-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The First Stars: Mass Growth Under Protostellar Feedback [Replacement]</title>
		<link>http://voxcharta.org/2012/02/20/the-first-stars-mass-growth-under-protostellar-feedback-replacement/</link>
		<comments>http://voxcharta.org/2012/02/20/the-first-stars-mass-growth-under-protostellar-feedback-replacement/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:38:33 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[asymptotic value]]></category>
		<category><![CDATA[chemical signature]]></category>
		<category><![CDATA[cosmological simulations]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[dense gas]]></category>
		<category><![CDATA[disk mass]]></category>
		<category><![CDATA[early universe]]></category>
		<category><![CDATA[free population]]></category>
		<category><![CDATA[high density]]></category>
		<category><![CDATA[main sequence]]></category>
		<category><![CDATA[neutral hydrogen]]></category>
		<category><![CDATA[order of magnitude]]></category>
		<category><![CDATA[photodissociation]]></category>
		<category><![CDATA[protostar]]></category>
		<category><![CDATA[solar mass]]></category>
		<category><![CDATA[sound speed]]></category>
		<category><![CDATA[statistical variation]]></category>
		<category><![CDATA[supernovae]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/the-first-stars-mass-growth-under-protostellar-feedback-replacement/</guid>
		<description><![CDATA[We perform three-dimensional cosmological simulations to examine the growth of metal-free, Population III (Pop III) stars under radiative feedback. We begin our simulation at z=100 and trace the evolution of gas and dark matter until the formation of the first minihalo. We then follow the collapse of the gas within the minihalo up to densities [...]]]></description>
			<content:encoded><![CDATA[<p>We perform three-dimensional cosmological simulations to examine the growth of metal-free, Population III (Pop III) stars under radiative feedback. We begin our simulation at z=100 and trace the evolution of gas and dark matter until the formation of the first minihalo. We then follow the collapse of the gas within the minihalo up to densities of n = 10^12 cm^-3, at which point we replace the high-density particles with a sink particle to represent the growing protostar. We model the effect of Lyman-Werner (LW) radiation emitted by the protostar, and employ a ray-tracing scheme to follow the growth of the surrounding H II region over the next 5000 yr. We find that a disk assembles around the first protostar, and that radiative feedback will not prevent further fragmentation of the disk to form multiple Pop III stars. Ionization of neutral hydrogen and photodissociation of H_2 by LW radiation leads to heating of the dense gas to several thousand Kelvin, and this warm region expands outward at the gas sound speed. Once the extent of this warm region becomes equivalent to the size of the disk, the disk mass declines while the accretion rate onto the protostars is reduced by an order of magnitude. This occurs when the largest sink has grown to ~ 20 M_sol while the second sink has grown to 7 M_sol, and we estimate the main sink will approach an asymptotic value of ~ 30 M_sol by the time it reaches the main sequence. Our simulation thus indicates that the most likely outcome is a massive Pop III binary. However, we simulate only one minihalo, and the statistical variation between minihaloes may be substantial. If Pop III stars were typically unable to grow to more than a few tens of solar masses, this would have important consequences for the occurence of pair-instability supernovae in the early Universe as well as the Pop III chemical signature in the oldest stars observable today.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/the-first-stars-mass-growth-under-protostellar-feedback-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Inhomogeneity-induced variance of cosmological parameters [Replacement]</title>
		<link>http://voxcharta.org/2012/02/20/inhomogeneity-induced-variance-of-cosmological-parameters-replacement/</link>
		<comments>http://voxcharta.org/2012/02/20/inhomogeneity-induced-variance-of-cosmological-parameters-replacement/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:37:17 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[buchert]]></category>
		<category><![CDATA[cold dark matter]]></category>
		<category><![CDATA[consequence]]></category>
		<category><![CDATA[cosmic variance]]></category>
		<category><![CDATA[cosmological parameters]]></category>
		<category><![CDATA[curvature]]></category>
		<category><![CDATA[fluctuation]]></category>
		<category><![CDATA[formalism]]></category>
		<category><![CDATA[geometry]]></category>
		<category><![CDATA[global value]]></category>
		<category><![CDATA[gpc]]></category>
		<category><![CDATA[homogeneity]]></category>
		<category><![CDATA[isotropy]]></category>
		<category><![CDATA[Lambda]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[modern cosmology]]></category>
		<category><![CDATA[mpc]]></category>
		<category><![CDATA[regime]]></category>
		<category><![CDATA[typical survey]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/inhomogeneity-induced-variance-of-cosmological-parameters-replacement/</guid>
		<description><![CDATA[Modern cosmology relies on the assumption of large-scale isotropy and homogeneity of the Universe. However, locally the Universe is inhomogeneous and anisotropic. So, how can local measurements (at the 100 Mpc scale) be used to determine global cosmological parameters (defined at the 10 Gpc scale)? We use Buchert&#8217;s averaging formalism and determine a set of [...]]]></description>
			<content:encoded><![CDATA[<p>Modern cosmology relies on the assumption of large-scale isotropy and homogeneity of the Universe. However, locally the Universe is inhomogeneous and anisotropic. So, how can local measurements (at the 100 Mpc scale) be used to determine global cosmological parameters (defined at the 10 Gpc scale)? We use Buchert&#8217;s averaging formalism and determine a set of locally averaged cosmological parameters in the context of the flat Lambda cold dark matter model. We calculate their ensemble means (i.e. their global values) and variances (i.e. their cosmic variances). We apply our results to typical survey geometries and focus on the study of the effects of local fluctuations of the curvature parameter. By this means we show, that in the linear regime cosmological backreaction and averaging can be reformulated as the issue of cosmic variance. The cosmic variance is found largest for the curvature parameter and discuss some of its consequences. We further propose to use the observed variance of cosmological parameters to measure the growth factor. [abbreviated]</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/inhomogeneity-induced-variance-of-cosmological-parameters-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Magnetic Field Amplification by Small-Scale Dynamo Action: Dependence on Turbulence Models and Reynolds and Prandtl Numbers [Replacement]</title>
		<link>http://voxcharta.org/2012/02/20/magnetic-field-amplification-by-small-scale-dynamo-action-dependence-on-turbulence-models-and-reynolds-and-prandtl-numbers-replacement/</link>
		<comments>http://voxcharta.org/2012/02/20/magnetic-field-amplification-by-small-scale-dynamo-action-dependence-on-turbulence-models-and-reynolds-and-prandtl-numbers-replacement/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:37:03 +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[amplification]]></category>
		<category><![CDATA[burgers]]></category>
		<category><![CDATA[correlation function]]></category>
		<category><![CDATA[dependence]]></category>
		<category><![CDATA[differential]]></category>
		<category><![CDATA[dynamo action]]></category>
		<category><![CDATA[eigenvalue]]></category>
		<category><![CDATA[fluctuation]]></category>
		<category><![CDATA[linear differential equation]]></category>
		<category><![CDATA[magnetic energy]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[prandtl number]]></category>
		<category><![CDATA[reynolds number]]></category>
		<category><![CDATA[time evolution]]></category>
		<category><![CDATA[turbulence model]]></category>
		<category><![CDATA[turbulent kinetic energy]]></category>
		<category><![CDATA[typical velocity]]></category>
		<category><![CDATA[velocity correlation]]></category>
		<category><![CDATA[wkb approximation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/magnetic-field-amplification-by-small-scale-dynamo-action-dependence-on-turbulence-models-and-reynolds-and-prandtl-numbers-replacement/</guid>
		<description><![CDATA[The small-scale dynamo is a process by which turbulent kinetic energy is converted into magnetic energy, and thus is expected to depend crucially on the nature of turbulence. In this work, we present a model for the small-scale dynamo that takes into account the slope of the turbulent velocity spectrum v(l) ~ l^theta, where l [...]]]></description>
			<content:encoded><![CDATA[<p>The small-scale dynamo is a process by which turbulent kinetic energy is converted into magnetic energy, and thus is expected to depend crucially on the nature of turbulence. In this work, we present a model for the small-scale dynamo that takes into account the slope of the turbulent velocity spectrum v(l) ~ l^theta, where l and v(l) are the size of a turbulent fluctuation and the typical velocity on that scale. The time evolution of the fluctuation component of the magnetic field, i.e., the small-scale field, is described by the Kazantsev equation. We solve this linear differential equation for its eigenvalues with the quantum-mechanical WKB-approximation. The validity of this method is estimated as a function of the magnetic Prandtl number Pm. We calculate the minimal magnetic Reynolds number for dynamo action, Rm_crit, using our model of the turbulent velocity correlation function. For Kolmogorov turbulence (theta=1/3), we find that the critical magnetic Reynolds number is approximately 110 and for Burgers turbulence (theta=1/2) approximately 2700. Furthermore, we derive that the growth rate of the small-scale magnetic field for a general type of turbulence is Gamma ~ Re^((1-theta)/(1+theta)) in the limit of infinite magnetic Prandtl numbers. For decreasing magnetic Prandtl number (down to Pm approximately larger than 10), the growth rate of the small-scale dynamo decreases. The details of this drop depend on the WKB-approximation, which becomes invalid for a magnetic Prandtl number of about unity.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/magnetic-field-amplification-by-small-scale-dynamo-action-dependence-on-turbulence-models-and-reynolds-and-prandtl-numbers-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Evidence for extra radiation? Profile likelihood versus Bayesian posterior [Replacement]</title>
		<link>http://voxcharta.org/2012/02/20/evidence-for-extra-radiation-profile-likelihood-versus-bayesian-posterior-replacement/</link>
		<comments>http://voxcharta.org/2012/02/20/evidence-for-extra-radiation-profile-likelihood-versus-bayesian-posterior-replacement/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:36:47 +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[artifact]]></category>
		<category><![CDATA[cmb data]]></category>
		<category><![CDATA[confidence interval]]></category>
		<category><![CDATA[cosmic microwave background]]></category>
		<category><![CDATA[cosmological data]]></category>
		<category><![CDATA[discrepancy]]></category>
		<category><![CDATA[eff]]></category>
		<category><![CDATA[equality]]></category>
		<category><![CDATA[excess radiation]]></category>
		<category><![CDATA[expectation]]></category>
		<category><![CDATA[Hubble]]></category>
		<category><![CDATA[parameter constraints]]></category>
		<category><![CDATA[preference]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[profile likelihood]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[robustness]]></category>
		<category><![CDATA[standard model]]></category>
		<category><![CDATA[uncertainty]]></category>
		<category><![CDATA[volume effect]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/evidence-for-extra-radiation-profile-likelihood-versus-bayesian-posterior-replacement/</guid>
		<description><![CDATA[A number of recent analyses of cosmological data have reported hints for the presence of extra radiation beyond the standard model expectation. In order to test the robustness of these claims under different methods of constructing parameter constraints, we perform a Bayesian posterior-based and a likelihood profile-based analysis of current data. We confirm the presence [...]]]></description>
			<content:encoded><![CDATA[<p>A number of recent analyses of cosmological data have reported hints for the presence of extra radiation beyond the standard model expectation. In order to test the robustness of these claims under different methods of constructing parameter constraints, we perform a Bayesian posterior-based and a likelihood profile-based analysis of current data. We confirm the presence of a slight discrepancy between posterior- and profile-based constraints, with the marginalised posterior preferring higher values of the effective number of neutrino species N_eff. This can be traced back to a volume effect occurring during the marginalisation process, and we demonstrate that the effect is related to the fact that cosmic microwave background (CMB) data constrain N_eff only indirectly via the redshift of matter-radiation equality. Once present CMB data are combined with external information about, e.g., the Hubble parameter, the difference between the methods becomes small compared to the uncertainty of N_eff. We conclude that the preference of precision cosmological data for excess radiation is &#8220;real&#8221; and not an artifact of a specific choice of credible/confidence interval construction.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/evidence-for-extra-radiation-profile-likelihood-versus-bayesian-posterior-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Discovery of a Dissociative Galaxy Cluster Merger with Large Physical Separation [Replacement]</title>
		<link>http://voxcharta.org/2012/02/20/discovery-of-a-dissociative-galaxy-cluster-merger-with-large-physical-separation-replacement/</link>
		<comments>http://voxcharta.org/2012/02/20/discovery-of-a-dissociative-galaxy-cluster-merger-with-large-physical-separation-replacement/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:36:35 +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[Chandra]]></category>
		<category><![CDATA[cluster]]></category>
		<category><![CDATA[cluster gas]]></category>
		<category><![CDATA[cluster mergers]]></category>
		<category><![CDATA[cross section]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[galaxy cluster]]></category>
		<category><![CDATA[galaxy evolution]]></category>
		<category><![CDATA[gyr]]></category>
		<category><![CDATA[hubble space telescope]]></category>
		<category><![CDATA[interaction]]></category>
		<category><![CDATA[keck]]></category>
		<category><![CDATA[lens survey]]></category>
		<category><![CDATA[leverage]]></category>
		<category><![CDATA[merger]]></category>
		<category><![CDATA[physical separation]]></category>
		<category><![CDATA[sigma]]></category>
		<category><![CDATA[similar systems]]></category>
		<category><![CDATA[subaru]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/discovery-of-a-dissociative-galaxy-cluster-merger-with-large-physical-separation-replacement/</guid>
		<description><![CDATA[We present DLSCL J0916.2+2951 (z=0.53), a newly discovered major cluster merger in which the collisional cluster gas has become dissociated from the collisionless galaxies and dark matter. We identified the cluster using optical and weak lensing observations as part of the Deep Lens Survey. Our follow-up observations with Keck, Subaru, Hubble Space Telescope, and Chandra [...]]]></description>
			<content:encoded><![CDATA[<p>We present DLSCL J0916.2+2951 (z=0.53), a newly discovered major cluster merger in which the collisional cluster gas has become dissociated from the collisionless galaxies and dark matter. We identified the cluster using optical and weak lensing observations as part of the Deep Lens Survey. Our follow-up observations with Keck, Subaru, Hubble Space Telescope, and Chandra show that the cluster is a dissociative merger and constrain the dark matter self-interaction cross-section {\sigma}_{DM}m_{DM}^{-1}\leq7 cm^2g^{-1}. The system is observed at least 0.7\pm0.2 Gyr since first pass-through, thus providing a picture of cluster mergers 2-5 times further progressed than similar systems observed to date. This improved temporal leverage has implications for our understanding of merging clusters and their impact on galaxy evolution.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/discovery-of-a-dissociative-galaxy-cluster-merger-with-large-physical-separation-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Method of N-body simulation on the MOdified Gravity [Replacement]</title>
		<link>http://voxcharta.org/2012/02/20/method-of-n-body-simulation-on-the-modified-gravity-replacement-2/</link>
		<comments>http://voxcharta.org/2012/02/20/method-of-n-body-simulation-on-the-modified-gravity-replacement-2/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:36:19 +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[abbreviated name]]></category>
		<category><![CDATA[acceleration]]></category>
		<category><![CDATA[approximate calculation]]></category>
		<category><![CDATA[body simulation]]></category>
		<category><![CDATA[brandao]]></category>
		<category><![CDATA[curve]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[dicke]]></category>
		<category><![CDATA[gravity theory]]></category>
		<category><![CDATA[john moffat]]></category>
		<category><![CDATA[mog]]></category>
		<category><![CDATA[structure formation]]></category>
