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	<title>Vox Charta &#187; Instrumentation and Methods</title>
	<atom:link href="http://voxcharta.org/category/astro-ph/instrumentation-methods-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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			<item>
		<title>The Electron Capture Decay of 163-Ho to Measure the Electron Neutrino Mass with sub-eV Accuracy and Beyond [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/22/the-electron-capture-decay-of-163-ho-to-measure-the-electron-neutrino-mass-with-sub-ev-accuracy-and-beyond-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/22/the-electron-capture-decay-of-163-ho-to-measure-the-electron-neutrino-mass-with-sub-ev-accuracy-and-beyond-cross-listing/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 02:01:43 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accuracy]]></category>
		<category><![CDATA[decay]]></category>
		<category><![CDATA[electron neutrino]]></category>
		<category><![CDATA[roadmap]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/the-electron-capture-decay-of-163-ho-to-measure-the-electron-neutrino-mass-with-sub-ev-accuracy-and-beyond-cross-listing/</guid>
		<description><![CDATA[We have investigated the possibility of measuring the electron neutrino mass with sub-eV sensitivity by studying the electron capture decay of 163-Ho with cryogenic microcalorimeters. In this paper we will introduce an experiment&#8217;s concept, discuss the technical requirements, and identify a roadmap to reach a sensitivity of 0.1 eV and beyond.
]]></description>
			<content:encoded><![CDATA[<p>We have investigated the possibility of measuring the electron neutrino mass with sub-eV sensitivity by studying the electron capture decay of 163-Ho with cryogenic microcalorimeters. In this paper we will introduce an experiment&#8217;s concept, discuss the technical requirements, and identify a roadmap to reach a sensitivity of 0.1 eV and beyond.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/the-electron-capture-decay-of-163-ho-to-measure-the-electron-neutrino-mass-with-sub-ev-accuracy-and-beyond-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Space Astronomy for the mid-21st Century: Robotically Maintained Space Telescopes</title>
		<link>http://voxcharta.org/2012/02/22/space-astronomy-for-the-mid-21st-century-robotically-maintained-space-telescopes/</link>
		<comments>http://voxcharta.org/2012/02/22/space-astronomy-for-the-mid-21st-century-robotically-maintained-space-telescopes/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:49:48 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[21st century]]></category>
		<category><![CDATA[astronomical telescope]]></category>
		<category><![CDATA[autonomy]]></category>
		<category><![CDATA[capability]]></category>
		<category><![CDATA[decade]]></category>
		<category><![CDATA[lifetime]]></category>
		<category><![CDATA[mirror]]></category>
		<category><![CDATA[operational budget]]></category>
		<category><![CDATA[prerequisite]]></category>
		<category><![CDATA[robotic missions]]></category>
		<category><![CDATA[running costs]]></category>
		<category><![CDATA[scientific instrument]]></category>
		<category><![CDATA[space astronomy]]></category>
		<category><![CDATA[space telescope]]></category>
		<category><![CDATA[spacecraft components]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/space-astronomy-for-the-mid-21st-century-robotically-maintained-space-telescopes/</guid>
		<description><![CDATA[The historical development of ground based astronomical telescopes leads us to expect that space-based astronomical telescopes will need to be operational for many decades. The exchange of scientific instruments in space will be a prerequisite for the long lasting scientific success of such missions. Operationally, the possibility to repair or replace key spacecraft components in [...]]]></description>
			<content:encoded><![CDATA[<p>The historical development of ground based astronomical telescopes leads us to expect that space-based astronomical telescopes will need to be operational for many decades. The exchange of scientific instruments in space will be a prerequisite for the long lasting scientific success of such missions. Operationally, the possibility to repair or replace key spacecraft components in space will be mandatory. We argue that these requirements can be fulfilled with robotic missions and see the development of the required engineering as the main challenge. Ground based operations, scientifically and technically, will require a low operational budget of the running costs. These can be achieved through enhanced autonomy of the spacecraft and mission independent concepts for the support of the software. This concept can be applied to areas where the mirror capabilities do not constrain the lifetime of the mission.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/space-astronomy-for-the-mid-21st-century-robotically-maintained-space-telescopes/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>First Science Observations with SOFIA/FORCAST: The FORCAST Mid-infrared Camera</title>
		<link>http://voxcharta.org/2012/02/22/first-science-observations-with-sofiaforcast-the-forcast-mid-infrared-camera/</link>
		<comments>http://voxcharta.org/2012/02/22/first-science-observations-with-sofiaforcast-the-forcast-mid-infrared-camera/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:39:50 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[capability]]></category>
		<category><![CDATA[diffraction]]></category>
		<category><![CDATA[first science]]></category>
		<category><![CDATA[images]]></category>
		<category><![CDATA[infrared astronomy]]></category>
		<category><![CDATA[infrared camera]]></category>
		<category><![CDATA[infrared instrument]]></category>
		<category><![CDATA[Lambda]]></category>
		<category><![CDATA[light flight]]></category>
		<category><![CDATA[micron]]></category>
		<category><![CDATA[science flights]]></category>
		<category><![CDATA[science observations]]></category>
		<category><![CDATA[science results]]></category>
		<category><![CDATA[sofia]]></category>
		<category><![CDATA[stratospheric observatory]]></category>
		<category><![CDATA[unique science]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/first-science-observations-with-sofiaforcast-the-forcast-mid-infrared-camera/</guid>
		<description><![CDATA[The Stratospheric Observatory for Infrared Astronomy (SOFIA) completed its first light flight in May of 2010 using the facility mid-infrared instrument FORCAST. Since then, FORCAST has successfully completed thirteen science flights on SOFIA. In this paper we describe the design, operation and performance of FORCAST as it relates to the initial three Short Science flights. [...]]]></description>
			<content:encoded><![CDATA[<p>The Stratospheric Observatory for Infrared Astronomy (SOFIA) completed its first light flight in May of 2010 using the facility mid-infrared instrument FORCAST. Since then, FORCAST has successfully completed thirteen science flights on SOFIA. In this paper we describe the design, operation and performance of FORCAST as it relates to the initial three Short Science flights. FORCAST was able to achieve near diffraction-limited images for lambda &gt; 30 microns allowing unique science results from the start with SOFIA. We also describe ongoing and future modifications that will improve overall capabilities and performance of FORCAST.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/first-science-observations-with-sofiaforcast-the-forcast-mid-infrared-camera/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Citations to Australian Astronomy: 5 and 10 Year Benchmarks [Replacement]</title>
		<link>http://voxcharta.org/2012/02/22/citations-to-australian-astronomy-5-and-10-year-benchmarks-replacement-2/</link>
		<comments>http://voxcharta.org/2012/02/22/citations-to-australian-astronomy-5-and-10-year-benchmarks-replacement-2/#comments</comments>
		<pubDate>Thu, 23 Feb 2012 01:32:46 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astronomical society]]></category>
		<category><![CDATA[astrophysics data system]]></category>
		<category><![CDATA[australian astronomy]]></category>
		<category><![CDATA[australian universities]]></category>
		<category><![CDATA[benchmark]]></category>
		<category><![CDATA[career researchers]]></category>
		<category><![CDATA[citation]]></category>
		<category><![CDATA[citation count]]></category>
		<category><![CDATA[first decade]]></category>
		<category><![CDATA[hirsch]]></category>
		<category><![CDATA[histogram]]></category>
		<category><![CDATA[metrics]]></category>
		<category><![CDATA[nasa]]></category>
		<category><![CDATA[nasa astrophysics data]]></category>
		<category><![CDATA[nasa astrophysics data system]]></category>
		<category><![CDATA[observatory]]></category>
		<category><![CDATA[percentile]]></category>
		<category><![CDATA[professional astronomers]]></category>
		<category><![CDATA[research organisations]]></category>
		<category><![CDATA[web page]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/22/citations-to-australian-astronomy-5-and-10-year-benchmarks-replacement-2/</guid>
		<description><![CDATA[Expanding upon Pimbblet&#8217;s informative 2011 analysis of career h-indices for members of the Astronomical Society of Australia, we provide additional citation metrics which are geared to a) quantifying the current performance of b) all professional astronomers in Australia. We have trawled the staff web-pages of Australian Universities, Observatories and Research Organisations hosting professional astronomers, and [...]]]></description>
			<content:encoded><![CDATA[<p>Expanding upon Pimbblet&#8217;s informative 2011 analysis of career h-indices for members of the Astronomical Society of Australia, we provide additional citation metrics which are geared to a) quantifying the current performance of b) all professional astronomers in Australia. We have trawled the staff web-pages of Australian Universities, Observatories and Research Organisations hosting professional astronomers, and identified 383 PhD-qualified, research-active, astronomers in the nation &#8211; 131 of these are not members of the Astronomical Society of Australia. Using the SAO/NASA Astrophysics Data System, we provide the three following common metrics based on publications in the first decade of the 21st century (2001-2010): h-index, author-normalised citation count and lead-author citation count. We additionally present a somewhat more inclusive analysis, applicable for many early-career researchers, that is based on publications from 2006-2010. Histograms and percentiles, plus top-performer lists, are presented for each category. Finally, building on Hirsch&#8217;s empirical equation, we find that the (10-year) h-index and (10-year) total citation count T can be approximated by the relation h = (0.5+sqrt{T})/sqrt{5} for h &gt; 5.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/22/citations-to-australian-astronomy-5-and-10-year-benchmarks-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>First Science Observations with SOFIA/FORCAST: 6 to 37 micron Imaging of the Central Orion Nebula</title>
		<link>http://voxcharta.org/2012/02/21/first-science-observations-with-sofiaforcast-6-to-37-micron-imaging-of-the-central-orion-nebula/</link>
		<comments>http://voxcharta.org/2012/02/21/first-science-observations-with-sofiaforcast-6-to-37-micron-imaging-of-the-central-orion-nebula/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 02:03:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[airborne telescope]]></category>
		<category><![CDATA[first science]]></category>
		<category><![CDATA[infrared image]]></category>
		<category><![CDATA[micron]]></category>
		<category><![CDATA[orion nebula]]></category>
		<category><![CDATA[resolution observations]]></category>
		<category><![CDATA[science observations]]></category>
		<category><![CDATA[sofia]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/first-science-observations-with-sofiaforcast-6-to-37-micron-imaging-of-the-central-orion-nebula/</guid>
		<description><![CDATA[We present new mid-infrared images of the central region of the Orion Nebula using the newly commissioned SOFIA airborne telescope and its 5 &#8212; 40 micron camera FORCAST. The 37.1 micron images represent the highest resolution observations (&#60;4&#34;) ever obtained of this region at these wavelengths. After BN/KL (which is described in a separate letter [...]]]></description>
			<content:encoded><![CDATA[<p>We present new mid-infrared images of the central region of the Orion Nebula using the newly commissioned SOFIA airborne telescope and its 5 &#8212; 40 micron camera FORCAST. The 37.1 micron images represent the highest resolution observations (&lt;4&quot;) ever obtained of this region at these wavelengths. After BN/KL (which is described in a separate letter in this issue), the dominant source at all wavelengths except 37.1 micron is the Ney-Allen Nebula, a crescent-shaped extended source associated with theta 1D. The morphology of the Ney-Allen nebula in our images is consistent with the interpretation that it is ambient dust swept up by the stellar wind from theta 1D, as suggested by Smith et al. (2005). Our observations also reveal emission from two &quot;proplyds&quot; (proto-planetary disks), and a few embedded young stellar objects (YSOs; IRc9, and OMC1S IRS1, 2, and 10). The spectral energy distribution for IRc9 is presented and fitted with standard YSO models from Robitaille et al. (2007) to constrain the total luminosity, disk size, and envelope size. The diffuse, nebular emission we observe at all FORCAST wavelengths is most likely from the background photodissociation region (PDR) and shows structure that coincides roughly with H_alpha and [N II] emission. We conclude that the spatial variations in the diffuse emission are likely due to undulations in the surface of the background PDR.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/first-science-observations-with-sofiaforcast-6-to-37-micron-imaging-of-the-central-orion-nebula/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Compact continuum source-finding for next generation radio surveys</title>
		<link>http://voxcharta.org/2012/02/21/compact-continuum-source-finding-for-next-generation-radio-surveys/</link>
		<comments>http://voxcharta.org/2012/02/21/compact-continuum-source-finding-for-next-generation-radio-surveys/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:58:16 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[aegean]]></category>
		<category><![CDATA[algorithm]]></category>
		<category><![CDATA[blind radio]]></category>
		<category><![CDATA[completeness]]></category>
		<category><![CDATA[continuum source]]></category>
		<category><![CDATA[daily basis]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[generation radio]]></category>
		<category><![CDATA[kernel]]></category>
		<category><![CDATA[next generation]]></category>
		<category><![CDATA[radio astronomy]]></category>
		<category><![CDATA[radio source]]></category>
		<category><![CDATA[radio survey]]></category>
		<category><![CDATA[reliability]]></category>
		<category><![CDATA[source catalogue]]></category>
		<category><![CDATA[square kilometer array]]></category>
		<category><![CDATA[Telescope]]></category>
		<category><![CDATA[transients]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/compact-continuum-source-finding-for-next-generation-radio-surveys/</guid>
		<description><![CDATA[We present a detailed analysis of four of the most widely used radio source finding packages in radio astronomy, and a program being developed for the Australian Square Kilometer Array Pathfinder (ASKAP) telescope. The four packages; SExtractor, SFind, IMSAD and Selavy are shown to produce source catalogues with high completeness and reliability. In this paper [...]]]></description>
			<content:encoded><![CDATA[<p>We present a detailed analysis of four of the most widely used radio source finding packages in radio astronomy, and a program being developed for the Australian Square Kilometer Array Pathfinder (ASKAP) telescope. The four packages; SExtractor, SFind, IMSAD and Selavy are shown to produce source catalogues with high completeness and reliability. In this paper we analyse the small fraction (~1%) of cases in which these packages do not perform well. This small fraction of sources will be of concern for the next generation of radio surveys which will produce many thousands of sources on a daily basis, in particular for blind radio transients surveys. From our analysis we identify the ways in which the underlying source finding algorithms fail. We demonstrate a new source finding algorithm Aegean, based on the application of a Laplacian kernel, which can avoid these problems and can produce complete and reliable source catalogues for the next generation of radio surveys.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/compact-continuum-source-finding-for-next-generation-radio-surveys/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Distinguishing between a true period and its alias, and other tasks of model discrimination</title>
		<link>http://voxcharta.org/2012/02/21/distinguishing-between-a-true-period-and-its-alias-and-other-tasks-of-model-discrimination/</link>
		<comments>http://voxcharta.org/2012/02/21/distinguishing-between-a-true-period-and-its-alias-and-other-tasks-of-model-discrimination/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:49:56 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[alias]]></category>
		<category><![CDATA[ambiguity]]></category>
		<category><![CDATA[closeness]]></category>
		<category><![CDATA[extrasolar planetary system]]></category>
		<category><![CDATA[hasty conclusions]]></category>
		<category><![CDATA[information criterion]]></category>
		<category><![CDATA[model discrimination]]></category>
		<category><![CDATA[rival models]]></category>
		<category><![CDATA[time series data]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/distinguishing-between-a-true-period-and-its-alias-and-other-tasks-of-model-discrimination/</guid>
		<description><![CDATA[We consider the task of distinguishing between two different alternative models that can roughly equally explain observed time series data, mainly focusing on the period ambiguity case (aliasing). We propose a test for checking whether the rival models are observationally equivalent for now or they are already distinguishable. It is the Vuong closeness test, which [...]]]></description>
			<content:encoded><![CDATA[<p>We consider the task of distinguishing between two different alternative models that can roughly equally explain observed time series data, mainly focusing on the period ambiguity case (aliasing). We propose a test for checking whether the rival models are observationally equivalent for now or they are already distinguishable. It is the Vuong closeness test, which is based on the Kullback-Leibler Information Criterion. It is asymptotically normal and can work (in certain sense) even in the misspecified case, when the both proposed alternatives are actually wrong. This test is also very simple for practical use. We apply it to several known extrasolar planetary systems and find that our method often helps to resolve various model ambiguities emerging in astronomical practice, but preventing us from hasty conclusions in other cases.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/distinguishing-between-a-true-period-and-its-alias-and-other-tasks-of-model-discrimination/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Publication Trends in Astronomy: The Lone Author [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/21/publication-trends-in-astronomy-the-lone-author-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/21/publication-trends-in-astronomy-the-lone-author-cross-listing/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:47:50 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astronomy journals]]></category>
		<category><![CDATA[astrophysics data system]]></category>
		<category><![CDATA[author papers]]></category>
		<category><![CDATA[collaborators]]></category>
		<category><![CDATA[nasa]]></category>
		<category><![CDATA[nasa astrophysics data]]></category>
		<category><![CDATA[nasa astrophysics data system]]></category>
		<category><![CDATA[publication trends]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/publication-trends-in-astronomy-the-lone-author-cross-listing/</guid>
		<description><![CDATA[In this short communication I highlight how the number of collaborators on papers in the main astronomy journals has evolved over time. We see a trend of moving away from single-author papers. This communication is based on data in the holdings of the SAO/NASA Astrophysics Data System (ADS).   The ADS is funded by [...]]]></description>
			<content:encoded><![CDATA[<p>In this short communication I highlight how the number of collaborators on papers in the main astronomy journals has evolved over time. We see a trend of moving away from single-author papers. This communication is based on data in the holdings of the SAO/NASA Astrophysics Data System (ADS).   The ADS is funded by NASA Grant NNX09AB39G.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/publication-trends-in-astronomy-the-lone-author-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>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>Southern Africa CTA Site Proposal</title>
		<link>http://voxcharta.org/2012/02/21/southern-africa-cta-site-proposal/</link>
		<comments>http://voxcharta.org/2012/02/21/southern-africa-cta-site-proposal/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:41:21 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[background level]]></category>
		<category><![CDATA[cherenkov telescopes]]></category>
		<category><![CDATA[cloud coverage]]></category>
		<category><![CDATA[cloudless sky]]></category>
		<category><![CDATA[cta]]></category>
		<category><![CDATA[fiber line]]></category>
		<category><![CDATA[keetmanshoop]]></category>
		<category><![CDATA[luderitz]]></category>
		<category><![CDATA[maximum wind speeds]]></category>
		<category><![CDATA[namibia]]></category>
		<category><![CDATA[national airports]]></category>
		<category><![CDATA[night sky]]></category>
		<category><![CDATA[night time]]></category>
		<category><![CDATA[railway line]]></category>
		<category><![CDATA[sky background]]></category>
		<category><![CDATA[sky brightness]]></category>
		<category><![CDATA[southern africa]]></category>
		<category><![CDATA[sutherland]]></category>
		<category><![CDATA[Telescope]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/southern-africa-cta-site-proposal/</guid>
		<description><![CDATA[Southern Africa has some of the world&#8217;s best sites for air Cherenkov telescopes. South Africa has only one viable site, which is south of Sutherland and also close to the Southern African Large Telescope (SALT). This site has very good infrastructure and is easy to access, but only 47% of the night-time has a cloudless [...]]]></description>
			<content:encoded><![CDATA[<p>Southern Africa has some of the world&#8217;s best sites for air Cherenkov telescopes. South Africa has only one viable site, which is south of Sutherland and also close to the Southern African Large Telescope (SALT). This site has very good infrastructure and is easy to access, but only 47% of the night-time has a cloudless sky usable for observations.   Namibia, which already hosts the H.E.S.S telescope, has a number of potential sites with much less cloud coverage. The H.E.S.S. site is one of the highest of these sites at 1840 m a.s.l. with about 64% of the night-time cloudless. It also has very low night sky background levels and is relatively close (about 100 km) to Windhoek. Moving further away from Windhoek to the south, the cloud coverage and artificial night sky brightness becomes even less, with the site at Kuibis (between Keetmanshoop and Luderitz) at 1640 m a.s.l. having clear night skies 73% of the time. Even though this site seems remote (being 660 km from Windhoek by road), it is close to the national B4 highway, a railway line, a power line and an optical fiber line. It is also less than two hours drive away from a harbour and national airports. The Namibian sites also receive very little snow, if any, and the wind speeds are less than 50 km/h for more than 90% of the time with maximum wind speeds of around 100 km/h. Seismically the whole Southern African region is very stable.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/southern-africa-cta-site-proposal/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Probing eV-mass scale axions with a Micromegas detector in the CAST experiment [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/probing-ev-mass-scale-axions-with-a-micromegas-detector-in-the-cast-experiment-replacement/</link>
		<comments>http://voxcharta.org/2012/02/21/probing-ev-mass-scale-axions-with-a-micromegas-detector-in-the-cast-experiment-replacement/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:40:39 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[axion]]></category>
		<category><![CDATA[bore]]></category>
		<category><![CDATA[cern]]></category>
		<category><![CDATA[characterization]]></category>
		<category><![CDATA[coupling]]></category>
		<category><![CDATA[decommissioned]]></category>
		<category><![CDATA[dipole magnet]]></category>
		<category><![CDATA[hypothetical particle]]></category>
		<category><![CDATA[mass range]]></category>
		<category><![CDATA[mass scale]]></category>
		<category><![CDATA[possible solution]]></category>
		<category><![CDATA[solar telescope]]></category>
		<category><![CDATA[strong interaction]]></category>
		<category><![CDATA[Sun]]></category>
		<category><![CDATA[thesis]]></category>
		<category><![CDATA[working principle]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/probing-ev-mass-scale-axions-with-a-micromegas-detector-in-the-cast-experiment-replacement/</guid>
		<description><![CDATA[The CAST (CERN Axion Solar Telescope) experiment is searching for axions, an hypothetical particle that emerges as a possible solution to the well known CP violation problem in strong interactions. CAST is using a decommissioned LHC dipole magnet able to track the Sun as a possible source of solar axions, and to convert them to [...]]]></description>
			<content:encoded><![CDATA[<p>The CAST (CERN Axion Solar Telescope) experiment is searching for axions, an hypothetical particle that emerges as a possible solution to the well known CP violation problem in strong interactions. CAST is using a decommissioned LHC dipole magnet able to track the Sun as a possible source of solar axions, and to convert them to X-rays photons detectable with low background X-ray detectors. CAST continues its data taking period scanning masses up to 1eV. This thesis presents the data obtained with a Micromegas detector for the scanned axion mass range up to 0.64eV. The working principle, characterization and analysis of the Micromegas detectors operating in CAST are detailed in this work. Moreover, the last detector data corresponding to the new data taking period, with 3He gas inside the bores, was used to obtain a preliminar and conservative upper limit on the axion-photon coupling for the new axion mass range explored, g_{a\gamma} &lt; 2.44 10^{-10} GeV^{-1}.</p>
]]></content:encoded>
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		<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>Citations to Australian Astronomy: 5 and 10 Year Benchmarks [Replacement]</title>
		<link>http://voxcharta.org/2012/02/21/citations-to-australian-astronomy-5-and-10-year-benchmarks-replacement/</link>
		<comments>http://voxcharta.org/2012/02/21/citations-to-australian-astronomy-5-and-10-year-benchmarks-replacement/#comments</comments>
		<pubDate>Wed, 22 Feb 2012 01:33:13 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astronomical society]]></category>
		<category><![CDATA[astrophysics data system]]></category>
		<category><![CDATA[australian astronomy]]></category>
		<category><![CDATA[australian universities]]></category>
		<category><![CDATA[benchmark]]></category>
		<category><![CDATA[career researchers]]></category>
		<category><![CDATA[citation]]></category>
		<category><![CDATA[citation count]]></category>
		<category><![CDATA[first decade]]></category>
		<category><![CDATA[hirsch]]></category>
		<category><![CDATA[histogram]]></category>
		<category><![CDATA[metrics]]></category>
		<category><![CDATA[nasa]]></category>
		<category><![CDATA[nasa astrophysics data]]></category>
		<category><![CDATA[nasa astrophysics data system]]></category>
		<category><![CDATA[observatory]]></category>
		<category><![CDATA[percentile]]></category>
		<category><![CDATA[professional astronomers]]></category>
		<category><![CDATA[research organisations]]></category>
		<category><![CDATA[web page]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/21/citations-to-australian-astronomy-5-and-10-year-benchmarks-replacement/</guid>
		<description><![CDATA[Expanding upon Pimbblet&#8217;s informative 2011 analysis of career h-indices for members of the Astronomical Society of Australia, we provide additional citation metrics which are geared to a) quantifying the current performance of b) all professional astronomers in Australia. We have trawled the staff web-pages of Australian Universities, Observatories and Research Organisations hosting professional astronomers, and [...]]]></description>
			<content:encoded><![CDATA[<p>Expanding upon Pimbblet&#8217;s informative 2011 analysis of career h-indices for members of the Astronomical Society of Australia, we provide additional citation metrics which are geared to a) quantifying the current performance of b) all professional astronomers in Australia. We have trawled the staff web-pages of Australian Universities, Observatories and Research Organisations hosting professional astronomers, and identified 383 PhD-qualified, research-active, astronomers in the nation &#8211; 131 of these are not members of the Astronomical Society of Australia. Using the SAO/NASA Astrophysics Data System, we provide the three following common metrics based on publications in the first decade of the 21st century (2001-2010): h-index, author-normalised citation count and lead-author citation count. We additionally present a somewhat more inclusive analysis, applicable for many early-career researchers, that is based on publications from 2006-2010. Histograms and percentiles, plus top-performer lists, are presented for each category. Finally, building on Hirsch&#8217;s empirical equation, we find that the (10-year) h-index and (10-year) total citation count T can be approximated by the relation h = (0.5+sqrt{T})/sqrt{5} for h &gt; 5.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/21/citations-to-australian-astronomy-5-and-10-year-benchmarks-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>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Citations to Australian Astronomy: 5 and 10 Year Benchmarks</title>