		<category><![CDATA[universe]]></category>
		<category><![CDATA[vector field]]></category>
		<category><![CDATA[viewpoint]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/method-of-n-body-simulation-on-the-modified-gravity-replacement-2/</guid>
		<description><![CDATA[Scalar Tensor Vector Gravity(STVG) is one of a modified gravity theory developed by John Moffat(2005). MOG is abbreviated name for this theory.This theory is added a massive vector field to Brans-Dicke theory. It can explain a galactic rotary curve and the structure formation without dark matter. Without dark energy,acceleration universe too. However,these are claims by [...]]]></description>
			<content:encoded><![CDATA[<p>Scalar Tensor Vector Gravity(STVG) is one of a modified gravity theory developed by John Moffat(2005). MOG is abbreviated name for this theory.This theory is added a massive vector field to Brans-Dicke theory. It can explain a galactic rotary curve and the structure formation without dark matter. Without dark energy,acceleration universe too. However,these are claims by the developer and collaboraters.This theory was only inspected by simple approximate calculation. Therefore it needs more objective verifications.We will carried out verification from the viewpoint of N-body simulation. Such study is already accomplished by Brandao(2010).However, they did not precisely formulate N-body simulation on MOG. This paper shows formulation of the N-body simulation on MOG more precisely.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/method-of-n-body-simulation-on-the-modified-gravity-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Issues on Generating Primordial Anisotropies at the End of Inflation [Replacement]</title>
		<link>http://voxcharta.org/2012/02/20/issues-on-generating-primordial-anisotropies-at-the-end-of-inflation-replacement-2/</link>
		<comments>http://voxcharta.org/2012/02/20/issues-on-generating-primordial-anisotropies-at-the-end-of-inflation-replacement-2/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:36:06 +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[Delta]]></category>
		<category><![CDATA[fluctuation]]></category>
		<category><![CDATA[formalism]]></category>
		<category><![CDATA[gauge field]]></category>
		<category><![CDATA[inflation]]></category>
		<category><![CDATA[invariant]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[scales]]></category>
		<category><![CDATA[spectator]]></category>
		<category><![CDATA[waterfall]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/issues-on-generating-primordial-anisotropies-at-the-end-of-inflation-replacement-2/</guid>
		<description><![CDATA[We revisit the idea of generating primordial anisotropies at the end of inflation in models of inflation with gauge fields. To be specific we consider the charged hybrid inflation model where the waterfall field is charged under a U(1) gauge field so the surface of end of inflation is controlled both by inflaton and the [...]]]></description>
			<content:encoded><![CDATA[<p>We revisit the idea of generating primordial anisotropies at the end of inflation in models of inflation with gauge fields. To be specific we consider the charged hybrid inflation model where the waterfall field is charged under a U(1) gauge field so the surface of end of inflation is controlled both by inflaton and the gauge fields. Using delta N formalism properly we find that the anisotropies generated at the end of inflation from the gauge field fluctuations are exponentially suppressed on cosmological scales. This is because the gauge field evolves exponentially during inflation while in order to generate appreciable anisotropies at the end of inflation the spectator gauge field has to be frozen and scale invariant. We argue that this is a generic feature, that is, one can not generate observable anisotropies at the end of inflation within an FRW background.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/issues-on-generating-primordial-anisotropies-at-the-end-of-inflation-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Type-Ia supernova rates and the progenitor problem, a review [Replacement]</title>
		<link>http://voxcharta.org/2012/02/20/type-ia-supernova-rates-and-the-progenitor-problem-a-review-replacement/</link>
		<comments>http://voxcharta.org/2012/02/20/type-ia-supernova-rates-and-the-progenitor-problem-a-review-replacement/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:35:53 +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[analogy]]></category>
		<category><![CDATA[astrophysics]]></category>
		<category><![CDATA[burst]]></category>
		<category><![CDATA[delay time]]></category>
		<category><![CDATA[environments]]></category>
		<category><![CDATA[martian]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[rate measurement]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[scientist]]></category>
		<category><![CDATA[sne ia]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[time distribution]]></category>
		<category><![CDATA[type ia]]></category>
		<category><![CDATA[unsolved problem]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/type-ia-supernova-rates-and-the-progenitor-problem-a-review-replacement/</guid>
		<description><![CDATA[The identity of the progenitor systems of type-Ia supernovae (SNe Ia) is a major unsolved problem in astrophysics. SN Ia rates are providing some striking clues. We review the basics of SN rate measurement, preach about some sins of SN rate measurement and analysis, and illustrate one of these sins with an analogy about Martian [...]]]></description>
			<content:encoded><![CDATA[<p>The identity of the progenitor systems of type-Ia supernovae (SNe Ia) is a major unsolved problem in astrophysics. SN Ia rates are providing some striking clues. We review the basics of SN rate measurement, preach about some sins of SN rate measurement and analysis, and illustrate one of these sins with an analogy about Martian scientists. We review the recent progress in measuring SN Ia rates in various environments and redshifts, and their use to reconstruct the SN Ia delay time distribution (DTD) &#8212; the SN rate versus time that would follow a hypothetical brief burst of star formation. A good number of DTD measurements, using a variety of methods, appear to be converging. At delays 1&lt;t&lt;10 Gyr, these measurements show a similar, ~t^-1, power-law shape. The DTD peaks at the shortest delays probed, although there is still some uncertainty regarding its precise shape at t&lt;1 Gyr. At face value, this result supports the idea of a double-degenerate progenitor origin for SNe Ia. Single-degenerate progenitors may still play a role in producing short-delay SNe Ia, or perhaps all SNe Ia, if the red-giant donor channel is more efficient than found by most theoretical models. Apart from the DTD shape, the DTD normalization enjoys fairly good agreement (though perhaps some tension), among the various measurements, with a Hubble-time-integrated DTD value of about 2+/- 1 SNe Ia per 1000 Msun (stellar mass formed with a low-mass-turnover IMF). A recent attempt to characterize the local white dwarf binary population suggests that the white dwarf merger rate can explain the Galactic SN Ia rate, if sub-Chandra mergers lead to SN Ia events. We conclude by pointing to some future directions that should lead to progress in the field, including measurement of the bivariate (delay and stretch) SN Ia response function .</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/type-ia-supernova-rates-and-the-progenitor-problem-a-review-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The 2010 very high energy gamma-ray flare &amp; 10 years of multi-wavelength observations of M 87 [Replacement]</title>
		<link>http://voxcharta.org/2012/02/20/the-2010-very-high-energy-gamma-ray-flare-10-years-of-multi-wavelength-observations-of-m-87-replacement/</link>
		<comments>http://voxcharta.org/2012/02/20/the-2010-very-high-energy-gamma-ray-flare-10-years-of-multi-wavelength-observations-of-m-87-replacement/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:35:31 +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[chandra x ray]]></category>
		<category><![CDATA[core region]]></category>
		<category><![CDATA[decay time]]></category>
		<category><![CDATA[evn]]></category>
		<category><![CDATA[exponential function]]></category>
		<category><![CDATA[gamma ray emission]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[giant radio]]></category>
		<category><![CDATA[innermost core]]></category>
		<category><![CDATA[light curve]]></category>
		<category><![CDATA[massive black hole]]></category>
		<category><![CDATA[radio flux]]></category>
		<category><![CDATA[radio galaxy]]></category>
		<category><![CDATA[radio observation]]></category>
		<category><![CDATA[ray observations]]></category>
		<category><![CDATA[relativistic outflows]]></category>
		<category><![CDATA[temporal characterization]]></category>
		<category><![CDATA[wavelength light]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/the-2010-very-high-energy-gamma-ray-flare-10-years-of-multi-wavelength-observations-of-m-87-replacement/</guid>
		<description><![CDATA[Abridged: The giant radio galaxy M 87 with its proximity, famous jet, and very massive black hole provides a unique opportunity to investigate the origin of very high energy (VHE; E&#62;100 GeV) gamma-ray emission generated in relativistic outflows and the surroundings of super-massive black holes. M 87 has been established as a VHE gamma-ray emitter [...]]]></description>
			<content:encoded><![CDATA[<p>Abridged: The giant radio galaxy M 87 with its proximity, famous jet, and very massive black hole provides a unique opportunity to investigate the origin of very high energy (VHE; E&gt;100 GeV) gamma-ray emission generated in relativistic outflows and the surroundings of super-massive black holes. M 87 has been established as a VHE gamma-ray emitter since 2006. The VHE gamma-ray emission displays strong variability on timescales as short as a day. In this paper, results from a joint VHE monitoring campaign on M 87 by the MAGIC and VERITAS instruments in 2010 are reported. During the campaign, a flare at VHE was detected triggering further observations at VHE (H.E.S.S.), X-rays (Chandra), and radio (43 GHz VLBA). The excellent sampling of the VHE gamma-ray light curve enables one to derive a precise temporal characterization of the flare: the single, isolated flare is well described by a two-sided exponential function with significantly different flux rise and decay times. While the overall variability pattern of the 2010 flare appears somewhat different from that of previous VHE flares in 2005 and 2008, they share very similar timescales (~day), peak fluxes (Phi(&gt;0.35 TeV) ~= (1-3) x 10^-11 ph cm^-2 s^-1), and VHE spectra. 43 GHz VLBA radio observations of the inner jet regions indicate no enhanced flux in 2010 in contrast to observations in 2008, where an increase of the radio flux of the innermost core regions coincided with a VHE flare. On the other hand, Chandra X-ray observations taken ~3 days after the peak of the VHE gamma-ray emission reveal an enhanced flux from the core. The long-term (2001-2010) multi-wavelength light curve of M 87, spanning from radio to VHE and including data from HST, LT, VLA and EVN, is used to further investigate the origin of the VHE gamma-ray emission. No unique, common MWL signature of the three VHE flares has been identified.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/the-2010-very-high-energy-gamma-ray-flare-10-years-of-multi-wavelength-observations-of-m-87-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Measuring the neutrino mass from future wide galaxy cluster catalogues [Replacement]</title>
		<link>http://voxcharta.org/2012/02/20/measuring-the-neutrino-mass-from-future-wide-galaxy-cluster-catalogues-replacement/</link>
		<comments>http://voxcharta.org/2012/02/20/measuring-the-neutrino-mass-from-future-wide-galaxy-cluster-catalogues-replacement/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:35:03 +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[cluster catalogues]]></category>
		<category><![CDATA[cluster counts]]></category>
		<category><![CDATA[cluster mass]]></category>
		<category><![CDATA[cluster number]]></category>
		<category><![CDATA[correlation function]]></category>
		<category><![CDATA[cosmic microwave background]]></category>
		<category><![CDATA[cosmological parameters]]></category>
		<category><![CDATA[dynamical evolution]]></category>
		<category><![CDATA[flat universe]]></category>
		<category><![CDATA[forest measurements]]></category>
		<category><![CDATA[free parameter]]></category>
		<category><![CDATA[galaxy cluster]]></category>
		<category><![CDATA[mass determination]]></category>
		<category><![CDATA[neutrino mass]]></category>
		<category><![CDATA[neutrino oscillation experiments]]></category>
		<category><![CDATA[nuisance parameter]]></category>
		<category><![CDATA[order of magnitude]]></category>
		<category><![CDATA[power spectrum]]></category>
		<category><![CDATA[redshift space]]></category>
		<category><![CDATA[spectral amplitude]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/measuring-the-neutrino-mass-from-future-wide-galaxy-cluster-catalogues-replacement/</guid>
		<description><![CDATA[We present forecast errors on a wide range of cosmological parameters obtained from a photometric cluster catalogue of a future wide-field Euclid-like survey. We focus in particular on the total neutrino mass as constrained by a combination of the galaxy cluster number counts and correlation function. For the latter we consider only the shape information [...]]]></description>
			<content:encoded><![CDATA[<p>We present forecast errors on a wide range of cosmological parameters obtained from a photometric cluster catalogue of a future wide-field Euclid-like survey. We focus in particular on the total neutrino mass as constrained by a combination of the galaxy cluster number counts and correlation function. For the latter we consider only the shape information and the Baryon Acoustic Oscillations (BAO), while marginalising over the spectral amplitude and the redshift space distortions. In addition to the cosmological parameters of the standard LCDM+nu model we also consider a non-vanishing curvature, and two parameters describing a redshift evolution for the dark energy equation of state. For completeness, we also marginalise over a set of &#8220;nuisance&#8221; parameters, representing the uncertainties on the cluster mass determination. We find that combining cluster counts with power spectrum information greatly improves the constraining power of each probe taken individually, with errors on cosmological parameters being reduced by up to an order of magnitude. In particular, the best improvements are for the parameters defining the dynamical evolution of dark energy, where cluster counts break degeneracies. Moreover, the resulting error on neutrino mass is at the level of \sigma(M_\nu)\sim 0.9 eV, comparable with that derived from present Ly-alpha forest measurements and Cosmic Microwave background (CMB) data in the framework of a non-flat Universe. Further adopting Planck priors and reducing the number of free parameters to a LCDM+nu cosmology allows to place constraints on the total neutrino mass of \sigma(M_\nu) \sim 0.08 eV, close to the lower bound enforced by neutrino oscillation experiments. [abridged]</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/measuring-the-neutrino-mass-from-future-wide-galaxy-cluster-catalogues-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A Q_6 flavor symmetry model for the nuMSM [Replacement]</title>
		<link>http://voxcharta.org/2012/02/20/a-q_6-flavor-symmetry-model-for-the-numsm-replacement/</link>
		<comments>http://voxcharta.org/2012/02/20/a-q_6-flavor-symmetry-model-for-the-numsm-replacement/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:34:49 +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[angle]]></category>
		<category><![CDATA[degeneracy]]></category>
		<category><![CDATA[flavor symmetry]]></category>
		<category><![CDATA[global data]]></category>
		<category><![CDATA[group properties]]></category>
		<category><![CDATA[mass ratio]]></category>
		<category><![CDATA[mass spectrum]]></category>
		<category><![CDATA[matrix]]></category>
		<category><![CDATA[mu tau]]></category>
		<category><![CDATA[standard model]]></category>
		<category><![CDATA[sterile neutrino]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/a-q_6-flavor-symmetry-model-for-the-numsm-replacement/</guid>
		<description><![CDATA[The extension of the Minimal Standard Model by three right-handed sterile neutrinos with masses smaller than the electroweak scale (nuMSM) is discussed in a Q_6 flavor symmetry framework. The lightness of the keV sterile neutrino and the near mass degeneracy of two heavier sterile neutrinos are naturally explained by exploiting group properties of Q_6. A [...]]]></description>
			<content:encoded><![CDATA[<p>The extension of the Minimal Standard Model by three right-handed sterile neutrinos with masses smaller than the electroweak scale (nuMSM) is discussed in a Q_6 flavor symmetry framework. The lightness of the keV sterile neutrino and the near mass degeneracy of two heavier sterile neutrinos are naturally explained by exploiting group properties of Q_6. A normal hierarchical mass spectrum and an approximately mu-tau symmetric mass matrix are predicted for three active neutrinos. Non-zero theta_{13} can be obtained together with a deviation of theta_{23} from the maximality, where both mixing angles are consistent with the latest global data including T2K and MINOS results. Furthermore, the tiny active-sterile mixing is related to the mass ratio between the lightest active and lightest sterile neutrinos.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/a-q_6-flavor-symmetry-model-for-the-numsm-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Virial Sequences for Thick Discs and Haloes: Flattening and Global Anisotropy [Replacement]</title>
		<link>http://voxcharta.org/2012/02/20/virial-sequences-for-thick-discs-and-haloes-flattening-and-global-anisotropy-replacement-2/</link>
		<comments>http://voxcharta.org/2012/02/20/virial-sequences-for-thick-discs-and-haloes-flattening-and-global-anisotropy-replacement-2/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:34:13 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[anisotropy]]></category>
		<category><![CDATA[dark halo]]></category>
		<category><![CDATA[density profile]]></category>
		<category><![CDATA[ellipticity]]></category>
		<category><![CDATA[frenk]]></category>
		<category><![CDATA[matter density]]></category>
		<category><![CDATA[nfw]]></category>
		<category><![CDATA[observational data]]></category>
		<category><![CDATA[outer halo]]></category>
		<category><![CDATA[parsec]]></category>
		<category><![CDATA[physical model]]></category>
		<category><![CDATA[solar mass]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[thick disc]]></category>
		<category><![CDATA[thin disc]]></category>
		<category><![CDATA[tracer density]]></category>
		<category><![CDATA[velocity dispersion]]></category>
		<category><![CDATA[vertical velocity]]></category>
		<category><![CDATA[virial theorem]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/virial-sequences-for-thick-discs-and-haloes-flattening-and-global-anisotropy-replacement-2/</guid>
		<description><![CDATA[The virial theorem prescribes the ratio of the globally-averaged equatorial to vertical velocity dispersion of a tracer population in spherical and flattened dark haloes. This gives sequences of physical models in the plane of global anisotropy and flattening. The tracer may have any density, though there are particularly simple results for power-laws and exponentials. We [...]]]></description>
			<content:encoded><![CDATA[<p>The virial theorem prescribes the ratio of the globally-averaged equatorial to vertical velocity dispersion of a tracer population in spherical and flattened dark haloes. This gives sequences of physical models in the plane of global anisotropy and flattening. The tracer may have any density, though there are particularly simple results for power-laws and exponentials. We prove the flattening theorem: for a spheroidally stratified tracer density with axis ratio q in a dark density potential with axis ratio g, the ratio of globally averaged equatorial to vertical velocity dispersion depends only on q/g. As the stellar halo density and velocity dispersion of the Milky Way are accessible to observations, this provides a new method for measuring the flattening of the dark matter. If the kinematics of the local halo subdwarfs are representative, then the Milky Way&#8217;s dark halo is oblate with a flattening in the potential of g ~ 0.85, corresponding to a flattening in the dark matter density of ~ 0.7. The fractional pressure excess for power-law populations is roughly proportional to both the ellipticity and the fall-off exponent. Given the same pressure excess, if the density profile of one stellar population declines more quickly than that of another, then it must be rounder. This implies that the dual halo structure claimed by Carollo et al. (2007) for the Galaxy, a flatter inner halo and a rounder outer halo, is inconsistent with the virial theorem. For the thick disc, we provide formulae for the virial sequences of double-exponential discs in logarithmic and Navarro-Frenk-White (NFW) haloes. There are good matches to the observational data on the flattening and anisotropy of the thick disc if the thin disc is exponential with a short scalelength ~ 2.6 kpc and normalisation of 56 solar masses per square parsec, together with a logarithmic dark halo.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/virial-sequences-for-thick-discs-and-haloes-flattening-and-global-anisotropy-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Constraints on Neutrino Mass and Light Degrees of Freedom in Extended Cosmological Parameter Spaces [Replacement]</title>
		<link>http://voxcharta.org/2012/02/20/constraints-on-neutrino-mass-and-light-degrees-of-freedom-in-extended-cosmological-parameter-spaces-replacement/</link>
		<comments>http://voxcharta.org/2012/02/20/constraints-on-neutrino-mass-and-light-degrees-of-freedom-in-extended-cosmological-parameter-spaces-replacement/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:33:54 +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[acoustic oscillations]]></category>
		<category><![CDATA[cosmic microwave background]]></category>
		<category><![CDATA[cosmological model]]></category>
		<category><![CDATA[cosmological parameters]]></category>
		<category><![CDATA[critical density]]></category>
		<category><![CDATA[curvature]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[degrees of freedom]]></category>
		<category><![CDATA[energy component]]></category>
		<category><![CDATA[energy density]]></category>
		<category><![CDATA[free parameter]]></category>
		<category><![CDATA[helium abundance]]></category>
		<category><![CDATA[hst]]></category>
		<category><![CDATA[massive neutrinos]]></category>
		<category><![CDATA[neutrino mass]]></category>
		<category><![CDATA[parameter space]]></category>
		<category><![CDATA[primordial helium]]></category>
		<category><![CDATA[spectral index]]></category>
		<category><![CDATA[SPT]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/constraints-on-neutrino-mass-and-light-degrees-of-freedom-in-extended-cosmological-parameter-spaces-replacement/</guid>
		<description><![CDATA[From a combination of probes including the cosmic microwave background (WMAP7+SPT), Hubble constant (HST), baryon acoustic oscillations (SDSS+2dFGRS), and supernova distances (Union2), we have explored the extent to which the constraints on the effective number of neutrinos and sum of neutrino masses are affected by our ignorance of other cosmological parameters, including the curvature of [...]]]></description>
			<content:encoded><![CDATA[<p>From a combination of probes including the cosmic microwave background (WMAP7+SPT), Hubble constant (HST), baryon acoustic oscillations (SDSS+2dFGRS), and supernova distances (Union2), we have explored the extent to which the constraints on the effective number of neutrinos and sum of neutrino masses are affected by our ignorance of other cosmological parameters, including the curvature of the universe, running of the spectral index, primordial helium abundance, evolving late-time dark energy, and early dark energy. In a combined analysis of the effective number of neutrinos and sum of neutrino masses, we find mild (2.2 sigma) preference for additional light degrees of freedom. However, the effective number of neutrinos is consistent with the canonical expectation of 3 massive neutrinos and no extra relativistic species to within 1 sigma when allowing for evolving dark energy and relaxing the strong inflation prior on the curvature and running. The agreement improves with the possibility of an early dark energy component, itself constrained to be less than 5% of the critical density (95% CL) in our expanded parameter space. In extensions of the standard cosmological model, the derived amplitude of linear matter fluctuations sigma_8 is found to closely agree with low-redshift cluster abundance measurements. The sum of neutrino masses is robust to assumptions of the effective number of neutrinos, late-time dark energy, curvature, and running at the level of 1.2 eV (95% CL). The upper bound degrades to 2.0 eV (95% CL) when further including the early dark energy density and primordial helium abundance as additional free parameters. Even in extended cosmological parameter spaces, Planck alone could determine the possible existence of extra relativistic species at 4 sigma confidence and constrain the sum of neutrino masses to 0.2 eV (68% CL).</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/constraints-on-neutrino-mass-and-light-degrees-of-freedom-in-extended-cosmological-parameter-spaces-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>On the Unification of Active Galactic Nuclei [Replacement]</title>
		<link>http://voxcharta.org/2012/02/20/on-the-unification-of-active-galactic-nuclei-replacement/</link>
		<comments>http://voxcharta.org/2012/02/20/on-the-unification-of-active-galactic-nuclei-replacement/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:33:10 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[agns]]></category>
		<category><![CDATA[compton]]></category>
		<category><![CDATA[distribution function]]></category>
		<category><![CDATA[distribution type]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[ir luminosity]]></category>
		<category><![CDATA[meaningful studies]]></category>
		<category><![CDATA[notion]]></category>
		<category><![CDATA[obscuration]]></category>
		<category><![CDATA[statistic]]></category>
		<category><![CDATA[unification]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/on-the-unification-of-active-galactic-nuclei-replacement/</guid>
		<description><![CDATA[The inevitable spread in properties of the toroidal obscuration of active galactic nuclei (AGNs) invalidates the widespread notion that type 1 and 2 AGNs are intrinsically the same objects, drawn randomly from the distribution of torus covering factors. Instead, AGNs are drawn \emph{preferentially} from this distribution; type 2 are more likely drawn from the distribution [...]]]></description>
			<content:encoded><![CDATA[<p>The inevitable spread in properties of the toroidal obscuration of active galactic nuclei (AGNs) invalidates the widespread notion that type 1 and 2 AGNs are intrinsically the same objects, drawn randomly from the distribution of torus covering factors. Instead, AGNs are drawn \emph{preferentially} from this distribution; type 2 are more likely drawn from the distribution higher end, type 1 from its lower end. Type 2 AGNs have a higher IR luminosity, lower narrow-line luminosity and a higher fraction of Compton thick X-ray obscuration than type 1. Meaningful studies of unification statistics cannot be conducted without first determining the intrinsic distribution function of torus covering factors.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/on-the-unification-of-active-galactic-nuclei-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>emcee: The MCMC Hammer [Replacement]</title>
		<link>http://voxcharta.org/2012/02/20/emcee-the-mcmc-hammer-replacement/</link>
		<comments>http://voxcharta.org/2012/02/20/emcee-the-mcmc-hammer-replacement/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:31:44 +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[algorithm]]></category>
		<category><![CDATA[api]]></category>
		<category><![CDATA[astrophysics]]></category>
		<category><![CDATA[cpu core]]></category>
		<category><![CDATA[emcee]]></category>
		<category><![CDATA[gnu general public license]]></category>
		<category><![CDATA[goodman]]></category>
		<category><![CDATA[literature]]></category>
		<category><![CDATA[markov chain monte]]></category>
		<category><![CDATA[markov chain monte carlo]]></category>
		<category><![CDATA[mcmc]]></category>
		<category><![CDATA[open source]]></category>
		<category><![CDATA[parallelism]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[parameter space]]></category>
		<category><![CDATA[python implementation]]></category>
		<category><![CDATA[sampling method]]></category>
		<category><![CDATA[stable]]></category>
		<category><![CDATA[weare]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/emcee-the-mcmc-hammer-replacement/</guid>
		<description><![CDATA[We introduce a stable, well tested Python implementation of the affine-invariant ensemble sampler for Markov chain Monte Carlo (MCMC) proposed by Goodman &#38; Weare (2010). The code is open source and has already been used in several published projects in the astrophysics literature. The algorithm behind emcee has several advantages over traditional MCMC sampling methods [...]]]></description>
			<content:encoded><![CDATA[<p>We introduce a stable, well tested Python implementation of the affine-invariant ensemble sampler for Markov chain Monte Carlo (MCMC) proposed by Goodman &amp; Weare (2010). The code is open source and has already been used in several published projects in the astrophysics literature. The algorithm behind emcee has several advantages over traditional MCMC sampling methods and it has excellent performance as measured by the autocorrelation time (or function calls per independent sample). One major advantage of the algorithm is that it requires hand-tuning of only 1 or 2 parameters compared to $\sim N^2$ for a traditional algorithm in an N-dimensional parameter space. In this document, we describe the algorithm and the details of our implementation and API. Exploiting the parallelism of the ensemble method, emcee permits any user to take advantage of multiple CPU cores without extra effort. The code is available online at <a href="http://danfm.ca/emcee">http://danfm.ca/emcee</a> under the GNU General Public License v2.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/emcee-the-mcmc-hammer-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Anisotropic to Isotropic Phase Transitions in the Early Universe [Replacement]</title>
		<link>http://voxcharta.org/2012/02/20/anisotropic-to-isotropic-phase-transitions-in-the-early-universe-replacement/</link>
		<comments>http://voxcharta.org/2012/02/20/anisotropic-to-isotropic-phase-transitions-in-the-early-universe-replacement/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:31:06 +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[analogy]]></category>
		<category><![CDATA[baryon asymmetry]]></category>
		<category><![CDATA[dirac equation]]></category>
		<category><![CDATA[early universe]]></category>
		<category><![CDATA[entropy]]></category>
		<category><![CDATA[fermion]]></category>
		<category><![CDATA[isotropic phase]]></category>
		<category><![CDATA[lorentz symmetry]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[partition function]]></category>
		<category><![CDATA[phase transition]]></category>
		<category><![CDATA[space time]]></category>
		<category><![CDATA[thermodynamics]]></category>
		<category><![CDATA[transfer matrix]]></category>
		<category><![CDATA[transition]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/anisotropic-to-isotropic-phase-transitions-in-the-early-universe-replacement/</guid>
		<description><![CDATA[We propose that the early Universe was not Lorentz symmetric and that a gradual transition to the Lorentz symmetric phase occurred. An underlying form of the Dirac equation hints to such a transition for fermions. Fermions were coupled to space-time in a non-trivial manner such that they were massless in the Lorentz violating phase. The [...]]]></description>
			<content:encoded><![CDATA[<p>We propose that the early Universe was not Lorentz symmetric and that a gradual transition to the Lorentz symmetric phase occurred. An underlying form of the Dirac equation hints to such a transition for fermions. Fermions were coupled to space-time in a non-trivial manner such that they were massless in the Lorentz violating phase. The partition function is used as a transfer matrix to model this transition on a two level thermodynamics system that describes how such a transition might have occurred. The system that models this transition evolves, with temperature, from a state of large to negligible entropy and this is interpreted as describing the transition to a state with Lorentz symmetry. In addition to this, analogy is created with the properties of this system to describe how the fields were massless and how a baryon asymmetry can be generated in this model.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/anisotropic-to-isotropic-phase-transitions-in-the-early-universe-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A New Class of Four-Dimensional N=1 Supergravity with Non-minimal Derivative Couplings [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/19/a-new-class-of-four-dimensional-n1-supergravity-with-non-minimal-derivative-couplings-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/19/a-new-class-of-four-dimensional-n1-supergravity-with-non-minimal-derivative-couplings-cross-listing/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:54:14 +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[chiral]]></category>
		<category><![CDATA[coupling]]></category>
		<category><![CDATA[curvature]]></category>
		<category><![CDATA[derivative]]></category>
		<category><![CDATA[einstein]]></category>
		<category><![CDATA[interaction]]></category>
		<category><![CDATA[scalar]]></category>
		<category><![CDATA[shell]]></category>
		<category><![CDATA[supergravity]]></category>
		<category><![CDATA[tensor]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/a-new-class-of-four-dimensional-n1-supergravity-with-non-minimal-derivative-couplings-cross-listing/</guid>
		<description><![CDATA[In the N=1 four-dimensional new-minimal supergravity framework, we supersymmetrise the coupling of the scalar kinetic term to the Einstein tensor. This coupling, although introduces a non-minimal derivative interaction of curvature to matter, it does not introduce harmful higher-derivatives. For this construction, we employ off-shell chiral and real linear multiplets. Physical scalars are accommodated in the [...]]]></description>
			<content:encoded><![CDATA[<p>In the N=1 four-dimensional new-minimal supergravity framework, we supersymmetrise the coupling of the scalar kinetic term to the Einstein tensor. This coupling, although introduces a non-minimal derivative interaction of curvature to matter, it does not introduce harmful higher-derivatives. For this construction, we employ off-shell chiral and real linear multiplets. Physical scalars are accommodated in the chiral multiplet whereas curvature resides in a linear one.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/a-new-class-of-four-dimensional-n1-supergravity-with-non-minimal-derivative-couplings-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Is Quasar Variability a Damped Random Walk?</title>