		<link>http://voxcharta.org/2012/02/20/citations-to-australian-astronomy-5-and-10-year-benchmarks/</link>
		<comments>http://voxcharta.org/2012/02/20/citations-to-australian-astronomy-5-and-10-year-benchmarks/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 02:05:42 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astronomical society]]></category>
		<category><![CDATA[astrophysics data system]]></category>
		<category><![CDATA[australian astronomy]]></category>
		<category><![CDATA[australian universities]]></category>
		<category><![CDATA[benchmark]]></category>
		<category><![CDATA[career researchers]]></category>
		<category><![CDATA[citation]]></category>
		<category><![CDATA[citation count]]></category>
		<category><![CDATA[first decade]]></category>
		<category><![CDATA[hirsch]]></category>
		<category><![CDATA[histogram]]></category>
		<category><![CDATA[metrics]]></category>
		<category><![CDATA[nasa]]></category>
		<category><![CDATA[nasa astrophysics data]]></category>
		<category><![CDATA[nasa astrophysics data system]]></category>
		<category><![CDATA[observatory]]></category>
		<category><![CDATA[percentile]]></category>
		<category><![CDATA[professional astronomers]]></category>
		<category><![CDATA[research organisations]]></category>
		<category><![CDATA[web page]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/citations-to-australian-astronomy-5-and-10-year-benchmarks/</guid>
		<description><![CDATA[Expanding upon Pimbblet&#8217;s informative 2011 analysis of career h-indices for members of the Astronomical Society of Australia, we provide additional citation metrics which are geared to a) quantifying the current performance of b) all professional astronomers in Australia. We have trawled the staff web-pages of Australian Universities, Observatories and Research Organisations hosting professional astronomers, and [...]]]></description>
			<content:encoded><![CDATA[<p>Expanding upon Pimbblet&#8217;s informative 2011 analysis of career h-indices for members of the Astronomical Society of Australia, we provide additional citation metrics which are geared to a) quantifying the current performance of b) all professional astronomers in Australia. We have trawled the staff web-pages of Australian Universities, Observatories and Research Organisations hosting professional astronomers, and identified 383 PhD-qualified, research-active, astronomers in the nation &#8211; 131 of these are not members of the Astronomical Society of Australia. Using the SAO/NASA Astrophysics Data System, we provide the three following common metrics based on publications in the first decade of the 21st century (2001-2010): h-index, author-normalised citation count and lead-author citation count. We additionally present a somewhat more inclusive analysis, applicable for many early-career researchers, that is based on publications from 2006&#8211;2010. Histograms and percentiles, plus top-performer lists, are presented for each category. Finally, building on Hirsch&#8217;s empirical equation, we find that the (10-year) h-index and total citation count T can be approximated by the relation h = (0.5+\sqrt{T})/\sqrt{5} for h &gt; 5.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/citations-to-australian-astronomy-5-and-10-year-benchmarks/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>No role for muons in the DAMA annual modulation results</title>
		<link>http://voxcharta.org/2012/02/20/no-role-for-muons-in-the-dama-annual-modulation-results/</link>
		<comments>http://voxcharta.org/2012/02/20/no-role-for-muons-in-the-dama-annual-modulation-results/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 02:02:03 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[collaboration]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[gran sasso]]></category>
		<category><![CDATA[long time]]></category>
		<category><![CDATA[modulation signature]]></category>
		<category><![CDATA[muon]]></category>
		<category><![CDATA[nai]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/no-role-for-muons-in-the-dama-annual-modulation-results/</guid>
		<description><![CDATA[Since long time it has been pointed out by the DAMA collaboration that muons surviving the Gran Sasso mountain cannot mimic the Dark Matter annual modulation signature exploited by the DAMA/NaI and DAMA/LIBRA experiments. In the present paper, these and further arguments are gathered together in order to enable a wider community to suitably approach [...]]]></description>
			<content:encoded><![CDATA[<p>Since long time it has been pointed out by the DAMA collaboration that muons surviving the Gran Sasso mountain cannot mimic the Dark Matter annual modulation signature exploited by the DAMA/NaI and DAMA/LIBRA experiments. In the present paper, these and further arguments are gathered together in order to enable a wider community to suitably approach this point.</p>
]]></content:encoded>
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		<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>The GREGOR solar telescope on Tenerife</title>
		<link>http://voxcharta.org/2012/02/20/the-gregor-solar-telescope-on-tenerife/</link>
		<comments>http://voxcharta.org/2012/02/20/the-gregor-solar-telescope-on-tenerife/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:52:13 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[adaptive optics]]></category>
		<category><![CDATA[focal plane instrument]]></category>
		<category><![CDATA[instrumentation]]></category>
		<category><![CDATA[light configuration]]></category>
		<category><![CDATA[mirror]]></category>
		<category><![CDATA[science goal]]></category>
		<category><![CDATA[solar telescope]]></category>
		<category><![CDATA[tenerife]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/the-gregor-solar-telescope-on-tenerife/</guid>
		<description><![CDATA[2011 was a successful year for the GREGOR project. The telescope was finally completed in May with the installation of the 1.5-meter primary mirror. The installation of the first-light focal plane instruments was completed by the end of the year. At the same time, the preparations for the installation of the high-order adaptive optics were [...]]]></description>
			<content:encoded><![CDATA[<p>2011 was a successful year for the GREGOR project. The telescope was finally completed in May with the installation of the 1.5-meter primary mirror. The installation of the first-light focal plane instruments was completed by the end of the year. At the same time, the preparations for the installation of the high-order adaptive optics were finished, its integration to the telescope is scheduled for early 2012. This paper describes the telescope and its instrumentation in their present first light configuration, and provides a brief overview of the science goals of GREGOR.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/the-gregor-solar-telescope-on-tenerife/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Electromagnetic follow-up of gravitational wave transient signal candidates</title>
		<link>http://voxcharta.org/2012/02/20/electromagnetic-follow-up-of-gravitational-wave-transient-signal-candidates/</link>
		<comments>http://voxcharta.org/2012/02/20/electromagnetic-follow-up-of-gravitational-wave-transient-signal-candidates/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:44:30 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astronomy]]></category>
		<category><![CDATA[background events]]></category>
		<category><![CDATA[counterpart]]></category>
		<category><![CDATA[gravitational wave detector]]></category>
		<category><![CDATA[image analysis]]></category>
		<category><![CDATA[ligo]]></category>
		<category><![CDATA[multi messenger]]></category>
		<category><![CDATA[observation study]]></category>
		<category><![CDATA[radio wavelength]]></category>
		<category><![CDATA[sky]]></category>
		<category><![CDATA[wave event]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/electromagnetic-follow-up-of-gravitational-wave-transient-signal-candidates/</guid>
		<description><![CDATA[Pioneering efforts aiming at the development of multi-messenger gravitational wave and electromagnetic astronomy have been made. An electromagnetic observation follow-up program of candidate gravitational wave events has been performed (Dec 17 2009 to Jan 8 2010 and Sep 4 to Oct 20 2010) during the recent runs of the LIGO and Virgo gravitational wave detectors. [...]]]></description>
			<content:encoded><![CDATA[<p>Pioneering efforts aiming at the development of multi-messenger gravitational wave and electromagnetic astronomy have been made. An electromagnetic observation follow-up program of candidate gravitational wave events has been performed (Dec 17 2009 to Jan 8 2010 and Sep 4 to Oct 20 2010) during the recent runs of the LIGO and Virgo gravitational wave detectors. It involved ground-based and space electromagnetic facilities observing the sky at optical, X-ray and radio wavelengths. The joint gravitational wave and electromagnetic observation study requires the development of specific image analysis procedures able to discriminate the possible electromagnetic counterpart of gravitational wave triggers from contaminant/background events. The paper presents an overview of the electromagnetic follow-up program and the image analysis procedures.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/electromagnetic-follow-up-of-gravitational-wave-transient-signal-candidates/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>The European Southern Observatory and VLT Telescopes on Paranal [Replacement]</title>
		<link>http://voxcharta.org/2012/02/20/the-european-southern-observatory-and-vlt-telescopes-on-paranal-replacement/</link>
		<comments>http://voxcharta.org/2012/02/20/the-european-southern-observatory-and-vlt-telescopes-on-paranal-replacement/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:32:44 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cerro paranal]]></category>
		<category><![CDATA[european southern observatory]]></category>
		<category><![CDATA[overview lecture]]></category>
		<category><![CDATA[perspective]]></category>
		<category><![CDATA[southern observatory eso]]></category>
		<category><![CDATA[Telescope]]></category>
		<category><![CDATA[vlt telescope]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/the-european-southern-observatory-and-vlt-telescopes-on-paranal-replacement/</guid>
		<description><![CDATA[The Very Large Telescope (VLT) of the European Southern Observatory (ESO) on Cerro Paranal is one of the most influential observing complexes in the world. In this overview lecture, an introduction to the ESO organization and VLT telescopes is presented, along with a small selection of scientific works. Particular attention is given to the importance [...]]]></description>
			<content:encoded><![CDATA[<p>The Very Large Telescope (VLT) of the European Southern Observatory (ESO) on Cerro Paranal is one of the most influential observing complexes in the world. In this overview lecture, an introduction to the ESO organization and VLT telescopes is presented, along with a small selection of scientific works. Particular attention is given to the importance of the VLT for the Russian scientific community, as well as to present and future perspectives for making use of ESO and VLT data.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/the-european-southern-observatory-and-vlt-telescopes-on-paranal-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>First Successful Adaptive Optics PSF Reconstruction at W. M. Keck Observatory [Replacement]</title>
		<link>http://voxcharta.org/2012/02/20/first-successful-adaptive-optics-psf-reconstruction-at-w-m-keck-observatory-replacement/</link>
		<comments>http://voxcharta.org/2012/02/20/first-successful-adaptive-optics-psf-reconstruction-at-w-m-keck-observatory-replacement/#comments</comments>
		<pubDate>Tue, 21 Feb 2012 01:32:14 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[aberration]]></category>
		<category><![CDATA[accuracy]]></category>
		<category><![CDATA[adaptive optics]]></category>
		<category><![CDATA[ao system]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[critical aspect]]></category>
		<category><![CDATA[gemini north]]></category>
		<category><![CDATA[guide star]]></category>
		<category><![CDATA[initial test]]></category>
		<category><![CDATA[keck ii]]></category>
		<category><![CDATA[keck observatory]]></category>
		<category><![CDATA[observation campaign]]></category>
		<category><![CDATA[optical turbulence]]></category>
		<category><![CDATA[phase diversity]]></category>
		<category><![CDATA[r project]]></category>
		<category><![CDATA[reconstruction]]></category>
		<category><![CDATA[sky]]></category>
		<category><![CDATA[stationarity]]></category>
		<category><![CDATA[turbulence parameters]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/20/first-successful-adaptive-optics-psf-reconstruction-at-w-m-keck-observatory-replacement/</guid>
		<description><![CDATA[We present the last results of our PSF reconstruction (PSF-R) project for the Keck-II and Gemini-North AO systems in natural guide star mode. Our initial tests have shown that the most critical aspects of PSF-R are the determination of the system static aberrations and the optical turbulence parameters, and we have set up a specific [...]]]></description>
			<content:encoded><![CDATA[<p>We present the last results of our PSF reconstruction (PSF-R) project for the Keck-II and Gemini-North AO systems in natural guide star mode. Our initial tests have shown that the most critical aspects of PSF-R are the determination of the system static aberrations and the optical turbulence parameters, and we have set up a specific observation campaign on the two systems to explore this. We demonstrate that deformable mirror based seeing monitor works well, and 10% accuracy is easily obtained. Phase diversity has been demonstrated to work on sky sources. Besides, residual phase stationarity is an important assumption in PSF-R, and we demonstrate here that it is basically true. As a result of these tests and verifications, we have been able for the first time to obtain a very good PSF reconstruction for the Keck-II system, in bright natural guide star mode.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/20/first-successful-adaptive-optics-psf-reconstruction-at-w-m-keck-observatory-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<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>
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		<item>
		<title>High Frame-rate Imaging Based Photometry, Photometric Reduction of Data from Electron-multiplying Charge Coupled Devices (EMCCDs)</title>
		<link>http://voxcharta.org/2012/02/19/high-frame-rate-imaging-based-photometry-photometric-reduction-of-data-from-electron-multiplying-charge-coupled-devices-emccds/</link>
		<comments>http://voxcharta.org/2012/02/19/high-frame-rate-imaging-based-photometry-photometric-reduction-of-data-from-electron-multiplying-charge-coupled-devices-emccds/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:48:49 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[algorithm]]></category>
		<category><![CDATA[amplification]]></category>
		<category><![CDATA[bia]]></category>
		<category><![CDATA[conventional ccd]]></category>
		<category><![CDATA[electron]]></category>
		<category><![CDATA[emccd]]></category>
		<category><![CDATA[expectation maximization]]></category>
		<category><![CDATA[faint star]]></category>
		<category><![CDATA[frame rate]]></category>
		<category><![CDATA[galactic bulge]]></category>
		<category><![CDATA[gravitational microlensing]]></category>
		<category><![CDATA[main sequence star]]></category>
		<category><![CDATA[phenomena]]></category>
		<category><![CDATA[prerequisite]]></category>
		<category><![CDATA[probabilistic model]]></category>
		<category><![CDATA[rate applications]]></category>
		<category><![CDATA[readout noise]]></category>
		<category><![CDATA[reduction steps]]></category>
		<category><![CDATA[spurious charges]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/high-frame-rate-imaging-based-photometry-photometric-reduction-of-data-from-electron-multiplying-charge-coupled-devices-emccds/</guid>
		<description><![CDATA[The EMCCD is a type of CCD that delivers fast readout times and negligible readout noise, making it an ideal detector for high frame rate applications which improve resolution, like lucky imaging or shift-and-add. This improvement in resolution can potentially improve the photometry of faint stars in extremely crowded fields significantly by alleviating crowding. This [...]]]></description>
			<content:encoded><![CDATA[<p>The EMCCD is a type of CCD that delivers fast readout times and negligible readout noise, making it an ideal detector for high frame rate applications which improve resolution, like lucky imaging or shift-and-add. This improvement in resolution can potentially improve the photometry of faint stars in extremely crowded fields significantly by alleviating crowding. This improvement in resolution is a prerequisite for observing gravitational microlensing in main sequence stars towards the galactic bulge. However, the photometric stability of this device has not been assessed. The EMCCD has sources of noise not found in conventional CCDs, and new methods for photometric reduction must be developed. We aim to investigate how the normal photometric reduction steps from conventional CCDs should be adjusted to be applicable to EMCCD data. One complication is that a bias frame cannot be obtained conventionally, as the output from an EMCCD is not normally distributed. Also, the readout process generates spurious charges in any CCD, but in EMCCD data, these charges are visible as opposed to the conventional CCD. A simple probabilistic model for the dark output of an EMCCD is developed. Fitting this model with the expectation-maximization algorithm allows us to estimate the bias, readout noise, amplification, and spurious charge rate per pixel and thus correct for these phenomena. To investigate the stability of the photometry, corrected frames of a crowded field are reduced with a PSF fitting photometry package. We find that it is possible to develop an algorithm that elegantly reduces EMCCD data and produces stable photometry at the 1% level in an extremely crowded field.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/high-frame-rate-imaging-based-photometry-photometric-reduction-of-data-from-electron-multiplying-charge-coupled-devices-emccds/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<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>
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		<item>
		<title>Gone with the Wind ON_Mars (GOWON): A Wind-Driven Networked System of Mobile Sensors on Mars [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/19/gone-with-the-wind-on_mars-gowon-a-wind-driven-networked-system-of-mobile-sensors-on-mars-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/19/gone-with-the-wind-on_mars-gowon-a-wind-driven-networked-system-of-mobile-sensors-on-mars-cross-listing/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:47:17 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[chemistry labs]]></category>
		<category><![CDATA[dust storm]]></category>
		<category><![CDATA[energy technologies]]></category>
		<category><![CDATA[exploration mission]]></category>
		<category><![CDATA[ferromagnetic minerals]]></category>
		<category><![CDATA[gone with the wind]]></category>
		<category><![CDATA[gowon]]></category>
		<category><![CDATA[integrated circuits]]></category>
		<category><![CDATA[mars missions]]></category>
		<category><![CDATA[maximum speed]]></category>
		<category><![CDATA[micro electro mechanical systems]]></category>
		<category><![CDATA[minerals and rocks]]></category>
		<category><![CDATA[miniature cameras]]></category>
		<category><![CDATA[missions to mars]]></category>
		<category><![CDATA[mobile sensors]]></category>
		<category><![CDATA[natural characteristics]]></category>
		<category><![CDATA[proposed system]]></category>
		<category><![CDATA[saltation]]></category>
		<category><![CDATA[scalable architecture]]></category>
		<category><![CDATA[wet chemistry]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/gone-with-the-wind-on_mars-gowon-a-wind-driven-networked-system-of-mobile-sensors-on-mars-cross-listing/</guid>
		<description><![CDATA[We propose a revolutionary way of studying the surface of Mars using a wind-driven network of mobile sensors- Gone with the Wind ON_Mars (GOWON). GOWON is a scalable architecture that will allow in-situ mapping of a wide range of phenomena, exploiting existing capabilities, but radically improving our ability to study Mars. GOWON has the following [...]]]></description>
			<content:encoded><![CDATA[<p>We propose a revolutionary way of studying the surface of Mars using a wind-driven network of mobile sensors- Gone with the Wind ON_Mars (GOWON). GOWON is a scalable architecture that will allow in-situ mapping of a wide range of phenomena, exploiting existing capabilities, but radically improving our ability to study Mars. GOWON has the following characteristics: 1.it consists of a dynamic wireless network of many compact mobile sensors. 2.the mobile sensors (called moballs) are spherically-shaped and wind-driven; they are lightweight and bouncy. 3. moballs communicate with each other and earth through a satellite system orbiting Mars. There is also peer-to-peer communication between the moballs, creating a network of shared data, computing, and tasks.   Motivation and Rationale Thanks to earlier exploration missions to Mars we now have a much better understanding of many of the natural characteristics of the red planet. We now know that there is an abundance of wind (with average speeds of 10 m/s and much higher maximum speeds [1]), dust storms, high levels of saltation [2], crustal magnetic fields generated by an abundance of ferromagnetic minerals and rocks [3], etc. Future Mars missions must therefore attempt to leverage these characteristics, and must do so by exploiting recent advances in low power micro-devices using MEMS (Micro-Electro-Mechanical Systems that harvest vibration and other movement into energy) technologies and others, miniature cameras, miniature wet chemistry labs, integrated circuits, low power wireless devices, etc. We believe the system proposed here addresses this opportunity heads on. Our proposed system is much more than a collection of sensors; the system is larger than the sum of its parts. In addition to communicating with the satellite, the moballs can communicate with each other and therefore distribute tasks, data, computations, etc.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
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		<item>
		<title>The Positioning System of the ANTARES Neutrino Telescope</title>
		<link>http://voxcharta.org/2012/02/19/the-positioning-system-of-the-antares-neutrino-telescope/</link>
		<comments>http://voxcharta.org/2012/02/19/the-positioning-system-of-the-antares-neutrino-telescope/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:45:17 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[antares]]></category>
		<category><![CDATA[compass]]></category>
		<category><![CDATA[detector alignment]]></category>
		<category><![CDATA[flexible structure]]></category>
		<category><![CDATA[inclination]]></category>
		<category><![CDATA[mediterranean sea]]></category>
		<category><![CDATA[mooring]]></category>
		<category><![CDATA[necessary corrections]]></category>
		<category><![CDATA[neutrino interaction]]></category>
		<category><![CDATA[neutrino telescope]]></category>
		<category><![CDATA[optical module]]></category>
		<category><![CDATA[orientation]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[positioning system]]></category>
		<category><![CDATA[reconstruction]]></category>
		<category><![CDATA[sea bed]]></category>
		<category><![CDATA[sea currents]]></category>
		<category><![CDATA[secondary particles]]></category>
		<category><![CDATA[toulon]]></category>
		<category><![CDATA[triangulation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/the-positioning-system-of-the-antares-neutrino-telescope/</guid>
		<description><![CDATA[The ANTARES neutrino telescope, located 40km off the coast of Toulon in the Mediterranean Sea at a mooring depth of about 2475m, consists of twelve detection lines equipped typically with 25 storeys. Every storey carries three optical modules that detect Cherenkov light induced by charged secondary particles (typically muons) coming from neutrino interactions. As these [...]]]></description>
			<content:encoded><![CDATA[<p>The ANTARES neutrino telescope, located 40km off the coast of Toulon in the Mediterranean Sea at a mooring depth of about 2475m, consists of twelve detection lines equipped typically with 25 storeys. Every storey carries three optical modules that detect Cherenkov light induced by charged secondary particles (typically muons) coming from neutrino interactions. As these lines are flexible structures fixed to the sea bed and held taut by a buoy, sea currents cause the lines to move and the storeys to rotate. The knowledge of the position of the optical modules with a precision better than 10cm is essential for a good reconstruction of particle tracks. In this paper the ANTARES positioning system is described. It consists of an acoustic positioning system, for distance triangulation, and a compass-tiltmeter system, for the measurement of the orientation and inclination of the storeys. Necessary corrections are discussed and the results of the detector alignment procedure are described.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/the-positioning-system-of-the-antares-neutrino-telescope/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A Bayesian Approach to Calibrating Period-Luminosity Relations of RR Lyrae Stars in the Mid-Infrared</title>
		<link>http://voxcharta.org/2012/02/19/a-bayesian-approach-to-calibrating-period-luminosity-relations-of-rr-lyrae-stars-in-the-mid-infrared/</link>
		<comments>http://voxcharta.org/2012/02/19/a-bayesian-approach-to-calibrating-period-luminosity-relations-of-rr-lyrae-stars-in-the-mid-infrared/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:43:32 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[applicability]]></category>
		<category><![CDATA[bayesian approach]]></category>
		<category><![CDATA[detailed description]]></category>
		<category><![CDATA[distance]]></category>
		<category><![CDATA[distributions]]></category>
		<category><![CDATA[example application]]></category>
		<category><![CDATA[hubble space telescope]]></category>
		<category><![CDATA[investigations]]></category>
		<category><![CDATA[least square]]></category>
		<category><![CDATA[linear model]]></category>
		<category><![CDATA[methodology]]></category>
		<category><![CDATA[model parameter]]></category>
		<category><![CDATA[rr lyrae stars]]></category>
		<category><![CDATA[substantial benefit]]></category>
		<category><![CDATA[variable star]]></category>
		<category><![CDATA[vindication]]></category>
		<category><![CDATA[waveband]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/a-bayesian-approach-to-calibrating-period-luminosity-relations-of-rr-lyrae-stars-in-the-mid-infrared/</guid>
		<description><![CDATA[A Bayesian approach to calibrating period-luminosity (PL) relations has substantial benefits over generic least-squares fits. In particular, the Bayesian approach takes into account the full prior distribution of the model parameters, such as the a priori distances, and refits these parameters as part of the process of settling on the most highly-constrained final fit. Additionally, [...]]]></description>
			<content:encoded><![CDATA[<p>A Bayesian approach to calibrating period-luminosity (PL) relations has substantial benefits over generic least-squares fits. In particular, the Bayesian approach takes into account the full prior distribution of the model parameters, such as the a priori distances, and refits these parameters as part of the process of settling on the most highly-constrained final fit. Additionally, the Bayesian approach can naturally ingest data from multiple wavebands and simultaneously fit the parameters of PL relations for each waveband in a procedure that constrains the parameter posterior distributions so as to minimize the scatter of the final fits appropriately in all wavebands. Here we describe the generalized approach to Bayesian model fitting and then specialize to a detailed description of applying Bayesian linear model fitting to the mid-infrared PL relations of RR Lyrae variable stars. For this example application we quantify the improvement afforded by using a Bayesian model fit. We also compare distances previously predicted in our example application to recently published parallax distances measured with the Hubble Space Telescope and find their agreement to be a vindication of our methodology. Our intent with this article is to spread awareness of the benefits and applicability of this Bayesian approach and encourage future PL relation investigations to consider employing this powerful analysis method.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/a-bayesian-approach-to-calibrating-period-luminosity-relations-of-rr-lyrae-stars-in-the-mid-infrared/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Measurement of Solar Diameter and Limb Darkening Function with the Eclipse Observations [Replacement]</title>
		<link>http://voxcharta.org/2012/02/19/the-measurement-of-solar-diameter-and-limb-darkening-function-with-the-eclipse-observations-replacement/</link>
		<comments>http://voxcharta.org/2012/02/19/the-measurement-of-solar-diameter-and-limb-darkening-function-with-the-eclipse-observations-replacement/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:38:23 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[11 years]]></category>
		<category><![CDATA[15 january]]></category>
		<category><![CDATA[arcsec]]></category>
		<category><![CDATA[astrometry]]></category>
		<category><![CDATA[baily]]></category>
		<category><![CDATA[drift scan]]></category>
		<category><![CDATA[eclipse]]></category>
		<category><![CDATA[evaluations]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[inflection point]]></category>
		<category><![CDATA[lunar limb]]></category>
		<category><![CDATA[Measurement]]></category>
		<category><![CDATA[naked eye]]></category>
		<category><![CDATA[satellite data]]></category>
		<category><![CDATA[solar cycle]]></category>
		<category><![CDATA[solar diameter]]></category>
		<category><![CDATA[total solar irradiance]]></category>