		<link>http://voxcharta.org/2012/02/19/is-quasar-variability-a-damped-random-walk/</link>
		<comments>http://voxcharta.org/2012/02/19/is-quasar-variability-a-damped-random-walk/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:53:55 +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[adequate description]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[covariance function]]></category>
		<category><![CDATA[cutoff time]]></category>
		<category><![CDATA[deviations]]></category>
		<category><![CDATA[existence]]></category>
		<category><![CDATA[kepler]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[long time]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[random walk]]></category>
		<category><![CDATA[short time]]></category>
		<category><![CDATA[time scale]]></category>
		<category><![CDATA[variability]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/is-quasar-variability-a-damped-random-walk/</guid>
		<description><![CDATA[The damped random walk (DRW) model is increasingly used to model the variability in quasar light curves, but it is still uncertain whether the DRW model provides an adequate description of quasar variability across all time scales. Using a sample of OGLE quasar light curves, we consider four modifications to the DRW model by introducing [...]]]></description>
			<content:encoded><![CDATA[<p>The damped random walk (DRW) model is increasingly used to model the variability in quasar light curves, but it is still uncertain whether the DRW model provides an adequate description of quasar variability across all time scales. Using a sample of OGLE quasar light curves, we consider four modifications to the DRW model by introducing additional parameters into the covariance function to search for deviations from the DRW model on both short and long time scales. We find excellent agreement with the DRW model on time scales that are well sampled by the data (from a month to a few years), possibly with some intrinsic scatter in the additional parameters. On very short time scales (below a few months), we see some evidence of the existence of a cutoff time scale below which the correlation is stronger than the DRW model, echoing the recent finding of Mushotzky et al. (2011) using quasar light curves from Kepler. On very long time scales (&gt; a few years), the light curves do not constrain models well, but are generally consistent with the DRW model.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/is-quasar-variability-a-damped-random-walk/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Measuring X-ray variability in faint/sparsely-sampled AGN</title>
		<link>http://voxcharta.org/2012/02/19/measuring-x-ray-variability-in-faintsparsely-sampled-agn/</link>
		<comments>http://voxcharta.org/2012/02/19/measuring-x-ray-variability-in-faintsparsely-sampled-agn/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:50:37 +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[active galactic nuclei]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[biases]]></category>
		<category><![CDATA[cdf]]></category>
		<category><![CDATA[Chandra]]></category>
		<category><![CDATA[future x]]></category>
		<category><![CDATA[lightcurve]]></category>
		<category><![CDATA[maximum likelihood]]></category>
		<category><![CDATA[measurement error]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[monte carlo simulation]]></category>
		<category><![CDATA[population]]></category>
		<category><![CDATA[sampling pattern]]></category>
		<category><![CDATA[statistic]]></category>
		<category><![CDATA[uncertainty]]></category>
		<category><![CDATA[uniform sampling]]></category>
		<category><![CDATA[variability]]></category>
		<category><![CDATA[variance]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xmm newton]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/measuring-x-ray-variability-in-faintsparsely-sampled-agn/</guid>
		<description><![CDATA[We discuss some practical aspects of measuring the variability amplitude of faint and distant active galactic nuclei (AGN), characterized by sparsely sampled lightcurves and low statistic. In such cases the excess variance, commonly used to estimate the intrinsic lightcurve variance, is affected by strong biases and uncertainties since it represents a maximum likelihood variability estimator [...]]]></description>
			<content:encoded><![CDATA[<p>We discuss some practical aspects of measuring the variability amplitude of faint and distant active galactic nuclei (AGN), characterized by sparsely sampled lightcurves and low statistic. In such cases the excess variance, commonly used to estimate the intrinsic lightcurve variance, is affected by strong biases and uncertainties since it represents a maximum likelihood variability estimator only for identical/normal distributed measurements errors and uniform sampling. We performed realistic Monte Carlo simulations of AGN lightcurves, reproducing both the sampling pattern and measurement errors typical of multi-epoch deep surveys, such as the XMM-Newton observations of the Chandra Deep Field South (CDFS), or assuming different sampling patterns that may characterize long surveys with sub-optimal observing conditions. We used the results to estimate our ability to measure the intrinsic source variability as well as to constrain the observing strategy of future X-ray missions studying distant and/or faint AGN populations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/measuring-x-ray-variability-in-faintsparsely-sampled-agn/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The XMM Cluster Survey: The interplay between the brightest cluster galaxy and the intra-cluster medium via AGN feedback</title>
		<link>http://voxcharta.org/2012/02/19/the-xmm-cluster-survey-the-interplay-between-the-brightest-cluster-galaxy-and-the-intra-cluster-medium-via-agn-feedback/</link>
		<comments>http://voxcharta.org/2012/02/19/the-xmm-cluster-survey-the-interplay-between-the-brightest-cluster-galaxy-and-the-intra-cluster-medium-via-agn-feedback/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:50:18 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[cluster]]></category>
		<category><![CDATA[cluster galaxy]]></category>
		<category><![CDATA[cluster group]]></category>
		<category><![CDATA[cluster mass]]></category>
		<category><![CDATA[cluster survey]]></category>
		<category><![CDATA[empirical definition]]></category>
		<category><![CDATA[first data]]></category>
		<category><![CDATA[fuel supply]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[host galaxy]]></category>
		<category><![CDATA[icm]]></category>
		<category><![CDATA[interplay]]></category>
		<category><![CDATA[keV]]></category>
		<category><![CDATA[mass range]]></category>
		<category><![CDATA[unity]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/the-xmm-cluster-survey-the-interplay-between-the-brightest-cluster-galaxy-and-the-intra-cluster-medium-via-agn-feedback/</guid>
		<description><![CDATA[Using a sample of 123 X-ray clusters and groups drawn from the XMM-Cluster Survey first data release, we investigate the interplay between the brightest cluster galaxy (BCG), its black hole, and the intra-cluster/group medium (ICM). It appears that for groups and clusters with a BCG likely to host significant AGN feedback, gas cooling dominates in [...]]]></description>
			<content:encoded><![CDATA[<p>Using a sample of 123 X-ray clusters and groups drawn from the XMM-Cluster Survey first data release, we investigate the interplay between the brightest cluster galaxy (BCG), its black hole, and the intra-cluster/group medium (ICM). It appears that for groups and clusters with a BCG likely to host significant AGN feedback, gas cooling dominates in those with Tx &gt; 2 keV while AGN feedback dominates below. This may be understood through the sub-unity exponent found in the scaling relation we derive between the BCG mass and cluster mass over the halo mass range 10^13 &lt; M500  2 keV) and again co-located with an effective fuel supply of dense, cooling gas. This demonstrates that the most massive black holes appear to know more about their host cluster than they do about their host galaxy. The results lead us to propose a physically motivated, empirical definition of &#8216;cluster&#8217; and &#8216;group&#8217;, delineated at 2 keV.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/the-xmm-cluster-survey-the-interplay-between-the-brightest-cluster-galaxy-and-the-intra-cluster-medium-via-agn-feedback/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Carbon Detection in Early-Time Optical Spectra of Type Ia Supernovae</title>
		<link>http://voxcharta.org/2012/02/19/carbon-detection-in-early-time-optical-spectra-of-type-ia-supernovae/</link>
		<comments>http://voxcharta.org/2012/02/19/carbon-detection-in-early-time-optical-spectra-of-type-ia-supernovae/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:49:59 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorption feature]]></category>
		<category><![CDATA[earliest times]]></category>
		<category><![CDATA[explosion]]></category>
		<category><![CDATA[mechanisms]]></category>
		<category><![CDATA[optical spectra]]></category>
		<category><![CDATA[scenarios]]></category>
		<category><![CDATA[sne ia]]></category>
		<category><![CDATA[type ia supernovae]]></category>
		<category><![CDATA[unburned fuel]]></category>
		<category><![CDATA[white dwarf]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/carbon-detection-in-early-time-optical-spectra-of-type-ia-supernovae/</guid>
		<description><![CDATA[While O is often seen in spectra of Type Ia supernovae (SNe Ia) as both unburned fuel and a product of C burning, C is only occasionally seen at the earliest times, and it represents the most direct way of investigating primordial white dwarf material and its relation to SN Ia explosion scenarios and mechanisms. [...]]]></description>
			<content:encoded><![CDATA[<p>While O is often seen in spectra of Type Ia supernovae (SNe Ia) as both unburned fuel and a product of C burning, C is only occasionally seen at the earliest times, and it represents the most direct way of investigating primordial white dwarf material and its relation to SN Ia explosion scenarios and mechanisms. In this paper, we search for C absorption features in 188 optical spectra of 144 low-redshift (z &lt; 0.1) SNe Ia with ages &lt;3.6 d after maximum brightness. These data were obtained as part of the Berkeley SN Ia Program (BSNIP; Silverman et al. 2012a,b, submitted) and represent the largest spectral dataset in which C has ever been searched. We find that ~11 per cent of the SNe studied show definite C absorption features while ~25 per cent show some evidence for C II in their spectra. Also, if one obtains a spectrum at t &lt; -5 d, then there is a better than 30 per cent chance of detecting a distinct absorption feature from C II. SNe Ia that show C are found to resemble those without C in many respects, but objects with C tend to have bluer optical colours than those without. The typical expansion velocity of the C II 6580 Ang. feature is measured to be 12,000-13,000 km/s, and the ratio of the C II 6580 Ang. to Si II 6355 Ang. velocities is remarkably constant with time and among different objects with a median value of ~1.05. While the pseudo-equivalent widths (pEWs) of the C II 6580 Ang. and C II 7234 Ang. features are found mostly to decrease with time, we see evidence of a significant increase in pEW between ~12 and 11 d before maximum brightness, which is actually predicted by some theoretical models. The range of pEWs measured from the BSNIP data implies a range of C mass in SN Ia ejecta of about (2-30) x 10^{-3} M_Sun.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/carbon-detection-in-early-time-optical-spectra-of-type-ia-supernovae/feed/</wfw:commentRss>
		<slash:comments>1</slash:comments>
		</item>
		<item>
		<title>B2 0954+25A: a typical Fermi blazar or a gamma-loud Narrow Line Seyfert 1</title>
		<link>http://voxcharta.org/2012/02/19/b2-095425a-a-typical-fermi-blazar-or-a-gamma-loud-narrow-line-seyfert-1/</link>
		<comments>http://voxcharta.org/2012/02/19/b2-095425a-a-typical-fermi-blazar-or-a-gamma-loud-narrow-line-seyfert-1/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:49:45 +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[blazar]]></category>
		<category><![CDATA[broad band]]></category>
		<category><![CDATA[composite analysis]]></category>
		<category><![CDATA[estimates]]></category>
		<category><![CDATA[Fermi]]></category>
		<category><![CDATA[flatness]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[line profile]]></category>
		<category><![CDATA[observational properties]]></category>
		<category><![CDATA[pmn]]></category>
		<category><![CDATA[quasar]]></category>
		<category><![CDATA[radio lobes]]></category>
		<category><![CDATA[radio spectrum]]></category>
		<category><![CDATA[satellite]]></category>
		<category><![CDATA[spectral energy distribution]]></category>
		<category><![CDATA[spectrum radio]]></category>
		<category><![CDATA[transition]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/b2-095425a-a-typical-fermi-blazar-or-a-gamma-loud-narrow-line-seyfert-1/</guid>
		<description><![CDATA[B2 0954+25A, detected by the {\it Fermi} satellite, is a blazar with interesting observational properties: it has been observed to transit from a jet dominated to a disk dominated state; its radio spectrum appears flat at all observing frequencies (down to 74 MHz); optically, the H$\beta$ line profile is asymmetric. The flatness of radio spectrum [...]]]></description>
			<content:encoded><![CDATA[<p>B2 0954+25A, detected by the {\it Fermi} satellite, is a blazar with interesting observational properties: it has been observed to transit from a jet dominated to a disk dominated state; its radio spectrum appears flat at all observing frequencies (down to 74 MHz); optically, the H$\beta$ line profile is asymmetric. The flatness of radio spectrum suggests that the isotropic emission from radio lobes is very weak, despite the large size of its jet ($\gtrsim$ 500 kpc). Its broad&#8211;band spectral energy distribution is surprisingly similar to that of the prototypical $\gamma$&#8211;ray, radio loud, Narrow Line Seyfert 1 ($\gamma$&#8211;NLS1) galaxy PMN J0948+0022. In this work we revisit the mass estimates of B2 0954+25A considering only the symmetric component of the H$\beta$ line and find (1&#8211;3) $\times 10^8$ M$_{\sun}$. In light of our composite analysis, we propose to classify the source as a transition object between the class of Flat Spectrum Radio Quasar and $\gamma$&#8211;ray, radio loud NLS1. A comparison with two members of each class (3C 273 and PMN J0948+0022) is discussed.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/b2-095425a-a-typical-fermi-blazar-or-a-gamma-loud-narrow-line-seyfert-1/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>On the average density profile of dark-matter halos in the inner regions of massive early-type galaxies</title>
		<link>http://voxcharta.org/2012/02/19/on-the-average-density-profile-of-dark-matter-halos-in-the-inner-regions-of-massive-early-type-galaxies/</link>
		<comments>http://voxcharta.org/2012/02/19/on-the-average-density-profile-of-dark-matter-halos-in-the-inner-regions-of-massive-early-type-galaxies/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:49:09 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[chabrier]]></category>
		<category><![CDATA[contraction]]></category>
		<category><![CDATA[cosmological simulations]]></category>
		<category><![CDATA[dark matter halo]]></category>
		<category><![CDATA[density profile]]></category>
		<category><![CDATA[einstein]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[inner regions]]></category>
		<category><![CDATA[innermost region]]></category>
		<category><![CDATA[matter density]]></category>
		<category><![CDATA[radius]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[salpeter]]></category>
		<category><![CDATA[slope]]></category>
		<category><![CDATA[stellar imf]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[structure formation]]></category>
		<category><![CDATA[synthesis]]></category>
		<category><![CDATA[type galaxy]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/on-the-average-density-profile-of-dark-matter-halos-in-the-inner-regions-of-massive-early-type-galaxies/</guid>
		<description><![CDATA[We study a sample of 39 massive early-type lens galaxies at redshift z &#60; 0.3 to determine the slope of the average dark-matter density profile in the innermost regions. We keep the strong lensing and stellar population synthesis modeling as simple as possible to measure the galaxy total and luminous masses. By rescaling the values [...]]]></description>
			<content:encoded><![CDATA[<p>We study a sample of 39 massive early-type lens galaxies at redshift z &lt; 0.3 to determine the slope of the average dark-matter density profile in the innermost regions. We keep the strong lensing and stellar population synthesis modeling as simple as possible to measure the galaxy total and luminous masses. By rescaling the values of the Einstein radius and dark-matter projected mass with the values of the luminous effective radius and mass, we combine all the data of the galaxies in the sample. We find that between 0.3 and 0.9 times the value of the effective radius the average logarithmic slope of the dark-matter projected density profile is -1.0 +/- 0.2 (i.e., approximately isothermal) or -0.7 +/- 0.5 (i.e., shallower than isothermal), if, respectively, a constant Chabrier or heavier, Salpeter-like stellar IMF is adopted. These results provide positive evidence of the influence of the baryonic component on the contraction of the galaxy dark-matter halos, compared to the predictions of dark matter-only cosmological simulations, and open a new way to test models of structure formation and evolution within the standard LCDM cosmological scenario.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/on-the-average-density-profile-of-dark-matter-halos-in-the-inner-regions-of-massive-early-type-galaxies/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A Relic Star Cluster in the Sextans Dwarf Spheroidal Galaxy &#8211; Implications for Early Star and Galaxy Formation</title>
		<link>http://voxcharta.org/2012/02/19/a-relic-star-cluster-in-the-sextans-dwarf-spheroidal-galaxy-implications-for-early-star-and-galaxy-formation/</link>
		<comments>http://voxcharta.org/2012/02/19/a-relic-star-cluster-in-the-sextans-dwarf-spheroidal-galaxy-implications-for-early-star-and-galaxy-formation/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:48:36 +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[abundance]]></category>
		<category><![CDATA[dwarf galaxy]]></category>
		<category><![CDATA[environments]]></category>
		<category><![CDATA[existence]]></category>
		<category><![CDATA[four star]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[galaxy formation]]></category>
		<category><![CDATA[galaxy population]]></category>
		<category><![CDATA[imf]]></category>
		<category><![CDATA[init]]></category>
		<category><![CDATA[initial mass function]]></category>
		<category><![CDATA[observational data]]></category>
		<category><![CDATA[relic]]></category>
		<category><![CDATA[salpeter]]></category>
		<category><![CDATA[six stars]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[star cluster]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[tentative evidence]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/a-relic-star-cluster-in-the-sextans-dwarf-spheroidal-galaxy-implications-for-early-star-and-galaxy-formation/</guid>
		<description><![CDATA[We present tentative evidence for the existence of a dissolved star cluster in the Sextans dwarf spheroidal galaxy. In a sample of six stars, we identify three (possibly four) stars around [Fe/H] =-2.7 that are highly clustered in a multi-dimensional chemical abundance space. The estimated initial stellar mass of the cluster is M*,init = 1.9^+1.5_-0.9 [...]]]></description>
			<content:encoded><![CDATA[<p>We present tentative evidence for the existence of a dissolved star cluster in the Sextans dwarf spheroidal galaxy. In a sample of six stars, we identify three (possibly four) stars around [Fe/H] =-2.7 that are highly clustered in a multi-dimensional chemical abundance space. The estimated initial stellar mass of the cluster is M*,init = 1.9^+1.5_-0.9 (1.6^+1.2_-0.8)*10^5 Msol assuming a Salpeter (Kroupa) initial mass function (IMF). If corroborated by follow-up spectroscopy, this ancient star cluster at [Fe/H] =-2.7 is the most metal-poor system identified to date. Inspired by this finding, we also present a new way to interpret the cumulative metallicity functions of dwarf galaxies. From available observational data, we speculate that the ultra-faint dwarf galaxy population, or a significant fraction thereof, and the more luminous, classical dwarf spheroidal population were formed in different environments and would thus be distinct in origin.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/a-relic-star-cluster-in-the-sextans-dwarf-spheroidal-galaxy-implications-for-early-star-and-galaxy-formation/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Four Fundamental Foreground Power Spectrum Shapes for 21 cm Cosmology Observations</title>
		<link>http://voxcharta.org/2012/02/19/four-fundamental-foreground-power-spectrum-shapes-for-21-cm-cosmology-observations/</link>
		<comments>http://voxcharta.org/2012/02/19/four-fundamental-foreground-power-spectrum-shapes-for-21-cm-cosmology-observations/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:48:02 +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[astrophysical sources]]></category>
		<category><![CDATA[bao]]></category>
		<category><![CDATA[calibration]]></category>
		<category><![CDATA[contamination]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[foreground]]></category>
		<category><![CDATA[impediment]]></category>
		<category><![CDATA[instrumental effects]]></category>
		<category><![CDATA[origins]]></category>
		<category><![CDATA[power spectra]]></category>
		<category><![CDATA[power spectrum]]></category>
		<category><![CDATA[shape]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[subtraction]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/four-fundamental-foreground-power-spectrum-shapes-for-21-cm-cosmology-observations/</guid>
		<description><![CDATA[Contamination from instrumental effects interacting with bright astrophysical sources is the primary impediment to measuring Epoch of Reionization and BAO 21 cm power spectra-an effect called mode-mixing. In this paper we identify four fundamental power spectrum shapes produced by mode-mixing that will affect all upcoming observations. We are able, for the first time, to explain [...]]]></description>
			<content:encoded><![CDATA[<p>Contamination from instrumental effects interacting with bright astrophysical sources is the primary impediment to measuring Epoch of Reionization and BAO 21 cm power spectra-an effect called mode-mixing. In this paper we identify four fundamental power spectrum shapes produced by mode-mixing that will affect all upcoming observations. We are able, for the first time, to explain the wedge-like structure seen in advanced simulations and to forecast the shape of an &#8216;EoR window&#8217; that is mostly free of contamination. Understanding the origins of these contaminations also enables us to identify calibration and foreground subtraction errors below the imaging limit, providing a powerful new tool for precision observations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/four-fundamental-foreground-power-spectrum-shapes-for-21-cm-cosmology-observations/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Cosmicflows-2: SNIa Calibration and H0</title>
		<link>http://voxcharta.org/2012/02/19/cosmicflows-2-snia-calibration-and-h0/</link>
		<comments>http://voxcharta.org/2012/02/19/cosmicflows-2-snia-calibration-and-h0/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:47:46 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accurate distances]]></category>
		<category><![CDATA[calibration]]></category>
		<category><![CDATA[cepheid]]></category>
		<category><![CDATA[cosmological model]]></category>
		<category><![CDATA[distortions]]></category>
		<category><![CDATA[fluctuation]]></category>
		<category><![CDATA[fundamental plane]]></category>
		<category><![CDATA[giant branch]]></category>
		<category><![CDATA[hubble constant]]></category>
		<category><![CDATA[hubble flow]]></category>
		<category><![CDATA[Lambda]]></category>
		<category><![CDATA[peculiar motion]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[snia]]></category>
		<category><![CDATA[spiral]]></category>
		<category><![CDATA[surface brightness]]></category>
		<category><![CDATA[trgb]]></category>
		<category><![CDATA[type ia supernova]]></category>
		<category><![CDATA[zero point]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/cosmicflows-2-snia-calibration-and-h0/</guid>
		<description><![CDATA[The construction of the Cosmicflows-2 compendium of distances involves the merging of distance measures contributed by the following methods: (Cepheid) Period-Luminosity, Tip of the Red Giant Branch (TRGB), Surface Brightness Fluctuation (SBF), Luminosity-Linewidth (TF), Fundamental Plane (FP), and Type Ia supernova (SNIa). The method involving SNIa is at the top of an interconnected ladder, providing [...]]]></description>
			<content:encoded><![CDATA[<p>The construction of the Cosmicflows-2 compendium of distances involves the merging of distance measures contributed by the following methods: (Cepheid) Period-Luminosity, Tip of the Red Giant Branch (TRGB), Surface Brightness Fluctuation (SBF), Luminosity-Linewidth (TF), Fundamental Plane (FP), and Type Ia supernova (SNIa). The method involving SNIa is at the top of an interconnected ladder, providing accurate distances to well beyond the expected range of distortions to Hubble flow from peculiar motions. In this paper, the SNIa scale is anchored by 36 TF spirals with Cepheid or TRGB distances, 56 SNIa hosts with TF distances, and 61 groups or clusters hosting SNIa with Cepheid, SBF, TF, or FP distances. With the SNIa scale zero point set, a value of the Hubble Constant is evaluated over a range of redshifts 0.03 &lt; z &lt; 0.5, assuming a cosmological model with Omega_m = 0.27 and Omega_Lambda = 0.73. The value determined for the Hubble Constant is H0 = 75.9 \pm 3.8 km s-1 Mpc-1.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/cosmicflows-2-snia-calibration-and-h0/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Primordial seeds of supermassive black holes</title>
		<link>http://voxcharta.org/2012/02/19/primordial-seeds-of-supermassive-black-holes/</link>
		<comments>http://voxcharta.org/2012/02/19/primordial-seeds-of-supermassive-black-holes/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:46:38 +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[1 million]]></category>
		<category><![CDATA[density perturbations]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[inflation]]></category>
		<category><![CDATA[inflationary epoch]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[period]]></category>
		<category><![CDATA[population]]></category>
		<category><![CDATA[scalar field]]></category>
		<category><![CDATA[seeds]]></category>
		<category><![CDATA[solar mass]]></category>
		<category><![CDATA[spectrum]]></category>
		<category><![CDATA[supermassive black hole]]></category>
		<category><![CDATA[transition]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/primordial-seeds-of-supermassive-black-holes/</guid>
		<description><![CDATA[Supermassive black holes exist in the centers of galaxies, including Milky Way, but there is no compelling theory of their formation. Furthermore, observations of quasars imply that supermassive black holes have already existed at some very high redshifts, suggesting the possibility of their primordial origin. In a class of well-motivated models, inflationary epoch could include [...]]]></description>
			<content:encoded><![CDATA[<p>Supermassive black holes exist in the centers of galaxies, including Milky Way, but there is no compelling theory of their formation. Furthermore, observations of quasars imply that supermassive black holes have already existed at some very high redshifts, suggesting the possibility of their primordial origin. In a class of well-motivated models, inflationary epoch could include two or more periods of inflation dominated by different scalar fields. The transition between such periods of inflation could enhance the spectrum of density perturbations on some specific scale, which could lead to formation of primordial black holes with a very narrow range of masses of the order of 0.1 to 1 million solar masses. These primordial black holes could have provided the requisite seeds for the observed population of supermassive black holes.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/primordial-seeds-of-supermassive-black-holes/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The SL2S Galaxy-scale Gravitational Lens Sample. I: The alignment of mass and light in massive early-type galaxies at z=0.2-0.9</title>
		<link>http://voxcharta.org/2012/02/19/the-sl2s-galaxy-scale-gravitational-lens-sample-i-the-alignment-of-mass-and-light-in-massive-early-type-galaxies-at-z0-2-0-9/</link>
		<comments>http://voxcharta.org/2012/02/19/the-sl2s-galaxy-scale-gravitational-lens-sample-i-the-alignment-of-mass-and-light-in-massive-early-type-galaxies-at-z0-2-0-9/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:46:20 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[canada france]]></category>
		<category><![CDATA[companion paper]]></category>
		<category><![CDATA[cosmic time]]></category>
		<category><![CDATA[dark matter content]]></category>
		<category><![CDATA[elongation]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gravitational lens]]></category>
		<category><![CDATA[gravitational lenses]]></category>
		<category><![CDATA[hawaii]]></category>
		<category><![CDATA[keck]]></category>
		<category><![CDATA[legacy]]></category>
		<category><![CDATA[lens model]]></category>
		<category><![CDATA[mass distribution]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[position angle]]></category>
		<category><![CDATA[relative alignment]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[subset]]></category>
		<category><![CDATA[type galaxy]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/the-sl2s-galaxy-scale-gravitational-lens-sample-i-the-alignment-of-mass-and-light-in-massive-early-type-galaxies-at-z0-2-0-9/</guid>
		<description><![CDATA[We study the relative alignment of mass and light in a sample of 16 massive early-type galaxies at z=0.2-0.9 that act as strong gravitational lenses. The sample was identified from deep multiband images obtained as part of the Canada France Hawaii Legacy Survey (CFHTLS) as part of the Strong Lensing Legacy Survey (SL2S). Higher resolution [...]]]></description>
			<content:encoded><![CDATA[<p>We study the relative alignment of mass and light in a sample of 16 massive early-type galaxies at z=0.2-0.9 that act as strong gravitational lenses. The sample was identified from deep multiband images obtained as part of the Canada France Hawaii Legacy Survey (CFHTLS) as part of the Strong Lensing Legacy Survey (SL2S). Higher resolution follow-up imaging is available for a subset of 10 systems. We construct gravitational lens models and infer total enclosed mass, elongation, and position angle of the mass distribution. By comparison with the observed distribution of light we infer that there is a substantial amount of external shear $ \approx 0.12$, arising most likely from the environment of the SL2S lenses. In a companion paper (Ruff et al. 2011) we combine these measurements with follow-up Keck spectroscopy to study the evolution of the stellar and dark matter content of early-type galaxies as a function of cosmic time.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/the-sl2s-galaxy-scale-gravitational-lens-sample-i-the-alignment-of-mass-and-light-in-massive-early-type-galaxies-at-z0-2-0-9/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Periodic Radio Variability in NRAO 530: Phase Dispersion Minimization Analysis</title>
		<link>http://voxcharta.org/2012/02/19/periodic-radio-variability-in-nrao-530-phase-dispersion-minimization-analysis/</link>
		<comments>http://voxcharta.org/2012/02/19/periodic-radio-variability-in-nrao-530-phase-dispersion-minimization-analysis/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:46:04 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion disk]]></category>
		<category><![CDATA[blazar]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[instabilities]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[Monte Carlo]]></category>
		<category><![CDATA[nrao]]></category>
		<category><![CDATA[numerical simulation]]></category>
		<category><![CDATA[oscillation]]></category>
		<category><![CDATA[periodic components]]></category>
		<category><![CDATA[periodic fluctuations]]></category>
		<category><![CDATA[periodicity]]></category>
		<category><![CDATA[periodogram]]></category>
		<category><![CDATA[phase dispersion]]></category>
		<category><![CDATA[radio light]]></category>
		<category><![CDATA[reliability]]></category>
		<category><![CDATA[statistical confidence]]></category>
		<category><![CDATA[variability]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/periodic-radio-variability-in-nrao-530-phase-dispersion-minimization-analysis/</guid>
		<description><![CDATA[In this paper, a periodicity analysis of the radio light curves of the blazar NRAO 530 at 14.5, 8.0, and 4.8 GHz is presented employing an improved Phase Dispersion Minimization (PDM) technique. The result, which shows two persistent periodic components of $ \sim 6$ and $ \sim 10$ years at all three frequencies, is consistent [...]]]></description>
			<content:encoded><![CDATA[<p>In this paper, a periodicity analysis of the radio light curves of the blazar NRAO 530 at 14.5, 8.0, and 4.8 GHz is presented employing an improved Phase Dispersion Minimization (PDM) technique. The result, which shows two persistent periodic components of $ \sim 6$ and $ \sim 10$ years at all three frequencies, is consistent with the results obtained with the Lomb-Scargle periodogram and weighted wavelet Z-transform algorithms. The reliability of the derived periodicities is confirmed by the Monte Carlo numerical simulations which show a high statistical confidence. (Quasi-)Periodic fluctuations of the radio luminosity of NRAO 530 might be associated with the oscillations of the accretion disk triggered by hydrodynamic instabilities of the accreted flow. \keywords{methods: statistical &#8212; galaxies: active &#8212; galaxies: quasar: individual: NRAO 530}</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/periodic-radio-variability-in-nrao-530-phase-dispersion-minimization-analysis/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Herschel-ATLAS: VISTA VIKING near-IR counterparts in the Phase 1 GAMA 9h data</title>
		<link>http://voxcharta.org/2012/02/19/herschel-atlas-vista-viking-near-ir-counterparts-in-the-phase-1-gama-9h-data/</link>
		<comments>http://voxcharta.org/2012/02/19/herschel-atlas-vista-viking-near-ir-counterparts-in-the-phase-1-gama-9h-data/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:45:39 +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[atlas vista]]></category>
		<category><![CDATA[colours]]></category>
		<category><![CDATA[counterpart]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[herschel]]></category>
		<category><![CDATA[infrared data]]></category>
		<category><![CDATA[likelihood ratio]]></category>
		<category><![CDATA[object catalogue]]></category>