		<category><![CDATA[variation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/the-measurement-of-solar-diameter-and-limb-darkening-function-with-the-eclipse-observations-replacement/</guid>
		<description><![CDATA[The Total Solar Irradiance varies over a solar cycle of 11 years and maybe over cycles with longer period. Is the solar diameter variable over time too? We introduce a new method to perform high resolution astrometry of the solar diameter from the ground, through the observations of eclipses by reconsidering the definition of the [...]]]></description>
			<content:encoded><![CDATA[<p>The Total Solar Irradiance varies over a solar cycle of 11 years and maybe over cycles with longer period. Is the solar diameter variable over time too? We introduce a new method to perform high resolution astrometry of the solar diameter from the ground, through the observations of eclipses by reconsidering the definition of the solar edge. A discussion of the solar diameter and its variations must be linked to the Limb Darkening Function (LDF) using the luminosity evolution of a Baily&#8217;s Bead and the profile of the lunar limb available from satellite data. This approach unifies the definition of solar edge with LDF inflection point for eclipses and drift-scan or heliometric methods. The method proposed is applied for the videos of the eclipse in 15 January 2010 recorded in Uganda and in India. The result shows light at least 0.85 arcsec beyond the inflection point, and this suggests to reconsider the evaluations of the historical eclipses made with naked eye.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/the-measurement-of-solar-diameter-and-limb-darkening-function-with-the-eclipse-observations-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>BAMBI: blind accelerated multimodal Bayesian inference [Replacement]</title>
		<link>http://voxcharta.org/2012/02/19/bambi-blind-accelerated-multimodal-bayesian-inference-replacement/</link>
		<comments>http://voxcharta.org/2012/02/19/bambi-blind-accelerated-multimodal-bayesian-inference-replacement/#comments</comments>
		<pubDate>Mon, 20 Feb 2012 01:37:59 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[algorithm]]></category>
		<category><![CDATA[approximation]]></category>
		<category><![CDATA[artificial neural network]]></category>
		<category><![CDATA[bambi]]></category>
		<category><![CDATA[bayesian analysis]]></category>
		<category><![CDATA[combinations]]></category>
		<category><![CDATA[cosmological parameters]]></category>
		<category><![CDATA[inference]]></category>
		<category><![CDATA[likelihood function]]></category>
		<category><![CDATA[microwave anisotropy probe]]></category>
		<category><![CDATA[nns]]></category>
		<category><![CDATA[priors]]></category>
		<category><![CDATA[running time]]></category>
		<category><![CDATA[sampling]]></category>
		<category><![CDATA[speed increases]]></category>
		<category><![CDATA[surface]]></category>
		<category><![CDATA[wilkinson microwave anisotropy]]></category>
		<category><![CDATA[wilkinson microwave anisotropy probe]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/19/bambi-blind-accelerated-multimodal-bayesian-inference-replacement/</guid>
		<description><![CDATA[In this paper we present an algorithm for rapid Bayesian analysis that combines the benefits of nested sampling and artificial neural networks. The blind accelerated multimodal Bayesian inference (BAMBI) algorithm implements the MultiNest package for nested sampling as well as the training of an artificial neural network (NN) to learn the likelihood function. In the [...]]]></description>
			<content:encoded><![CDATA[<p>In this paper we present an algorithm for rapid Bayesian analysis that combines the benefits of nested sampling and artificial neural networks. The blind accelerated multimodal Bayesian inference (BAMBI) algorithm implements the MultiNest package for nested sampling as well as the training of an artificial neural network (NN) to learn the likelihood function. In the case of computationally expensive likelihoods, this allows the substitution of a much more rapid approximation in order to increase significantly the speed of the analysis. We begin by demonstrating, with a few toy examples, the ability of a NN to learn complicated likelihood surfaces. BAMBI&#8217;s ability to decrease running time for Bayesian inference is then demonstrated in the context of estimating cosmological parameters from Wilkinson Microwave Anisotropy Probe and other observations. We show that valuable speed increases are achieved in addition to obtaining NNs trained on the likelihood functions for the different model and data combinations. These NNs can then be used for an even faster follow-up analysis using the same likelihood and different priors. This is a fully general algorithm that can be applied, without any pre-processing, to other problems with computationally expensive likelihood functions.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/19/bambi-blind-accelerated-multimodal-bayesian-inference-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>First Successful Adaptive Optics PSF Reconstruction at W. M. Keck Observatory</title>
		<link>http://voxcharta.org/2012/02/16/first-successful-adaptive-optics-psf-reconstruction-at-w-m-keck-observatory/</link>
		<comments>http://voxcharta.org/2012/02/16/first-successful-adaptive-optics-psf-reconstruction-at-w-m-keck-observatory/#comments</comments>
		<pubDate>Fri, 17 Feb 2012 01:47:27 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[aberration]]></category>
		<category><![CDATA[accuracy]]></category>
		<category><![CDATA[adaptive optics]]></category>
		<category><![CDATA[ao system]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[critical aspect]]></category>
		<category><![CDATA[gemini north]]></category>
		<category><![CDATA[guide star]]></category>
		<category><![CDATA[initial test]]></category>
		<category><![CDATA[keck ii]]></category>
		<category><![CDATA[keck observatory]]></category>
		<category><![CDATA[observation campaign]]></category>
		<category><![CDATA[optical turbulence]]></category>
		<category><![CDATA[phase diversity]]></category>
		<category><![CDATA[r project]]></category>
		<category><![CDATA[reconstruction]]></category>
		<category><![CDATA[sky]]></category>
		<category><![CDATA[stationarity]]></category>
		<category><![CDATA[turbulence parameters]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/16/first-successful-adaptive-optics-psf-reconstruction-at-w-m-keck-observatory/</guid>
		<description><![CDATA[We present the last results of our PSF reconstruction (PSF-R) project for the Keck-II and Gemini-North AO systems in natural guide star mode. Our initial tests have shown that the most critical aspects of PSF-R are the determination of the system static aberrations and the optical turbulence parameters, and we have set up a specific [...]]]></description>
			<content:encoded><![CDATA[<p>We present the last results of our PSF reconstruction (PSF-R) project for the Keck-II and Gemini-North AO systems in natural guide star mode. Our initial tests have shown that the most critical aspects of PSF-R are the determination of the system static aberrations and the optical turbulence parameters, and we have set up a specific observation campaign on the two systems to explore this. We demonstrate that deformable mirror based seeing monitor works well, and 10% accuracy is easily obtained. Phase diversity has been demonstrated to work on sky sources. Besides, residual phase stationarity is an important assumption in PSF-R, and we demonstrate here that it is basically true. As a result of these tests and verifications, we have been able for the first time to obtain a very good PSF reconstruction for the Keck-II system, in bright natural guide star mode.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>First science results from SOFIA/FORCAST: The mid-infrared view of the compact HII region W3A</title>
		<link>http://voxcharta.org/2012/02/16/first-science-results-from-sofiaforcast-the-mid-infrared-view-of-the-compact-hii-region-w3a/</link>
		<comments>http://voxcharta.org/2012/02/16/first-science-results-from-sofiaforcast-the-mid-infrared-view-of-the-compact-hii-region-w3a/#comments</comments>
		<pubDate>Fri, 17 Feb 2012 01:44:20 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[arcsec]]></category>
		<category><![CDATA[aromatic hydrocarbon]]></category>
		<category><![CDATA[color temperature]]></category>
		<category><![CDATA[compact hii region]]></category>
		<category><![CDATA[diffuse ism]]></category>
		<category><![CDATA[dust component]]></category>
		<category><![CDATA[factor 3]]></category>
		<category><![CDATA[faint object]]></category>
		<category><![CDATA[first science]]></category>
		<category><![CDATA[infrared camera]]></category>
		<category><![CDATA[infrared view]]></category>
		<category><![CDATA[intense emission]]></category>
		<category><![CDATA[mass ratio]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[optical depth]]></category>
		<category><![CDATA[radiation field]]></category>
		<category><![CDATA[science program]]></category>
		<category><![CDATA[science results]]></category>
		<category><![CDATA[spectral energy distribution]]></category>
		<category><![CDATA[temperature maps]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/16/first-science-results-from-sofiaforcast-the-mid-infrared-view-of-the-compact-hii-region-w3a/</guid>
		<description><![CDATA[The massive star forming region W3 was observed with the faint object infrared camera for the SOFIA telescope (FORCAST) as part of the Short Science program. The 6.4, 6.6, 7.7, 19.7, 24.2, 31.5 and 37.1 \um bandpasses were used to observe the emission of Polycyclic Aromatic Hydrocarbon (PAH) molecules, Very Small Grains and Big Grains. [...]]]></description>
			<content:encoded><![CDATA[<p>The massive star forming region W3 was observed with the faint object infrared camera for the SOFIA telescope (FORCAST) as part of the Short Science program. The 6.4, 6.6, 7.7, 19.7, 24.2, 31.5 and 37.1 \um bandpasses were used to observe the emission of Polycyclic Aromatic Hydrocarbon (PAH) molecules, Very Small Grains and Big Grains. Optical depth and color temperature maps of W3A show that IRS2 has blown a bubble devoid of gas and dust of $\sim$0.05 pc radius. It is embedded in a dusty shell of ionized gas that contributes 40% of the total 24 \um emission of W3A. This dust component is mostly heated by far ultraviolet, rather than trapped Ly$\alpha$ photons. This shell is itself surrounded by a thin ($\sim$0.01 pc) photodissociation region where PAHs show intense emission. The infrared spectral energy distribution (SED) of three different zones located at 8, 20 and 25\arcsec from IRS2, show that the peak of the SED shifts towards longer wavelengths, when moving away from the star. Adopting the stellar radiation field for these three positions, DUSTEM model fits to these SEDs yield a dust-to-gas mass ratio in the ionized gas similar to that in the diffuse ISM. However, the ratio of the IR-to-UV opacity of the dust in the ionized shell is increased by a factor $\simeq$3 compared to the diffuse ISM.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/16/first-science-results-from-sofiaforcast-the-mid-infrared-view-of-the-compact-hii-region-w3a/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Building the cosmic distance scale: from Hipparcos to Gaia</title>
		<link>http://voxcharta.org/2012/02/16/building-the-cosmic-distance-scale-from-hipparcos-to-gaia/</link>
		<comments>http://voxcharta.org/2012/02/16/building-the-cosmic-distance-scale-from-hipparcos-to-gaia/#comments</comments>
		<pubDate>Fri, 17 Feb 2012 01:40:03 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astrometry]]></category>
		<category><![CDATA[calibration]]></category>
		<category><![CDATA[chemical element]]></category>
		<category><![CDATA[cluster membership]]></category>
		<category><![CDATA[distance scale]]></category>
		<category><![CDATA[dpac]]></category>
		<category><![CDATA[drastic revision]]></category>
		<category><![CDATA[fantino]]></category>
		<category><![CDATA[hipparcos catalogue]]></category>
		<category><![CDATA[launch]]></category>
		<category><![CDATA[million stars]]></category>
		<category><![CDATA[orders of magnitude]]></category>
		<category><![CDATA[proper motion]]></category>
		<category><![CDATA[satellite attitude]]></category>
		<category><![CDATA[solar neighbourhood]]></category>
		<category><![CDATA[sp 1200]]></category>
		<category><![CDATA[spectroscopic observation]]></category>
		<category><![CDATA[tycho catalogues]]></category>
		<category><![CDATA[van leeuwen]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/16/building-the-cosmic-distance-scale-from-hipparcos-to-gaia/</guid>
		<description><![CDATA[Hipparcos, the first ever experiment of global astrometry, was launched by ESA in 1989 and its results published in 1997 (Perryman et al., Astron. Astrophys. 323, L49, 1997; Perryman &#38; ESA (eds), The Hipparcos and Tycho catalogues, ESA SP-1200, 1997). A new reduction was later performed using an improved satellite attitude reconstruction leading to an [...]]]></description>
			<content:encoded><![CDATA[<p>Hipparcos, the first ever experiment of global astrometry, was launched by ESA in 1989 and its results published in 1997 (Perryman et al., Astron. Astrophys. 323, L49, 1997; Perryman &amp; ESA (eds), The Hipparcos and Tycho catalogues, ESA SP-1200, 1997). A new reduction was later performed using an improved satellite attitude reconstruction leading to an improved accuracy for stars brighter than 9th magnitude (van Leeuwen &amp; Fantino, Astron. Astrophys. 439, 791, 2005; van Leeuwen, Astron. Astrophys. 474, 653, 2007).   The Hipparcos Catalogue provided an extended dataset of very accurate astrometric data (positions, trigonometric parallaxes and proper motions), enlarging by two orders of magnitude the quantity and quality of distance determinations and luminosity calibrations. The availability of more than 20000 stars with a trigonometric parallax known to better than 10% opened the way to a drastic revision of our 3-D knowledge of the solar neighbourhood and to a renewal of the calibration of many distance indicators and age estimations. The prospects opened by Gaia, the next ESA cornerstone, planned for launch in June 2013 (Perryman et al., Astron. Astrophys. 369, 339, 2001), are still much more dramatic: a billion objects with systematic and quasi simultaneous astrometric, spectrophotometric and spectroscopic observations, about 150 million stars with expected distances to better than 10%, all over the Galaxy. All stellar distance indicators, in very large numbers, will be directly measured, providing a direct calibration of their luminosity and making possible detailed studies of the impacts of various effects linked to chemical element abundances, age or cluster membership. With the help of simulations of the data expected from Gaia, obtained from the mission simulator developed by DPAC, we will illustrate what Gaia can provide with some selected examples.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>emcee: The MCMC Hammer</title>
		<link>http://voxcharta.org/2012/02/16/emcee-the-mcmc-hammer/</link>
		<comments>http://voxcharta.org/2012/02/16/emcee-the-mcmc-hammer/#comments</comments>
		<pubDate>Fri, 17 Feb 2012 01:37:51 +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[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/2012/02/16/emcee-the-mcmc-hammer/</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/2012/02/16/emcee-the-mcmc-hammer/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Chandra Publication Statistics [Replacement]</title>
		<link>http://voxcharta.org/2012/02/16/chandra-publication-statistics-replacement/</link>
		<comments>http://voxcharta.org/2012/02/16/chandra-publication-statistics-replacement/#comments</comments>
		<pubDate>Fri, 17 Feb 2012 01:35:02 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[10 years]]></category>
		<category><![CDATA[bibliographic database]]></category>
		<category><![CDATA[Chandra]]></category>
		<category><![CDATA[citation]]></category>
		<category><![CDATA[data retrieval]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[main categories]]></category>
		<category><![CDATA[median time]]></category>
		<category><![CDATA[observation]]></category>
		<category><![CDATA[observatory]]></category>
		<category><![CDATA[publication output]]></category>
		<category><![CDATA[publication statistics]]></category>
		<category><![CDATA[traditional metrics]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/16/chandra-publication-statistics-replacement/</guid>
		<description><![CDATA[In this study we develop and propose publication metrics, based on an analysis of data from the Chandra bibliographic database, that are more meaningful and less sensitive to observatory-specific characteristics than the traditional metrics. They fall in three main categories: speed of publication; fraction of observing time published; and archival usage. Citation of results is [...]]]></description>
			<content:encoded><![CDATA[<p>In this study we develop and propose publication metrics, based on an analysis of data from the Chandra bibliographic database, that are more meaningful and less sensitive to observatory-specific characteristics than the traditional metrics. They fall in three main categories: speed of publication; fraction of observing time published; and archival usage. Citation of results is a fourth category, but lends itself less well to definite statements. For Chandra, the median time from observation to publication is 2.36 years; after about 7 years 90% of the observing time is published; after 10 years 70% of the observing time is published more than twice; and the total annual publication output of the mission is 60-70% of the cumulative observing time available, assuming a two year lag between data retrieval and publication.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/16/chandra-publication-statistics-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The European Southern Observatory and VLT Telescopes on Paranal</title>
		<link>http://voxcharta.org/2012/02/15/the-european-southern-observatory-and-vlt-telescopes-on-paranal/</link>
		<comments>http://voxcharta.org/2012/02/15/the-european-southern-observatory-and-vlt-telescopes-on-paranal/#comments</comments>
		<pubDate>Thu, 16 Feb 2012 01:47:58 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cerro paranal]]></category>
		<category><![CDATA[european southern observatory]]></category>
		<category><![CDATA[overview lecture]]></category>
		<category><![CDATA[perspective]]></category>
		<category><![CDATA[southern observatory eso]]></category>
		<category><![CDATA[Telescope]]></category>
		<category><![CDATA[vlt telescope]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/15/the-european-southern-observatory-and-vlt-telescopes-on-paranal/</guid>
		<description><![CDATA[The Very Large Telescope (VLT) of the European Southern Observatory (ESO) on Cerro Paranal is one of the most influential observing complexes in the world. In this overview lecture, an introduction to the ESO organization and VLT telescopes is presented, along with a small selection of scientific works. Particular attention is given to the importance [...]]]></description>
			<content:encoded><![CDATA[<p>The Very Large Telescope (VLT) of the European Southern Observatory (ESO) on Cerro Paranal is one of the most influential observing complexes in the world. In this overview lecture, an introduction to the ESO organization and VLT telescopes is presented, along with a small selection of scientific works. Particular attention is given to the importance of the VLT for the Russian scientific community, as well as to present and future perspectives for making use of ESO and VLT data.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/15/the-european-southern-observatory-and-vlt-telescopes-on-paranal/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Three-dimensional track reconstruction for directional Dark Matter detection</title>
		<link>http://voxcharta.org/2012/02/15/three-dimensional-track-reconstruction-for-directional-dark-matter-detection/</link>
		<comments>http://voxcharta.org/2012/02/15/three-dimensional-track-reconstruction-for-directional-dark-matter-detection/#comments</comments>
		<pubDate>Thu, 16 Feb 2012 01:43:48 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[angular resolution]]></category>
		<category><![CDATA[anode]]></category>
		<category><![CDATA[axis]]></category>
		<category><![CDATA[contrary]]></category>
		<category><![CDATA[dark matter detection]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[drift]]></category>
		<category><![CDATA[efficiency values]]></category>
		<category><![CDATA[keV]]></category>
		<category><![CDATA[likelihood method]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[recognition capability]]></category>
		<category><![CDATA[recoil]]></category>
		<category><![CDATA[recoil energy]]></category>
		<category><![CDATA[search strategy]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[spatial resolution]]></category>
		<category><![CDATA[track reconstruction]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/15/three-dimensional-track-reconstruction-for-directional-dark-matter-detection/</guid>
		<description><![CDATA[Directional detection of Dark Matter is a promising search strategy. However, to perform such detection, a given set of parameters has to be retrieved from the recoiling tracks : direction, sense and position in the detector volume. In order to optimize the track reconstruction and to fully exploit the data of forthcoming directional detectors, we [...]]]></description>
			<content:encoded><![CDATA[<p>Directional detection of Dark Matter is a promising search strategy. However, to perform such detection, a given set of parameters has to be retrieved from the recoiling tracks : direction, sense and position in the detector volume. In order to optimize the track reconstruction and to fully exploit the data of forthcoming directional detectors, we present a likelihood method dedicated to 3D track reconstruction. This new analysis method is applied to the MIMAC detector. It requires a full simulation of track measurements in order to compare real tracks to simulated ones. We conclude that a good spatial resolution can be achieved, i.e. sub-mm in the anode plane and cm along the drift axis. This opens the possibility to perform a fiducialization of directional detectors. The angular resolution is shown to range between 20$^\circ$ to 80$^\circ$, depending on the recoil energy, which is however enough to achieve a high significance discovery of Dark Matter. On the contrary, we show that sense recognition capability of directional detectors depends strongly on the recoil energy and the drift distance, with small efficiency values (50%-70%). We suggest not to consider this information either for exclusion or discovery of Dark Matter for recoils below 100 keV and then to focus on axial directional data.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/15/three-dimensional-track-reconstruction-for-directional-dark-matter-detection/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Photometric Reverberation Mapping of the Broad Emission Line Region in Quasars [Replacement]</title>
		<link>http://voxcharta.org/2012/02/15/photometric-reverberation-mapping-of-the-broad-emission-line-region-in-quasars-replacement/</link>
		<comments>http://voxcharta.org/2012/02/15/photometric-reverberation-mapping-of-the-broad-emission-line-region-in-quasars-replacement/#comments</comments>
		<pubDate>Thu, 16 Feb 2012 01:39:06 +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[black hole]]></category>
		<category><![CDATA[blr]]></category>
		<category><![CDATA[broadband]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[feasibility study]]></category>
		<category><![CDATA[mapping technique]]></category>
		<category><![CDATA[Measurement]]></category>
		<category><![CDATA[numerical simulation]]></category>
		<category><![CDATA[palomar]]></category>
		<category><![CDATA[pitfalls]]></category>
		<category><![CDATA[quasar]]></category>
		<category><![CDATA[reverberation]]></category>
		<category><![CDATA[size measurement]]></category>
		<category><![CDATA[subset]]></category>
		<category><![CDATA[survey]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/15/photometric-reverberation-mapping-of-the-broad-emission-line-region-in-quasars-replacement/</guid>
		<description><![CDATA[A method is proposed for measuring the size of the broad emission line region (BLR) in quasars using broadband photometric data. A feasibility study, based on numerical simulations, points to the advantages and pitfalls associated with this approach. The method is applied to a subset of the Palomar-Green quasar sample for which independent BLR size [...]]]></description>
			<content:encoded><![CDATA[<p>A method is proposed for measuring the size of the broad emission line region (BLR) in quasars using broadband photometric data. A feasibility study, based on numerical simulations, points to the advantages and pitfalls associated with this approach. The method is applied to a subset of the Palomar-Green quasar sample for which independent BLR size measurements are available. An agreement is found between the results of the photometric method and the spectroscopic reverberation mapping technique. Implications for the measurement of BLR sizes and black hole masses for numerous quasars in the era of large surveys are discussed.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/15/photometric-reverberation-mapping-of-the-broad-emission-line-region-in-quasars-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>All Transients, All the Time: Real-Time Radio Transient Detection with Interferometric Closure Quantities [Replacement]</title>
		<link>http://voxcharta.org/2012/02/15/all-transients-all-the-time-real-time-radio-transient-detection-with-interferometric-closure-quantities-replacement/</link>
		<comments>http://voxcharta.org/2012/02/15/all-transients-all-the-time-real-time-radio-transient-detection-with-interferometric-closure-quantities-replacement/#comments</comments>
		<pubDate>Thu, 16 Feb 2012 01:36:16 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[allen telescope array]]></category>
		<category><![CDATA[baseline]]></category>
		<category><![CDATA[electron density]]></category>
		<category><![CDATA[exoplanet]]></category>
		<category><![CDATA[generation radio]]></category>
		<category><![CDATA[host galaxy]]></category>
		<category><![CDATA[interferometer data]]></category>
		<category><![CDATA[intergalactic medium]]></category>
		<category><![CDATA[mjy]]></category>
		<category><![CDATA[pulsars]]></category>
		<category><![CDATA[radio interferometer]]></category>
		<category><![CDATA[science application]]></category>
		<category><![CDATA[time radio]]></category>
		<category><![CDATA[time scale]]></category>
		<category><![CDATA[timescale]]></category>
		<category><![CDATA[transients]]></category>
		<category><![CDATA[unique science]]></category>
		<category><![CDATA[very large array]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/15/all-transients-all-the-time-real-time-radio-transient-detection-with-interferometric-closure-quantities-replacement/</guid>
		<description><![CDATA[We demonstrate a new technique for detecting radio transients based on interferometric closure quantities. The technique uses the bispectrum, the product of visibilities around a closed-loop of baselines of an interferometer. The bispectrum is calibration independent, resistant to interference, and computationally efficient, so it can be built into correlators for real-time transient detection. Our technique [...]]]></description>
			<content:encoded><![CDATA[<p>We demonstrate a new technique for detecting radio transients based on interferometric closure quantities. The technique uses the bispectrum, the product of visibilities around a closed-loop of baselines of an interferometer. The bispectrum is calibration independent, resistant to interference, and computationally efficient, so it can be built into correlators for real-time transient detection. Our technique could find celestial transients anywhere in the field of view and localize them to arcsecond precision. At the Karl G. Jansky Very Large Array (VLA), such a system would have a high survey speed and a 5-sigma sensitivity of 38 mJy on 10 ms timescales with 1 GHz of bandwidth. The ability to localize dispersed millisecond pulses to arcsecond precision in large volumes of interferometer data has several unique science applications. Localizing individual pulses from Galactic pulsars will help find X-ray counterparts that define their physical properties, while finding host galaxies of extragalactic transients will measure the electron density of the intergalactic medium with a single dispersed pulse. Exoplanets and active stars have distinct millisecond variability that can be used to identify them and probe their magnetospheres. We use millisecond time scale visibilities from the Allen Telescope Array (ATA) and VLA to show that the bispectrum can detect dispersed pulses and reject local interference. The computational and data efficiency of the bispectrum will help find transients on a range of time scales with next-generation radio interferometers.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/15/all-transients-all-the-time-real-time-radio-transient-detection-with-interferometric-closure-quantities-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Optimal filters for detecting cosmic bubble collisions</title>
		<link>http://voxcharta.org/2012/02/14/optimal-filters-for-detecting-cosmic-bubble-collisions/</link>
		<comments>http://voxcharta.org/2012/02/14/optimal-filters-for-detecting-cosmic-bubble-collisions/#comments</comments>
		<pubDate>Wed, 15 Feb 2012 01:58:30 +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[algorithm]]></category>
		<category><![CDATA[collisions]]></category>
		<category><![CDATA[concordance]]></category>
		<category><![CDATA[cosmic microwave background]]></category>
		<category><![CDATA[cosmological model]]></category>
		<category><![CDATA[dataset]]></category>
		<category><![CDATA[enhancement]]></category>
		<category><![CDATA[global parameters]]></category>
		<category><![CDATA[inflation]]></category>
		<category><![CDATA[likelihood]]></category>
		<category><![CDATA[microwave anisotropy probe]]></category>
		<category><![CDATA[planck]]></category>
		<category><![CDATA[posterior probability]]></category>
		<category><![CDATA[probability distribution]]></category>
		<category><![CDATA[scenarios]]></category>
		<category><![CDATA[signature]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[wilkinson microwave anisotropy]]></category>