		<category><![CDATA[optical identification]]></category>
		<category><![CDATA[phase 1]]></category>
		<category><![CDATA[population]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[reliability]]></category>
		<category><![CDATA[search radius]]></category>
		<category><![CDATA[sigma]]></category>
		<category><![CDATA[spire]]></category>
		<category><![CDATA[viking]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/herschel-atlas-vista-viking-near-ir-counterparts-in-the-phase-1-gama-9h-data/</guid>
		<description><![CDATA[We identify near-infrared Ks band counterparts to Herschel-ATLAS sub-mm sources, using a preliminary object catalogue from the VISTA VIKING survey. The sub-mm sources are selected from the H-ATLAS Phase 1 catalogue of the GAMA 9h field, which includes all objects detected at 250, 350 or 500 um with the SPIRE instrument. We apply and discuss [...]]]></description>
			<content:encoded><![CDATA[<p>We identify near-infrared Ks band counterparts to Herschel-ATLAS sub-mm sources, using a preliminary object catalogue from the VISTA VIKING survey. The sub-mm sources are selected from the H-ATLAS Phase 1 catalogue of the GAMA 9h field, which includes all objects detected at 250, 350 or 500 um with the SPIRE instrument. We apply and discuss a likelihood ratio (LR) method for VIKING candidates within a search radius of 10&#8243; of the 22,000 SPIRE sources with a 5 sigma detection at 250 um. We find that 11,294(51%) of the SPIRE sources have a best VIKING counterpart with a reliability $R\ge 0.8$, and the false identification rate of these is estimated to be 4.2%. We expect to miss ~5% of true VIKING counterparts. There is evidence from Z-J and J-Ks colours that the reliable counterparts to SPIRE galaxies are marginally redder than the field population. We obtain photometric redshifts for ~68% of all (non-stellar) VIKING candidates with a median redshift of 0.405. Comparing to the results of the optical identifications supplied with the Phase I catalogue, we find that the use of medium-deep near-infrared data improves the identification rate of reliable counterparts from 36% to 51%.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/herschel-atlas-vista-viking-near-ir-counterparts-in-the-phase-1-gama-9h-data/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Constraints on quintessence and new physics from fundamental constant</title>
		<link>http://voxcharta.org/2012/02/19/constraints-on-quintessence-and-new-physics-from-fundamental-constant/</link>
		<comments>http://voxcharta.org/2012/02/19/constraints-on-quintessence-and-new-physics-from-fundamental-constant/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:44:15 +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[conformation]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[cosmological model]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[coupling constants]]></category>
		<category><![CDATA[Delta]]></category>
		<category><![CDATA[early universe]]></category>
		<category><![CDATA[electron mass]]></category>
		<category><![CDATA[equation of state]]></category>
		<category><![CDATA[fundamental constant]]></category>
		<category><![CDATA[mass ratio]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[mu alpha]]></category>
		<category><![CDATA[new physics]]></category>
		<category><![CDATA[proton]]></category>
		<category><![CDATA[quintessence]]></category>
		<category><![CDATA[scalar field]]></category>
		<category><![CDATA[symmetry]]></category>
		<category><![CDATA[zeta]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/constraints-on-quintessence-and-new-physics-from-fundamental-constant/</guid>
		<description><![CDATA[Changes in the values of the fundamental constants mu, the proton to electron mass ratio, and alpha, the fine structure constant due to rolling scalar fields have been discussed both in the context of cosmology and in new physics such as Super Symmetry (SUSY) models. This article examines the changes in these fundamental constants in [...]]]></description>
			<content:encoded><![CDATA[<p>Changes in the values of the fundamental constants mu, the proton to electron mass ratio, and alpha, the fine structure constant due to rolling scalar fields have been discussed both in the context of cosmology and in new physics such as Super Symmetry (SUSY) models. This article examines the changes in these fundamental constants in a particular example of such fields, freezing and thawing slow roll quintessence. Constraints are placed on the product of a cosmological quantity, w, the equation of state parameter, and the square of the coupling constants for mu and alpha with the field, zeta_x, x = mu,alpha, using the existing observational limits on the values of Delta x/x. Various examples of slow rolling quintessence models are used to further quantify the constraints. Some of the examples appear to be rejected by the existing data which strongly suggests that conformation to the values of the fundamental constants in the early universe is a standard test that should be applied to any cosmological model or suggested new physics.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/constraints-on-quintessence-and-new-physics-from-fundamental-constant/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Shift of the Baryon Acoustic Oscillation Scale: A Simple Physical Picture</title>
		<link>http://voxcharta.org/2012/02/19/the-shift-of-the-baryon-acoustic-oscillation-scale-a-simple-physical-picture/</link>
		<comments>http://voxcharta.org/2012/02/19/the-shift-of-the-baryon-acoustic-oscillation-scale-a-simple-physical-picture/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:40:52 +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[analytic expression]]></category>
		<category><![CDATA[bia]]></category>
		<category><![CDATA[correlation function]]></category>
		<category><![CDATA[fluctuation]]></category>
		<category><![CDATA[fourier space]]></category>
		<category><![CDATA[linear growth]]></category>
		<category><![CDATA[linear theory]]></category>
		<category><![CDATA[Measurement]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[next generation]]></category>
		<category><![CDATA[oscillation]]></category>
		<category><![CDATA[perturbation theory]]></category>
		<category><![CDATA[reconstruction]]></category>
		<category><![CDATA[shape]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[simulation result]]></category>
		<category><![CDATA[theory calculations]]></category>
		<category><![CDATA[tracers]]></category>
		<category><![CDATA[wavelength]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/the-shift-of-the-baryon-acoustic-oscillation-scale-a-simple-physical-picture/</guid>
		<description><![CDATA[A shift of the baryon acoustic oscillation (BAO) scale to smaller values than predicted by linear theory was observed in simulations. In this paper, we try to provide an intuitive physical understanding of why this shift occurs, explaining in more pedagogical detail earlier perturbation theory calculations. We find that the shift is mainly due to [...]]]></description>
			<content:encoded><![CDATA[<p>A shift of the baryon acoustic oscillation (BAO) scale to smaller values than predicted by linear theory was observed in simulations. In this paper, we try to provide an intuitive physical understanding of why this shift occurs, explaining in more pedagogical detail earlier perturbation theory calculations. We find that the shift is mainly due to the following physical effect. A measurement of the BAO scale is more sensitive to regions with long wavelength overdensities than underdensities, because (due to non-linear growth and bias) these overdense regions contain larger fluctuations and more tracers and hence contribute more to the total correlation function. In overdense regions the BAO scale shrinks because such regions locally behave as positively curved closed universes, and hence a smaller scale than predicted by linear theory is measured in the total correlation function. Other effects which also contribute to the shift are briefly discussed. We provide approximate analytic expressions for the non-linear shift including a brief discussion of biased tracers, and note that the shifts are different in real and Fourier space due to a change of the shape of the BAO feature. We explain why reconstruction should entirely reverse the shift. Our expressions and findings are in agreement with simulation results, and confirm that non-linear shifts should not be problematic for next-generation BAO measurements.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/the-shift-of-the-baryon-acoustic-oscillation-scale-a-simple-physical-picture/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Generalized Non-Commutative Inflation [Replacement]</title>
		<link>http://voxcharta.org/2012/02/19/generalized-non-commutative-inflation-replacement-2/</link>
		<comments>http://voxcharta.org/2012/02/19/generalized-non-commutative-inflation-replacement-2/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:39:09 +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[alexander]]></category>
		<category><![CDATA[brandenberger]]></category>
		<category><![CDATA[curves]]></category>
		<category><![CDATA[deformation]]></category>
		<category><![CDATA[dispersion relation]]></category>
		<category><![CDATA[fundamental equation]]></category>
		<category><![CDATA[high temperature]]></category>
		<category><![CDATA[inequality]]></category>
		<category><![CDATA[inflation]]></category>
		<category><![CDATA[magueijo]]></category>
		<category><![CDATA[massless particle]]></category>
		<category><![CDATA[momentum]]></category>
		<category><![CDATA[non commutative geometry]]></category>
		<category><![CDATA[numerical approach]]></category>
		<category><![CDATA[parameter family]]></category>
		<category><![CDATA[radiation]]></category>
		<category><![CDATA[scalar field]]></category>
		<category><![CDATA[symmetry]]></category>
		<category><![CDATA[universe]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/generalized-non-commutative-inflation-replacement-2/</guid>
		<description><![CDATA[Non-commutative geometry indicates a deformation of the energy-momentum dispersion relation $f(E)\equiv\frac{E}{pc}(\neq 1)$ for massless particles. This distorted energy-momentum relation can affect the radiation dominated phase of the universe at sufficiently high temperature. This prompted the idea of non-commutative inflation by Alexander, Brandenberger and Magueijo (2003, 2005 and 2007). These authors studied a one-parameter family of [...]]]></description>
			<content:encoded><![CDATA[<p>Non-commutative geometry indicates a deformation of the energy-momentum dispersion relation $f(E)\equiv\frac{E}{pc}(\neq 1)$ for massless particles. This distorted energy-momentum relation can affect the radiation dominated phase of the universe at sufficiently high temperature. This prompted the idea of non-commutative inflation by Alexander, Brandenberger and Magueijo (2003, 2005 and 2007). These authors studied a one-parameter family of non-relativistic dispersion relation that leads to inflation: the $\alpha$ family of curves $f(E)=1+(\lambda E)^{\alpha}$. We show here how the conceptually different structure of symmetries of non-commutative spaces can lead, in a mathematically consistent way, to the fundamental equations of non-commutative inflation driven by radiation. We describe how this structure can be considered independently of (but including) the idea of non-commutative spaces as a starting point of the general inflationary deformation of $SL(2,\mathbb{C})$. We analyze the conditions on the dispersion relation that leads to inflation as a set of inequalities which plays the same role as the slow roll conditions on the potential of a scalar field. We study conditions for a possible numerical approach to obtain a general one parameter family of dispersion relations that lead to successful inflation.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/generalized-non-commutative-inflation-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Distribution function approach to redshift space distortions. Part II: N-body simulations [Replacement]</title>
		<link>http://voxcharta.org/2012/02/19/distribution-function-approach-to-redshift-space-distortions-part-ii-n-body-simulations-replacement-2/</link>
		<comments>http://voxcharta.org/2012/02/19/distribution-function-approach-to-redshift-space-distortions-part-ii-n-body-simulations-replacement-2/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:38:34 +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[attractive method]]></category>
		<category><![CDATA[auto correlation]]></category>
		<category><![CDATA[body simulation]]></category>
		<category><![CDATA[convergence]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[cosine]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[density perturbations]]></category>
		<category><![CDATA[distortions]]></category>
		<category><![CDATA[distribution function]]></category>
		<category><![CDATA[dominant term]]></category>
		<category><![CDATA[energy density]]></category>
		<category><![CDATA[finger of god]]></category>
		<category><![CDATA[finite number]]></category>
		<category><![CDATA[growth history]]></category>
		<category><![CDATA[line of sight]]></category>
		<category><![CDATA[momentum]]></category>
		<category><![CDATA[mpc]]></category>
		<category><![CDATA[order of magnitude]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/distribution-function-approach-to-redshift-space-distortions-part-ii-n-body-simulations-replacement-2/</guid>
		<description><![CDATA[Measurement of redshift-space distortions (RSD) offers an attractive method to directly probe the cosmic growth history of density perturbations. A distribution function approach where RSD can be written as a sum over density weighted velocity moment correlators has recently been developed. We use Nbody simulations to investigate the individual contributions and convergence of this expansion [...]]]></description>
			<content:encoded><![CDATA[<p>Measurement of redshift-space distortions (RSD) offers an attractive method to directly probe the cosmic growth history of density perturbations. A distribution function approach where RSD can be written as a sum over density weighted velocity moment correlators has recently been developed. We use Nbody simulations to investigate the individual contributions and convergence of this expansion for dark matter. If the series is expanded as a function of powers of mu, cosine of the angle between the Fourier mode and line of sight, there are a finite number of terms contributing at each order. We present these terms and investigate their contribution to the total as a function of wavevector k. For mu^2 the correlation between density and momentum dominates on large scales. Higher order corrections, which act as a Finger-of-God (FoG) term, contribute 1% at k~0.015h/Mpc, 10% at k~0.05h/Mpc at z=0, while for k&gt;0.15h/Mpc they dominate and make the total negative. These higher order terms are dominated by density-energy density correlations which contribute negatively to the power, while the contribution from vorticity part of momentum density auto-correlation is an order of magnitude lower. For mu^4 term the dominant term on large scales is the scalar part of momentum density auto-correlation, while higher order terms dominate for k&gt;0.15h/Mpc. For mu^6 and mu^8 we find it has very little power for k&lt;0.15h/Mpc. We also compare the expansion to the full 2D P^ss(k,mu) as well as to their multipoles. For these statistics an infinite number of terms contribute and we find that the expansion achieves percent level accuracy for kmu&lt;0.15h/Mpc at 6th order, but breaks down on smaller scales because the series is no longer perturbative. We explore resummation of the terms into FoG kernels, which extend the convergence up to a factor of 2 in scale. We find that the FoG kernels are approximately Lorentzian.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/distribution-function-approach-to-redshift-space-distortions-part-ii-n-body-simulations-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Evidence for a non-universal stellar initial mass function in low-redshift high-density early-type galaxies [Replacement]</title>
		<link>http://voxcharta.org/2012/02/19/evidence-for-a-non-universal-stellar-initial-mass-function-in-low-redshift-high-density-early-type-galaxies-replacement/</link>
		<comments>http://voxcharta.org/2012/02/19/evidence-for-a-non-universal-stellar-initial-mass-function-in-low-redshift-high-density-early-type-galaxies-replacement/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:37:47 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absolute calibration]]></category>
		<category><![CDATA[chabrier]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[high density]]></category>
		<category><![CDATA[imf]]></category>
		<category><![CDATA[initial mass function]]></category>
		<category><![CDATA[ratios]]></category>
		<category><![CDATA[sdss]]></category>
		<category><![CDATA[sigma]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[stellar surface]]></category>
		<category><![CDATA[Sun]]></category>
		<category><![CDATA[synthesis]]></category>
		<category><![CDATA[type galaxy]]></category>
		<category><![CDATA[universe]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/evidence-for-a-non-universal-stellar-initial-mass-function-in-low-redshift-high-density-early-type-galaxies-replacement/</guid>
		<description><![CDATA[We determine an absolute calibration of stellar mass-to-light ratios for the densest \simeq 3% of early-type galaxies in the local universe (redshift z\simeq 0.08) from SDSS DR7. This sample of \sim 4000 galaxies has, assuming a Chabrier IMF, effective stellar surface densities, Sigma_e &#62; 2500 M_sun/pc^2, stellar population synthesis (SPS) stellar masses log_10(M_sps/M_sun)&#60;10.8, and aperture [...]]]></description>
			<content:encoded><![CDATA[<p>We determine an absolute calibration of stellar mass-to-light ratios for the densest \simeq 3% of early-type galaxies in the local universe (redshift z\simeq 0.08) from SDSS DR7. This sample of \sim 4000 galaxies has, assuming a Chabrier IMF, effective stellar surface densities, Sigma_e &gt; 2500 M_sun/pc^2, stellar population synthesis (SPS) stellar masses log_10(M_sps/M_sun)&lt;10.8, and aperture velocity dispersions of sigma_ap=168^{+37}_{-34} km/s (68% range). In contrast to typical early-type galaxies, we show that these dense early-type galaxies follow the virial fundamental plane, which suggests that mass-follows-light. With the additional assumption that any dark matter does not follow the light, the dynamical masses of dense galaxies provide a direct measurement of stellar masses. Our dynamical masses (M_dyn), obtained from the spherical Jeans equations, are only weakly sensitive to the choice of anisotropy (\beta) due to the relatively large aperture of the SDSS fiber for these galaxies: R_ap \simeq 1.5 R_e. Assuming isotropic orbits (\beta=0) we find a median log_{10} (M_dyn/M_sps) = 0.233 \pm 0.003, consistent with a Salpeter IMF, while more bottom heavy IMFs and standard Milky-Way IMFs are strongly disfavored. Our results are consistent with, but do not require, a dependence of the IMF on dynamical mass or velocity dispersion. We find evidence for a color dependence to the IMF such that redder galaxies have heavier IMFs with M_dyn/M_sps \propto (g-r)^{1.13\pm0.09}. This may reflect a more fundamental dependence of the IMF on the age or metallicity of a stellar population, or the density at which the stars formed.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/evidence-for-a-non-universal-stellar-initial-mass-function-in-low-redshift-high-density-early-type-galaxies-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Near-Infrared Properties of Type Ia Supernovae [Replacement]</title>
		<link>http://voxcharta.org/2012/02/19/near-infrared-properties-of-type-ia-supernovae-replacement/</link>
		<comments>http://voxcharta.org/2012/02/19/near-infrared-properties-of-type-ia-supernovae-replacement/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:35:29 +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[decline]]></category>
		<category><![CDATA[dependence]]></category>
		<category><![CDATA[homogeneity]]></category>
		<category><![CDATA[infrared properties]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[peak luminosity]]></category>
		<category><![CDATA[period light]]></category>
		<category><![CDATA[photometric properties]]></category>
		<category><![CDATA[sne ia]]></category>
		<category><![CDATA[standard candle]]></category>
		<category><![CDATA[type ia supernovae]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/near-infrared-properties-of-type-ia-supernovae-replacement/</guid>
		<description><![CDATA[The photometric properties of Type Ia supernovae (SNe Ia) in the near-infrared as garnered from observations made over the last 30 years are reviewed. During this period, light curves for more than 120 nearby SNe Ia have been published, revealing considerable homogeneity but also some fascinating differences. These data have confirmed that, for all but [...]]]></description>
			<content:encoded><![CDATA[<p>The photometric properties of Type Ia supernovae (SNe Ia) in the near-infrared as garnered from observations made over the last 30 years are reviewed. During this period, light curves for more than 120 nearby SNe Ia have been published, revealing considerable homogeneity but also some fascinating differences. These data have confirmed that, for all but the fastest declining objects, SNe Ia are essentially perfect standard candles in the near-infrared, displaying only a slight dependence of peak luminosity on decline rate and color.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/near-infrared-properties-of-type-ia-supernovae-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Internal Stellar Kinematics of M32 from the SPLASH Survey: Dark Halo Constraints and the Formation of Compact Elliptical Galaxies [Replacement]</title>
		<link>http://voxcharta.org/2012/02/19/internal-stellar-kinematics-of-m32-from-the-splash-survey-dark-halo-constraints-and-the-formation-of-compact-elliptical-galaxies-replacement/</link>
		<comments>http://voxcharta.org/2012/02/19/internal-stellar-kinematics-of-m32-from-the-splash-survey-dark-halo-constraints-and-the-formation-of-compact-elliptical-galaxies-replacement/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:32:46 +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[andromeda galaxy m31]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[dark halo]]></category>
		<category><![CDATA[deimos]]></category>
		<category><![CDATA[elliptical galaxy]]></category>
		<category><![CDATA[keck]]></category>
		<category><![CDATA[m32]]></category>
		<category><![CDATA[neighbor]]></category>
		<category><![CDATA[satellite]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[stellar kinematics]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/internal-stellar-kinematics-of-m32-from-the-splash-survey-dark-halo-constraints-and-the-formation-of-compact-elliptical-galaxies-replacement/</guid>
		<description><![CDATA[As part of the SPLASH survey of the Andromeda galaxy (M31) and its neighbors, we have obtained Keck/DEIMOS spectra of the compact elliptical (cE) satellite M32. This is the first resolved-star kinematical study of any cE galaxy. In contrast to previous studies that extended out to r&#60;30&#34;~1Re~100pc, we measure the rotation curve and velocity dispersion [...]]]></description>
			<content:encoded><![CDATA[<p>As part of the SPLASH survey of the Andromeda galaxy (M31) and its neighbors, we have obtained Keck/DEIMOS spectra of the compact elliptical (cE) satellite M32. This is the first resolved-star kinematical study of any cE galaxy. In contrast to previous studies that extended out to r&lt;30&quot;~1Re~100pc, we measure the rotation curve and velocity dispersion profile out to r~250&quot; and higher order Gauss-Hermite moments out to r~70&quot;. We achieve this by combining integrated-light spectroscopy at small radii (where crowding/blending are severe) with resolved stellar spectroscopy at larger radii, using spatial and kinematical information to statistically account for M31 contamination. The rotation curve and velocity dispersion profile extend well beyond the radius (r~150&quot;) where the isophotes are distorted. Unlike NGC 205, another close dwarf companion of M31, M32&#039;s kinematic are regular and symmetric and do not show obvious sharp gradients across the region of isophotal elongation and twists. We interpret M31&#039;s kinematics using three-integral axisymmetric dynamical equilibrium models constructed using Schwarzschild&#039;s orbit superposition technique. Models with a constant M/L can fit the data remarkably well. However, since such a model requires an increasing tangential anisotropy with radius, invoking the presence of an extended dark halo may be more plausible. Such an extended dark halo is definitely required to bind a half-dozen fast-moving stars observed at the largest radii, but these stars may not be an equilibrium component of M32. The observed regularity of the stellar kinematics, as well as the possible detection of an extended dark halo, are unexpected if M31 tides are significant at large radii. While these findings by themselves do not rule out tidal models for cE formation, they suggest that tidal stripping may not be as significant for shaping cE galaxies as has often been argued.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/internal-stellar-kinematics-of-m32-from-the-splash-survey-dark-halo-constraints-and-the-formation-of-compact-elliptical-galaxies-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The AGB population of NGC 6822: distribution and the C/M ratio from JHK photometry [Replacement]</title>
		<link>http://voxcharta.org/2012/02/19/the-agb-population-of-ngc-6822-distribution-and-the-cm-ratio-from-jhk-photometry-replacement/</link>
		<comments>http://voxcharta.org/2012/02/19/the-agb-population-of-ngc-6822-distribution-and-the-cm-ratio-from-jhk-photometry-replacement/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:32:33 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[agb stars]]></category>
		<category><![CDATA[asymptotic giant branch]]></category>
		<category><![CDATA[calibration]]></category>
		<category><![CDATA[close proximity]]></category>
		<category><![CDATA[colour separation]]></category>
		<category><![CDATA[dwarf galaxy]]></category>
		<category><![CDATA[galactic evolution]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gradient]]></category>
		<category><![CDATA[iron abundance]]></category>
		<category><![CDATA[isolation]]></category>
		<category><![CDATA[jhk]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[local group]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[metallicity]]></category>
		<category><![CDATA[oxygen]]></category>
		<category><![CDATA[photometry]]></category>
		<category><![CDATA[selection criteria]]></category>
		<category><![CDATA[spatial distribution]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/the-agb-population-of-ngc-6822-distribution-and-the-cm-ratio-from-jhk-photometry-replacement/</guid>
		<description><![CDATA[NGC 6822 is an irregular dwarf galaxy and part of the Local Group. Its close proximity and apparent isolation provide a unique opportunity to study galactic evolution without any obvious strong external influences. This paper aims to study the spatial distribution of the asymptotic giant branch (AGB) population and metallicity in NGC 6822. Using deep, [...]]]></description>
			<content:encoded><![CDATA[<p>NGC 6822 is an irregular dwarf galaxy and part of the Local Group. Its close proximity and apparent isolation provide a unique opportunity to study galactic evolution without any obvious strong external influences. This paper aims to study the spatial distribution of the asymptotic giant branch (AGB) population and metallicity in NGC 6822. Using deep, high quality JHK photometry, taken with WFCAM on UKIRT, carbon- and oxygen-rich AGB stars have been isolated. The ratio between their number, the C/M ratio, has then been used to derive the [Fe/H] abundance across the galaxy. The tip of the red giant branch is located at K0 = 17.41 \pm 0.11 mag and the colour separation between carbon- and oxygen-rich AGB stars is at (J &#8211; K)0 = 1.20 \pm 0.03 mag (i.e. (J &#8211; K)2MAS S {\guillemotright} 1.28 mag). A C/M ratio of 0.62 \pm 0.03 has been derived in the inner 4 kpc of the galaxy, which translates into an iron abundance of [Fe/H] = -1.29\pm0.07 dex. Variations of these parameters were investigated as a function of distance from the galaxy centre and azimuthal angle. The AGB population of NGC 6822 has been detected out to a radius of 4 kpc giving a diameter of 56 arcmin. It is metal-poor, but there is no obvious gradient in metallicity with either radial distance from the centre or azimuthal angle. The detected spread in the TRGB magnitude is consistent with that of a galaxy surrounded by a halo of old stars. The C/M ratio has the potential to be a very useful tool for the determination of metallicity in resolved galaxies but a better calibration of the C/M vs. [Fe/H] relation and a better understanding of the sensitivities of the C/M ratio to stellar selection criteria is first required.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/the-agb-population-of-ngc-6822-distribution-and-the-cm-ratio-from-jhk-photometry-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Distinguishing among dark matter annihilation channels with neutrino telescopes [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/19/distinguishing-among-dark-matter-annihilation-channels-with-neutrino-telescopes-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/19/distinguishing-among-dark-matter-annihilation-channels-with-neutrino-telescopes-cross-listing/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:32:18 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[annihilation]]></category>
		<category><![CDATA[array]]></category>
		<category><![CDATA[capability]]></category>
		<category><![CDATA[dark matter particles]]></category>
		<category><![CDATA[experimental error]]></category>
		<category><![CDATA[gauge]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[IceCube]]></category>
		<category><![CDATA[neutrino]]></category>
		<category><![CDATA[neutrino flux]]></category>
		<category><![CDATA[neutrino telescope]]></category>
		<category><![CDATA[novel method]]></category>
		<category><![CDATA[prospects]]></category>
		<category><![CDATA[ratios]]></category>
		<category><![CDATA[reconstruction]]></category>
		<category><![CDATA[regeneration]]></category>
		<category><![CDATA[spectrum]]></category>
		<category><![CDATA[Sun]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/distinguishing-among-dark-matter-annihilation-channels-with-neutrino-telescopes-cross-listing/</guid>
		<description><![CDATA[We investigate the prospects for distinguishing dark matter annihilation channels using the neutrino flux from gravitationally captured dark matter particles annihilating inside the sun. We show that, even with experimental error in energy reconstruction taken into account, the spectrum of contained muon tracks may be used to discriminate neutrino final states from the gauge boson/charged [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate the prospects for distinguishing dark matter annihilation channels using the neutrino flux from gravitationally captured dark matter particles annihilating inside the sun. We show that, even with experimental error in energy reconstruction taken into account, the spectrum of contained muon tracks may be used to discriminate neutrino final states from the gauge boson/charged lepton final states and to determine their corresponding branching ratios. We also discuss the effect of $\nu_\tau$ regeneration inside the sun as a novel method to distinguish the flavor of final state neutrinos. This effect as evidenced in the muon spectrum becomes important for dark matter masses above 300 GeV. Distinguishing primary neutrinos and their flavor may be achieved using multi-year data from a detector with the same capability and effective volume as the IceCube/DeepCore array.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/distinguishing-among-dark-matter-annihilation-channels-with-neutrino-telescopes-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Detecting Cosmic Gravitational-wave Background from Super-heavy Cosmic Strings with LISA [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/19/detecting-cosmic-gravitational-wave-background-from-super-heavy-cosmic-strings-with-lisa-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/19/detecting-cosmic-gravitational-wave-background-from-super-heavy-cosmic-strings-with-lisa-cross-listing/#comments</comments>
		<pubDate>Mon, 20 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[algorithm]]></category>
		<category><![CDATA[cmb data]]></category>
		<category><![CDATA[cosmic string]]></category>
		<category><![CDATA[data stream]]></category>
		<category><![CDATA[detection threshold]]></category>
		<category><![CDATA[epsilon]]></category>
		<category><![CDATA[galaxy formation]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[observation]]></category>
		<category><![CDATA[parameter space]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/detecting-cosmic-gravitational-wave-background-from-super-heavy-cosmic-strings-with-lisa-cross-listing/</guid>
		<description><![CDATA[Although cosmic string scenario for galaxy formation is disfavored by CMB data, it is of great interest in the generation of cosmic gravitational-wave background. This research aims to develop an algorithm to extract cosmic gravitational-wave background produced by cosmic strings from the LISA data stream, and apply the algorithm to the simulated data stream containing [...]]]></description>
			<content:encoded><![CDATA[<p>Although cosmic string scenario for galaxy formation is disfavored by CMB data, it is of great interest in the generation of cosmic gravitational-wave background. This research aims to develop an algorithm to extract cosmic gravitational-wave background produced by cosmic strings from the LISA data stream, and apply the algorithm to the simulated data stream containing the background produced by cosmic strings with various strength to study the detection threshold for this source. For 1-yr observation, It is found that the detection threshold of G{\mu} is 3.12 \times 10^-16 in the standard scenario. In the case that p and {\epsilon} are adjustable, the detectable region in parameter space is defined by (G{\mu})^2/3 {\epsilon}^-1/3 / p&gt; 4.6 \times 10-11.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/detecting-cosmic-gravitational-wave-background-from-super-heavy-cosmic-strings-with-lisa-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>New remarks on the Cosmological Argument [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/19/new-remarks-on-the-cosmological-argument-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/19/new-remarks-on-the-cosmological-argument-cross-listing/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:31:04 +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[aim]]></category>
		<category><![CDATA[aquinas]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[conclusion]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[empirical science]]></category>
		<category><![CDATA[fallacy of equivocation]]></category>
		<category><![CDATA[kalam argument]]></category>
		<category><![CDATA[kalam cosmological argument]]></category>
		<category><![CDATA[language version]]></category>
		<category><![CDATA[logic]]></category>
		<category><![CDATA[natural language]]></category>
		<category><![CDATA[physicist]]></category>
		<category><![CDATA[premises and conclusions]]></category>