		<category><![CDATA[wilkinson microwave anisotropy probe]]></category>
		<category><![CDATA[wilkinson microwave anisotropy probe wmap]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/14/optimal-filters-for-detecting-cosmic-bubble-collisions/</guid>
		<description><![CDATA[A number of well-motivated extensions of the LCDM concordance cosmological model postulate the existence of a population of sources embedded in the cosmic microwave background (CMB). One such example is the signature of cosmic bubble collisions which arise in models of eternal inflation. The most unambiguous way to test these scenarios is to evaluate the [...]]]></description>
			<content:encoded><![CDATA[<p>A number of well-motivated extensions of the LCDM concordance cosmological model postulate the existence of a population of sources embedded in the cosmic microwave background (CMB). One such example is the signature of cosmic bubble collisions which arise in models of eternal inflation. The most unambiguous way to test these scenarios is to evaluate the full posterior probability distribution of the global parameters defining the theory; however, a direct evaluation is computationally impractical on large datasets, such as those obtained by the Wilkinson Microwave Anisotropy Probe (WMAP) and Planck. A method to approximate the full posterior has been developed recently, which requires as an input a set of candidate sources which are most likely to give the largest contribution to the likelihood. In this article, we present an improved algorithm for detecting candidate sources using optimal filters, and apply it to detect candidate bubble collision signatures in WMAP 7-year observations. We show both theoretically and through simulations that this algorithm provides an enhancement in sensitivity over previous methods by a factor of approximately two. Moreover, no other filter-based approach can provide a superior enhancement of these signatures. Applying our algorithm to WMAP 7-year observations, we detect eight new candidate bubble collision signatures for follow-up analysis.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/14/optimal-filters-for-detecting-cosmic-bubble-collisions/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Regularization Techniques for PSF-Matching Kernels. I. Choice of Kernel Basis</title>
		<link>http://voxcharta.org/2012/02/14/regularization-techniques-for-psf-matching-kernels-i-choice-of-kernel-basis/</link>
		<comments>http://voxcharta.org/2012/02/14/regularization-techniques-for-psf-matching-kernels-i-choice-of-kernel-basis/#comments</comments>
		<pubDate>Wed, 15 Feb 2012 01:53:15 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[basis function]]></category>
		<category><![CDATA[compactness]]></category>
		<category><![CDATA[correct choice]]></category>
		<category><![CDATA[degree of freedom]]></category>
		<category><![CDATA[degrees of freedom]]></category>
		<category><![CDATA[delta function]]></category>
		<category><![CDATA[difference image]]></category>
		<category><![CDATA[estimators]]></category>
		<category><![CDATA[free basis]]></category>
		<category><![CDATA[gauss]]></category>
		<category><![CDATA[gaussian kernel]]></category>
		<category><![CDATA[generality]]></category>
		<category><![CDATA[image subtraction]]></category>
		<category><![CDATA[kernel size]]></category>
		<category><![CDATA[Lambda]]></category>
		<category><![CDATA[linear decomposition]]></category>
		<category><![CDATA[polynomial]]></category>
		<category><![CDATA[regularization techniques]]></category>
		<category><![CDATA[variance]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/14/regularization-techniques-for-psf-matching-kernels-i-choice-of-kernel-basis/</guid>
		<description><![CDATA[We review current methods for building PSF-matching kernels for the purposes of image subtraction or coaddition. Such methods use a linear decomposition of the kernel on a series of basis functions. The correct choice of these basis functions is fundamental to the efficiency and effectiveness of the matching &#8211; the chosen bases should represent the [...]]]></description>
			<content:encoded><![CDATA[<p>We review current methods for building PSF-matching kernels for the purposes of image subtraction or coaddition. Such methods use a linear decomposition of the kernel on a series of basis functions. The correct choice of these basis functions is fundamental to the efficiency and effectiveness of the matching &#8211; the chosen bases should represent the underlying signal using a reasonably small number of shapes, and/or have a minimum number of user-adjustable tuning parameters. We examine methods whose bases comprise multiple Gauss-Hermite polynomials, as well as a form free basis composed of delta-functions. Kernels derived from delta-functions are unsurprisingly shown to be more expressive; they are able to take more general shapes and perform better in situations where sum-of-Gaussian methods are known to fail. However, due to its many degrees of freedom (the maximum number allowed by the kernel size) this basis tends to overfit the problem, and yields noisy kernels having large variance. We introduce a new technique to regularize these delta-function kernel solutions, which bridges the gap between the generality of delta-function kernels, and the compactness of sum-of-Gaussian kernels. Through this regularization we are able to create general kernel solutions that represent the intrinsic shape of the PSF-matching kernel with only one degree of freedom, the strength of the regularization lambda. The role of lambda is effectively to exchange variance in the resulting difference image with variance in the kernel itself. We examine considerations in choosing the value of lambda, including statistical risk estimators and the ability of the solution to predict solutions for adjacent areas. Both of these suggest moderate strengths of lambda between 0.1 and 1.0, although this optimization is likely dataset dependent.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/14/regularization-techniques-for-psf-matching-kernels-i-choice-of-kernel-basis/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Removing the trend of drift induced from acceleration noise for LISA [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/14/removing-the-trend-of-drift-induced-from-acceleration-noise-for-lisa-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/14/removing-the-trend-of-drift-induced-from-acceleration-noise-for-lisa-cross-listing/#comments</comments>
		<pubDate>Wed, 15 Feb 2012 01:50:20 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration]]></category>
		<category><![CDATA[annealing]]></category>
		<category><![CDATA[drift]]></category>
		<category><![CDATA[frequency domain]]></category>
		<category><![CDATA[gelman]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[instrumental noise]]></category>
		<category><![CDATA[interferometer]]></category>
		<category><![CDATA[markov chain monte]]></category>
		<category><![CDATA[markov chain monte carlo]]></category>
		<category><![CDATA[monte carlo method]]></category>
		<category><![CDATA[new representation]]></category>
		<category><![CDATA[power spectrum]]></category>
		<category><![CDATA[probability distribution]]></category>
		<category><![CDATA[proof mass]]></category>
		<category><![CDATA[quadratic function]]></category>
		<category><![CDATA[random nature]]></category>
		<category><![CDATA[residuals]]></category>
		<category><![CDATA[time domain]]></category>
		<category><![CDATA[time series data]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/14/removing-the-trend-of-drift-induced-from-acceleration-noise-for-lisa-cross-listing/</guid>
		<description><![CDATA[In this paper we demonstrate a methodology to remove the power of the drift induced from random acceleration on LISA proof mass in the frequency domain. The drift must be cleaned from LISA time series data in advance of any further analysis. The cleaning is usually performed in the time domain by using a quadratic [...]]]></description>
			<content:encoded><![CDATA[<p>In this paper we demonstrate a methodology to remove the power of the drift induced from random acceleration on LISA proof mass in the frequency domain. The drift must be cleaned from LISA time series data in advance of any further analysis. The cleaning is usually performed in the time domain by using a quadratic function to fit the time series data, and then removing the fitted part from the data. Having Fourier transformed the residuals, and then convolved with LISA transfer function, LISA sensitivity curve can be obtained. However, cosmic gravitational-wave background cannot be retrieved with this approach due to its random nature. Here we provide a new representation of power spectrum given by discrete Fourier transform, which is applied to find the function of the drift power for the cleaning in the frequency domain. We also give the probability distribution used to analyze the data in the frequency domain. We combine several techniques, including Markov Chain Monte Carlo method, simulated annealing, and Gelman &amp; Rubin&#8217;s method, with Baye&#8217;s theorem to build the algorithm. The algorithm is utilized to analyze 24 simulations of LISA instrumental noise. We prove that the LISA sensitivity can be recovered through this approach. It can help us to build algorithms for some tasks which are must accomplished in the frequency domain for LISA data analysis. This method can be applied to other space-borne interferometers if charges on their proof masses cannot be perfectly cancelled.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/14/removing-the-trend-of-drift-induced-from-acceleration-noise-for-lisa-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Measuring the Effects of Artificial Viscosity in SPH Simulations of Rotating Fluid Flows [Replacement]</title>
		<link>http://voxcharta.org/2012/02/14/measuring-the-effects-of-artificial-viscosity-in-sph-simulations-of-rotating-fluid-flows-replacement/</link>
		<comments>http://voxcharta.org/2012/02/14/measuring-the-effects-of-artificial-viscosity-in-sph-simulations-of-rotating-fluid-flows-replacement/#comments</comments>
		<pubDate>Wed, 15 Feb 2012 01:34:19 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[applicability]]></category>
		<category><![CDATA[artificial viscosity]]></category>
		<category><![CDATA[characterization]]></category>
		<category><![CDATA[dependencies]]></category>
		<category><![CDATA[dependent viscosity]]></category>
		<category><![CDATA[detailed description]]></category>
		<category><![CDATA[disc flow]]></category>
		<category><![CDATA[drawback]]></category>
		<category><![CDATA[entropy]]></category>
		<category><![CDATA[flow examples]]></category>
		<category><![CDATA[flow parameters]]></category>
		<category><![CDATA[fluctuation]]></category>
		<category><![CDATA[formulae]]></category>
		<category><![CDATA[initial placement]]></category>
		<category><![CDATA[lows]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[shear viscosity]]></category>
		<category><![CDATA[sph particles]]></category>
		<category><![CDATA[sph simulation]]></category>
		<category><![CDATA[viscous effects]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/14/measuring-the-effects-of-artificial-viscosity-in-sph-simulations-of-rotating-fluid-flows-replacement/</guid>
		<description><![CDATA[A commonly cited drawback of SPH is the introduction of spurious shear viscosity by the artificial viscosity term in situations involving rotation. Existing approaches for quantifying its effect include approximate analytic formulae and disc-averaged be- haviour in specific ring-spreading simulations, based on the kinematic effects produced by the artificial viscosity. These methods have disadvantages, in [...]]]></description>
			<content:encoded><![CDATA[<p>A commonly cited drawback of SPH is the introduction of spurious shear viscosity by the artificial viscosity term in situations involving rotation. Existing approaches for quantifying its effect include approximate analytic formulae and disc-averaged be- haviour in specific ring-spreading simulations, based on the kinematic effects produced by the artificial viscosity. These methods have disadvantages, in that they typically are applicable to a very small range of physical scenarios, have a large number of simplifying assumptions, and often are tied to specific SPH formulations which do not include corrective (e.g., Balsara) or time-dependent viscosity terms. In this study we have developed a simple, generally applicable and practical technique for evaluating the local effect of artificial viscosity directly from the creation of specific entropy for each SPH particle. This local approach is simple and quick to implement, and it al- lows a detailed characterization of viscous effects as a function of position. Several advantages of this method are discussed, including its ease in evaluation, its greater accuracy and its broad applicability. In order to compare this new method with ex- isting ones, simple disc flow examples are used. Even in these basic cases, the very roughly approximate nature of the previous methods is shown. Our local method pro- vides a detailed description of the effects of the artificial viscosity throughout the disc, even for extended examples which implement Balsara corrections. As a further use of this approach, explicit dependencies of the effective viscosity in terms of SPH and flow parameters are estimated from the example cases. In an appendix, a method for the initial placement of SPH particles is discussed which is very effective in reducing numerical fluctuations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/14/measuring-the-effects-of-artificial-viscosity-in-sph-simulations-of-rotating-fluid-flows-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Regularizing made-to-measure particle models of galaxies</title>
		<link>http://voxcharta.org/2012/02/13/regularizing-made-to-measure-particle-models-of-galaxies/</link>
		<comments>http://voxcharta.org/2012/02/13/regularizing-made-to-measure-particle-models-of-galaxies/#comments</comments>
		<pubDate>Tue, 14 Feb 2012 02:20:21 +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[anisotropy]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[distribution function]]></category>
		<category><![CDATA[dynamical model]]></category>
		<category><![CDATA[dynamical structure]]></category>
		<category><![CDATA[elliptical galaxy]]></category>
		<category><![CDATA[galaxy models]]></category>
		<category><![CDATA[global phase]]></category>
		<category><![CDATA[kinematic data]]></category>
		<category><![CDATA[noisy data]]></category>
		<category><![CDATA[observational data]]></category>
		<category><![CDATA[parallel code]]></category>
		<category><![CDATA[particle model]]></category>
		<category><![CDATA[phase space]]></category>
		<category><![CDATA[priors]]></category>
		<category><![CDATA[smooth model]]></category>
		<category><![CDATA[target]]></category>
		<category><![CDATA[true solution]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/13/regularizing-made-to-measure-particle-models-of-galaxies/</guid>
		<description><![CDATA[Made-to-measure methods such as the parallel code NMAGIC are powerful tools to build galaxy models reproducing observational data. They work by adapting the particle weights in an N-body system until the target observables are well matched. Here we introduce a moving prior regularization (MPR) method for such particle models. It is based on determining from [...]]]></description>