		<category><![CDATA[universe]]></category>
		<category><![CDATA[variation]]></category>
		<category><![CDATA[william lane craig]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/new-remarks-on-the-cosmological-argument-cross-listing/</guid>
		<description><![CDATA[We present a formal analysis of the Cosmological Argument in its two main forms: that due to Aquinas, and the revised version of the Kalam Cosmological Argument more recently advocated by William Lane Craig. We formulate these two arguments in such a way that each conclusion follows in first-order logic from the corresponding assumptions. Our [...]]]></description>
			<content:encoded><![CDATA[<p>We present a formal analysis of the Cosmological Argument in its two main forms: that due to Aquinas, and the revised version of the Kalam Cosmological Argument more recently advocated by William Lane Craig. We formulate these two arguments in such a way that each conclusion follows in first-order logic from the corresponding assumptions. Our analysis shows that the conclusion which follows for Aquinas is considerably weaker than what his aims demand. With formalizations that are logically valid in hand, we reinterpret the natural language versions of the premises and conclusions in terms of concepts of causality consistent with (and used in) recent work in cosmology done by physicists. In brief: the Kalam argument commits the fallacy of equivocation in a way that seems beyond repair; two of the premises adopted by Aquinas seem dubious when the terms `cause&#8217; and `causality&#8217; are interpreted in the context of contemporary empirical science. Thus, while there are no problems with whether the conclusions follow logically from their assumptions, the Kalam argument is not viable, and the Aquinas argument does not imply a caused origination of the universe. The assumptions of the latter are at best less than obvious relative to recent work in the sciences. We conclude with mention of a new argument that makes some positive modifications to an alternative variation on Aquinas by Le Poidevin, which nonetheless seems rather weak.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/new-remarks-on-the-cosmological-argument-cross-listing/feed/</wfw:commentRss>
		<slash:comments>3</slash:comments>
		</item>
		<item>
		<title>A large, multi-epoch H{\alpha} survey at z=2.23, 1.47, 0.84 &amp; 0.40: the 11 Gyr evolution of star-forming galaxies from HiZELS</title>
		<link>http://voxcharta.org/2012/02/16/a-large-multi-epoch-halpha-survey-at-z2-23-1-47-0-84-0-40-the-11-gyr-evolution-of-star-forming-galaxies-from-hizels/</link>
		<comments>http://voxcharta.org/2012/02/16/a-large-multi-epoch-halpha-survey-at-z2-23-1-47-0-84-0-40-the-11-gyr-evolution-of-star-forming-galaxies-from-hizels/#comments</comments>
		<pubDate>Fri, 17 Feb 2012 01:52:44 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[approximation]]></category>
		<category><![CDATA[combined effort]]></category>
		<category><![CDATA[compilation]]></category>
		<category><![CDATA[cosmic variance]]></category>
		<category><![CDATA[deg]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[fir]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gyr]]></category>
		<category><![CDATA[history of the universe]]></category>
		<category><![CDATA[luminosity function]]></category>
		<category><![CDATA[slope]]></category>
		<category><![CDATA[star formation history]]></category>
		<category><![CDATA[subaru]]></category>
		<category><![CDATA[tracers]]></category>
		<category><![CDATA[ukirt]]></category>
		<category><![CDATA[uniform analysis]]></category>
		<category><![CDATA[uniform manner]]></category>
		<category><![CDATA[vlt]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/16/a-large-multi-epoch-halpha-survey-at-z2-23-1-47-0-84-0-40-the-11-gyr-evolution-of-star-forming-galaxies-from-hizels/</guid>
		<description><![CDATA[This paper presents new deep and wide narrow-band surveys undertaken with UKIRT, Subaru and the VLT; a unique combined effort to select large, robust samples of H-alpha (Ha) emitters at z=0.40, 0.84, 1.47 and 2.23 (corresponding to look-back times of 4.2, 7.0, 9.2 and 10.6 Gyrs) in a uniform manner over ~2 deg^2 in the [...]]]></description>
			<content:encoded><![CDATA[<p>This paper presents new deep and wide narrow-band surveys undertaken with UKIRT, Subaru and the VLT; a unique combined effort to select large, robust samples of H-alpha (Ha) emitters at z=0.40, 0.84, 1.47 and 2.23 (corresponding to look-back times of 4.2, 7.0, 9.2 and 10.6 Gyrs) in a uniform manner over ~2 deg^2 in the COSMOS and UDS fields. The deep multi-epoch Ha surveys reach ~3M_sun/yr out to z=2.2 for the first time, while the wide area and the coverage over two independent fields allow to greatly overcome cosmic variance. A total of 1742, 637, 515 and 556 Ha emitters are homogeneously selected at z=0.40, 0.84, 1.47 and 2.23, respectively, and used to determine the Ha luminosity function and its evolution. The faint-end slope is found to be -1.60+-0.08 over z=0-2.23, showing no evolution. The characteristic luminosity of SF galaxies, L*, evolves significantly as log[L*(z)]=0.45z+log[L*(z=0)]. This is the first time Ha has been used to trace SF activity with a single homogeneous survey at z=0.4-2.23. Overall, the evolution seen in Ha is in good agreement with the evolution seen using inhomogeneous compilations of other tracers of star formation, such as FIR and UV, jointly pointing towards the bulk of the evolution in the last 11 Gyrs being driven by a strong luminosity increase from z~0 to z~2.2. Our uniform analysis allows to derive the Ha star formation history of the Universe, for which the simple parametrisation log(SFRD)=-2.1/(1+z) is a good approximation for z&lt;2.23. Both the shape and normalisation of the Ha star formation history are consistent with the measurements of the stellar mass density growth, confirming that our Ha analysis traces the bulk of the formation of stars in the Universe up to z~2.2. The star formation activity over the last ~11Gyrs is responsible for producing ~95% of the total stellar mass density observed locally today.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/16/a-large-multi-epoch-halpha-survey-at-z2-23-1-47-0-84-0-40-the-11-gyr-evolution-of-star-forming-galaxies-from-hizels/feed/</wfw:commentRss>
		<slash:comments>1</slash:comments>
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		<title>Plain fundamentals of Fundamental Planes: Analytics and algorithms</title>
		<link>http://voxcharta.org/2012/02/16/plain-fundamentals-of-fundamental-planes-analytics-and-algorithms/</link>
		<comments>http://voxcharta.org/2012/02/16/plain-fundamentals-of-fundamental-planes-analytics-and-algorithms/#comments</comments>
		<pubDate>Fri, 17 Feb 2012 01:51:55 +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[coefficients]]></category>
		<category><![CDATA[confidence limit]]></category>
		<category><![CDATA[correlated errors]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[decrement]]></category>
		<category><![CDATA[differential]]></category>
		<category><![CDATA[explicit expression]]></category>
		<category><![CDATA[fundamental plane]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[galaxy formation]]></category>
		<category><![CDATA[open question]]></category>
		<category><![CDATA[orthogonal]]></category>
		<category><![CDATA[present time]]></category>
		<category><![CDATA[richness]]></category>
		<category><![CDATA[selection effect]]></category>
		<category><![CDATA[sigma]]></category>
		<category><![CDATA[type galaxy]]></category>
		<category><![CDATA[vector]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/16/plain-fundamentals-of-fundamental-planes-analytics-and-algorithms/</guid>
		<description><![CDATA[The coefficients a and b of the Fundamental Plane relation R ~ Sigma^a I^b depend on whether one minimizes the scatter in the R direction or orthogonal to the Plane. We provide explicit expressions for a and b (and confidence limits) in terms of the covariances between logR, logSigma and logI. Our analysis is more [...]]]></description>
			<content:encoded><![CDATA[<p>The coefficients a and b of the Fundamental Plane relation R ~ Sigma^a I^b depend on whether one minimizes the scatter in the R direction or orthogonal to the Plane. We provide explicit expressions for a and b (and confidence limits) in terms of the covariances between logR, logSigma and logI. Our analysis is more generally applicable to any other correlations between three variables: e.g., the color-magnitude-Sigma relation, the L-Sigma-Mbh relation, or the relation between the X-ray luminosity, Sunyaev-Zeldovich decrement and optical richness of a cluster, so we provide IDL code which implements these ideas, and we show how our analysis generalizes further to correlations between more than three variables. We show how to account for correlated errors and selection effects, and quantify the difference between the direct, inverse and orthogonal fit coefficients. We show that the three vectors associated with the Fundamental Plane can all be written as simple combinations of a and b because the distribution of I is much broader than that of Sigma, and Sigma and I are only weakly correlated. Why this should be so for galaxies is a fundamental open question about the physics of early-type galaxy formation. If luminosity evolution is differential, and Rs and Sigmas do not evolve, then this is just an accident: Sigma and I must have been correlated in the past. On the other hand, if the (lack of) correlation is similar to that at the present time, then differential luminosity evolution must have been accompanied by structural evolution. A model in which the luminosities of low-L galaxies evolve more rapidly than do those of higher-L galaxies is able to produce the observed decrease in a (by a factor of 2 at z~1) while having b decrease by only about 20 percent. In such a model, the Mdyn/L ratio is a steeper function of Mdyn at higher z.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/16/plain-fundamentals-of-fundamental-planes-analytics-and-algorithms/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>The HBI in a quasi-global model of the intracluster medium</title>
		<link>http://voxcharta.org/2012/02/16/the-hbi-in-a-quasi-global-model-of-the-intracluster-medium/</link>
		<comments>http://voxcharta.org/2012/02/16/the-hbi-in-a-quasi-global-model-of-the-intracluster-medium/#comments</comments>
		<pubDate>Fri, 17 Feb 2012 01:51:39 +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[aim]]></category>
		<category><![CDATA[anisotropy]]></category>
		<category><![CDATA[buoyancy]]></category>
		<category><![CDATA[core]]></category>
		<category><![CDATA[galaxy cluster]]></category>
		<category><![CDATA[global model]]></category>
		<category><![CDATA[global structure]]></category>
		<category><![CDATA[hbi]]></category>
		<category><![CDATA[heat conduction]]></category>
		<category><![CDATA[heat flux]]></category>
		<category><![CDATA[intracluster medium]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[momentum]]></category>
		<category><![CDATA[morphology]]></category>
		<category><![CDATA[parallel atmosphere]]></category>
		<category><![CDATA[plasma]]></category>
		<category><![CDATA[radial profile]]></category>
		<category><![CDATA[temperature gradient]]></category>
		<category><![CDATA[temperature profile]]></category>
		<category><![CDATA[viscosity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/16/the-hbi-in-a-quasi-global-model-of-the-intracluster-medium/</guid>
		<description><![CDATA[In this paper we investigate how convective instabilities influence heat conduction in the intracluster medium (ICM) of cool-core galaxy clusters. The ICM is a high-beta, weakly collisional plasma in which the transport of momentum and heat is aligned with the magnetic field. The anisotropy of heat conduction, in particular, gives rise to instabilities that can [...]]]></description>
			<content:encoded><![CDATA[<p>In this paper we investigate how convective instabilities influence heat conduction in the intracluster medium (ICM) of cool-core galaxy clusters. The ICM is a high-beta, weakly collisional plasma in which the transport of momentum and heat is aligned with the magnetic field. The anisotropy of heat conduction, in particular, gives rise to instabilities that can access energy stored in a temperature gradient of either sign. We focus on the heat-flux buoyancy-driven instability (HBI), which feeds on the outwardly increasing temperature profile of cluster cool cores. Our aim is to elucidate how the global structure of a cluster impacts on the growth and morphology of the linear HBI modes when in the presence of Braginskii viscosity, and ultimately on the ability of the HBI to thermally insulate cores. We employ an idealised quasi-global model, the plane-parallel atmosphere, which captures the essential physics &#8212; e.g. the global radial profile of the cluster &#8212; while letting the problem remain analytically tractable. Our main result is that the dominant HBI modes are localised to the the innermost (~&lt;20%) regions of cool cores. It is then probable that, in the nonlinear regime, appreciable field-line insulation will be similarly localised. Thus, while radio-mode feedback appears necessary in the central few tens of kpc, heat conduction may be capable of offsetting radiative losses throughout most of a cool core over a significant fraction of the Hubble time. Finally, our linear solutions provide a convenient numerical test for the nonlinear codes that tackle the saturation of such convective instabilities in the presence of anisotropic transport.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/16/the-hbi-in-a-quasi-global-model-of-the-intracluster-medium/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Forming Early-Type Galaxies in LambdaCDM Simulations -I. Assembly histories</title>
		<link>http://voxcharta.org/2012/02/16/forming-early-type-galaxies-in-lambdacdm-simulations-i-assembly-histories/</link>
		<comments>http://voxcharta.org/2012/02/16/forming-early-type-galaxies-in-lambdacdm-simulations-i-assembly-histories/#comments</comments>
		<pubDate>Fri, 17 Feb 2012 01:51:03 +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[cosmological simulations]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[density profile]]></category>
		<category><![CDATA[driven wind]]></category>
		<category><![CDATA[formation mechanism]]></category>
		<category><![CDATA[galaxy population]]></category>
		<category><![CDATA[gas stream]]></category>
		<category><![CDATA[half mass]]></category>
		<category><![CDATA[initial condition]]></category>
		<category><![CDATA[initial growth]]></category>
		<category><![CDATA[massive galaxy]]></category>
		<category><![CDATA[phase formation]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[resolution simulation]]></category>
		<category><![CDATA[sni]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[stellar material]]></category>
		<category><![CDATA[type galaxy]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/16/forming-early-type-galaxies-in-lambdacdm-simulations-i-assembly-histories/</guid>
		<description><![CDATA[We present a sample of nine very high resolution cosmological simulations starting from LambdaCDM initial conditions. Our simulations include primordial radiative cooling, photoionization, star formation, supernova II feedback, but exclude supernova driven winds and AGN feedback. We confirm our earlier results with higher resolution simulations and demonstrate that the simulated galaxies assemble in two phases, [...]]]></description>
			<content:encoded><![CDATA[<p>We present a sample of nine very high resolution cosmological simulations starting from LambdaCDM initial conditions. Our simulations include primordial radiative cooling, photoionization, star formation, supernova II feedback, but exclude supernova driven winds and AGN feedback. We confirm our earlier results with higher resolution simulations and demonstrate that the simulated galaxies assemble in two phases, with the initial growth dominated by compact in situ star formation fueled by cold, low entropy gas streams, whereas the late growth is dominated by accretion of old stars formed in subunits outside the main galaxy. The two-phase formation mechanism naturally explains the observed downsizing, bimodality and size growth of the galaxy population. Very high resolution simulations show that gravitational feedback strongly suppresses late star formation in massive galaxies contributing to the observed galaxy color bimodality. However, additional heating sources probably in the form of AGN and SNI feedback are also required to prevent late gas inflows and associated residual star formation in the more massive galaxies. The accretion of stellar material (dry minor mergers) is also responsible for the observed size growth of early-type galaxies. Consistent with their assembly histories we find that the dark matter fractions within the stellar half-mass radii continuously increase towards lower redshift from about f_DM~0.05 at z~3 to f_DM~0.1-0.3 at z=0. In addition, the logarithmic slope of the total density profile is nearly isothermal at the present-day (gamma&#8217;~1.9-2.2) also in good agreement with recent lensing observations. Our simulations predict almost constant slopes until redshift z =1 and then steeper slopes of gamma~3 at higher redshifts. (Abridged)</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/16/forming-early-type-galaxies-in-lambdacdm-simulations-i-assembly-histories/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Buoyancy Instabilities in a Weakly Collisional Intracluster Medium</title>
		<link>http://voxcharta.org/2012/02/16/buoyancy-instabilities-in-a-weakly-collisional-intracluster-medium/</link>
		<comments>http://voxcharta.org/2012/02/16/buoyancy-instabilities-in-a-weakly-collisional-intracluster-medium/#comments</comments>
		<pubDate>Fri, 17 Feb 2012 01:50:46 +0000</pubDate>
		<dc:creator>astro-ph</