			<content:encoded><![CDATA[<p>Made-to-measure methods such as the parallel code NMAGIC are powerful tools to build galaxy models reproducing observational data. They work by adapting the particle weights in an N-body system until the target observables are well matched. Here we introduce a moving prior regularization (MPR) method for such particle models. It is based on determining from the particles a distribution of priors in phase-space, which are updated in parallel with the weight adaptation. This method allows one to construct smooth models from noisy data without erasing global phase-space gradients. We first apply MPR to a spherical system for which the distribution function can in theory be uniquely recovered from idealized data. We show that NMAGIC with MPR indeed converges to the true solution with very good accuracy, independent of the initial particle model. Compared to the standard weight entropy regularization, biases in the anisotropy structure are removed and local fluctuations in the intrinsic distribution function are reduced. We then investigate how the uncertainties in the inferred dynamical structure increase with less complete and noisier kinematic data, and how the dependence on the initial particle model also increases. Finally, we apply the MPR technique to the two intermediate-luminosity elliptical galaxies NGC 4697 and NGC 3379, obtaining smoother dynamical models in luminous and dark matter potentials.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/13/regularizing-made-to-measure-particle-models-of-galaxies/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Sticking coefficient of hydrogen and deuterium on silicates under interstellar conditions</title>
		<link>http://voxcharta.org/2012/02/13/sticking-coefficient-of-hydrogen-and-deuterium-on-silicates-under-interstellar-conditions/</link>
		<comments>http://voxcharta.org/2012/02/13/sticking-coefficient-of-hydrogen-and-deuterium-on-silicates-under-interstellar-conditions/#comments</comments>
		<pubDate>Tue, 14 Feb 2012 02:06:24 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[coefficients]]></category>
		<category><![CDATA[deuterium]]></category>
		<category><![CDATA[experimental result]]></category>
		<category><![CDATA[extrapolation]]></category>
		<category><![CDATA[formulae]]></category>
		<category><![CDATA[gas temperature]]></category>
		<category><![CDATA[impactor]]></category>
		<category><![CDATA[interstellar dust grain]]></category>
		<category><![CDATA[isotopic effects]]></category>
		<category><![CDATA[molecular beam]]></category>
		<category><![CDATA[molecular hydrogen formation]]></category>
		<category><![CDATA[physical model]]></category>
		<category><![CDATA[quadrupole mass spectrometer]]></category>
		<category><![CDATA[recombination]]></category>
		<category><![CDATA[silicate]]></category>
		<category><![CDATA[thermal distribution]]></category>
		<category><![CDATA[water ice]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/13/sticking-coefficient-of-hydrogen-and-deuterium-on-silicates-under-interstellar-conditions/</guid>
		<description><![CDATA[Sticking of H and D atoms on interstellar dust grains is the first step in molecular hydrogen formation, which is a key reaction in the InterStellar Medium (ISM). After studying the sticking coefficients of H2 and D2 molecules on amorphous silicate surfaces experimentally and theoretically, we extrapolate the results to the sticking coefficient of atoms [...]]]></description>
			<content:encoded><![CDATA[<p>Sticking of H and D atoms on interstellar dust grains is the first step in molecular hydrogen formation, which is a key reaction in the InterStellar Medium (ISM). After studying the sticking coefficients of H2 and D2 molecules on amorphous silicate surfaces experimentally and theoretically, we extrapolate the results to the sticking coefficient of atoms and propose a formulae that gives the sticking coefficients of H and D on both silicates and icy dust grains. In our experiments, we used the King and Wells method for measuring the sticking coefficients of H2 and D2 molecules on a silicate surface held at 10 K. It consists of measuring with a QMS (quadrupole mass spectrometer) the signals of H2 and D2 molecules reflected by the surface during the exposure of the sample to the molecular beam at a temperature ranging from 20 K to 340 K. We tested the efficiency of a physical model, developed previously for sticking on water-ice surfaces. We applied this model to our experimental results for the sticking coefficients of H2 and D2 molecules on a silicate surface and estimated the sticking coefficient of atoms by a single measurement of atomic recombination and propose an extrapolation. Sticking of H, D, HD, H2, and D2 on silicates grains behaves the same as on icy dust grains. The sticking decreases with the gas temperature, and is dependent on the mass of the impactor. The sticking coefficient for both surfaces and impactors can be modeled by an analytical formulae S(T), which describes both the experiments and the thermal distribution expected in an astrophysical context. The parameters S0 and T0 are summarized in a table. Previous estimates for the sticking coefficient of H atoms are close to the new estimation; however, we find that, when isotopic effects are taken into account, the sticking coefficient variations can be as much as a factor of 2 at T=100 K.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/13/sticking-coefficient-of-hydrogen-and-deuterium-on-silicates-under-interstellar-conditions/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Evolutionary Computation in Astronomy and Astrophysics: A Review [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/13/evolutionary-computation-in-astronomy-and-astrophysics-a-review-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/13/evolutionary-computation-in-astronomy-and-astrophysics-a-review-cross-listing/#comments</comments>
		<pubDate>Tue, 14 Feb 2012 02:04:59 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astronomical science]]></category>
		<category><![CDATA[astronomy and astrophysics]]></category>
		<category><![CDATA[biological mechanisms]]></category>
		<category><![CDATA[computational resource]]></category>
		<category><![CDATA[darwinian principles]]></category>
		<category><![CDATA[estimation]]></category>
		<category><![CDATA[evolutionary computation]]></category>
		<category><![CDATA[future research]]></category>
		<category><![CDATA[general description]]></category>
		<category><![CDATA[global perspective]]></category>
		<category><![CDATA[last ten years]]></category>
		<category><![CDATA[mechanisms of evolution]]></category>
		<category><![CDATA[methodology]]></category>
		<category><![CDATA[objective optimization]]></category>
		<category><![CDATA[optimization method]]></category>
		<category><![CDATA[optimization problem]]></category>
		<category><![CDATA[principles of life]]></category>
		<category><![CDATA[promising applications]]></category>
		<category><![CDATA[quality solutions]]></category>
		<category><![CDATA[repercussion]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/13/evolutionary-computation-in-astronomy-and-astrophysics-a-review-cross-listing/</guid>
		<description><![CDATA[In general Evolutionary Computation (EC) includes a number of optimization methods inspired by biological mechanisms of evolution. The methods catalogued in this area use the Darwinian principles of life evolution to produce algorithms that returns high quality solutions to hard-to-solve optimization problems. The main strength of EC is precisely that they provide good solutions even [...]]]></description>
			<content:encoded><![CDATA[<p>In general Evolutionary Computation (EC) includes a number of optimization methods inspired by biological mechanisms of evolution. The methods catalogued in this area use the Darwinian principles of life evolution to produce algorithms that returns high quality solutions to hard-to-solve optimization problems. The main strength of EC is precisely that they provide good solutions even if the computational resources (e.g., running time) are limited. Astronomy and Astrophysics are two fields that often require optimizing problems of high complexity or analyzing a huge amount of data and the so-called complete optimization methods are inherently limited by the size of the problem/data. For instance, reliable analysis of large amounts of data is central to modern astrophysics and astronomical sciences in general. EC techniques perform well where other optimization methods are inherently limited (as complete methods applied to NP-hard problems), and in the last ten years, numerous proposals have come up that apply with greater or lesser success methodologies of evolutional computation to common engineering problems. Some of these problems, such as the estimation of non-lineal parameters, the development of automatic learning techniques, the implementation of control systems, or the resolution of multi-objective optimization problems, have had (and have) a special repercussion in the fields. For these reasons EC emerges as a feasible alternative for traditional methods. In this paper, we discuss some promising applications in this direction and a number of recent works in this area; the paper also includes a general description of EC to provide a global perspective to the reader and gives some guidelines of application of EC techniques for future research</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/13/evolutionary-computation-in-astronomy-and-astrophysics-a-review-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Balloon-borne gamma-ray telescope with nuclear emulsion : overview and status</title>
		<link>http://voxcharta.org/2012/02/13/balloon-borne-gamma-ray-telescope-with-nuclear-emulsion-overview-and-status/</link>
		<comments>http://voxcharta.org/2012/02/13/balloon-borne-gamma-ray-telescope-with-nuclear-emulsion-overview-and-status/#comments</comments>
		<pubDate>Tue, 14 Feb 2012 02:03:15 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[balloon]]></category>
		<category><![CDATA[capability]]></category>
		<category><![CDATA[electron pairs]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[gamma ray telescope]]></category>
		<category><![CDATA[innovation]]></category>
		<category><![CDATA[nuclear emulsion]]></category>
		<category><![CDATA[polarization]]></category>
		<category><![CDATA[precise measurement]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/13/balloon-borne-gamma-ray-telescope-with-nuclear-emulsion-overview-and-status/</guid>
		<description><![CDATA[Detecting the first electron pairs with nuclear emulsion allows a precise measurement of the direction of incident gamma-rays as well as their polarization. With recent innovations in emulsion scanning, emulsion analyzing capability is becoming increasingly powerful. Presently, we are developing a balloon-borne gamma-ray telescope using nuclear emulsion. An overview and a status of our telescope [...]]]></description>
			<content:encoded><![CDATA[<p>Detecting the first electron pairs with nuclear emulsion allows a precise measurement of the direction of incident gamma-rays as well as their polarization. With recent innovations in emulsion scanning, emulsion analyzing capability is becoming increasingly powerful. Presently, we are developing a balloon-borne gamma-ray telescope using nuclear emulsion. An overview and a status of our telescope is given.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/13/balloon-borne-gamma-ray-telescope-with-nuclear-emulsion-overview-and-status/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The HARPS-TERRA project I. Description of the algorithms, performance and new measurements on a few remarkable stars observed by HARPS</title>
		<link>http://voxcharta.org/2012/02/13/the-harps-terra-project-i-description-of-the-algorithms-performance-and-new-measurements-on-a-few-remarkable-stars-observed-by-harps/</link>
		<comments>http://voxcharta.org/2012/02/13/the-harps-terra-project-i-description-of-the-algorithms-performance-and-new-measurements-on-a-few-remarkable-stars-observed-by-harps/#comments</comments>
		<pubDate>Tue, 14 Feb 2012 02:02:55 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorption spectrum]]></category>
		<category><![CDATA[calibration source]]></category>
		<category><![CDATA[correlation function]]></category>
		<category><![CDATA[cross correlation]]></category>
		<category><![CDATA[doppler measurement]]></category>
		<category><![CDATA[doppler shift]]></category>
		<category><![CDATA[doppler spectroscopy]]></category>
		<category><![CDATA[habitable world]]></category>
		<category><![CDATA[la silla chile]]></category>
		<category><![CDATA[least square]]></category>
		<category><![CDATA[nearby star]]></category>
		<category><![CDATA[optical wavelength]]></category>
		<category><![CDATA[precision doppler]]></category>
		<category><![CDATA[radial velocity]]></category>
		<category><![CDATA[signal to noise ratio]]></category>
		<category><![CDATA[spectrograph]]></category>
		<category><![CDATA[stellar spectrum]]></category>
		<category><![CDATA[template matching]]></category>
		<category><![CDATA[terra project]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/13/the-harps-terra-project-i-description-of-the-algorithms-performance-and-new-measurements-on-a-few-remarkable-stars-observed-by-harps/</guid>
		<description><![CDATA[Doppler spectroscopy has uncovered or confirmed all the known planets orbiting nearby stars. Two different approaches are used to obtain precision Doppler measurements at optical wavelengths. The first approach is the gas cell method, which is based on the least-squares matching of the absorption spectrum of Iodine over-imposed to the spectrum of the star. The [...]]]></description>
			<content:encoded><![CDATA[<p>Doppler spectroscopy has uncovered or confirmed all the known planets orbiting nearby stars. Two different approaches are used to obtain precision Doppler measurements at optical wavelengths. The first approach is the gas cell method, which is based on the least-squares matching of the absorption spectrum of Iodine over-imposed to the spectrum of the star. The second method relies on the construction of a stabilized spectrograph calibrated in wavelength with an externally fed calibration source. The most precise stabilized spectrometer in operation is HARPS, operated by ESO in La Silla/Chile. In the case of HARPS, the Doppler measurement is obtained using the so&#8211;called Cross-Correlation Function technique (CCF). It consists of multiplying the stellar spectrum with a binary mask and finding the minimum of such product as a function of the stellar Doppler shift. Such mask is weighted to account for the different depths of the stellar lines. It is known that CCF is suboptimal in exploiting the Doppler information in the stellar spectrum. Here, we describe an algorithm to obtain precision RV measurements based on least squares matching of each observation to a high signal-to-noise ratio template. Such algorithm is implemented in our software called HARPS-TERRA (Template Enhanced Radial velocity Re-analysis Application). We show that, compared to CCF, template matching provides a significant improvement in accuracy, specially when applied to M dwarfs. We conclude that other stabilized spectrographs should use a similar approach to achieve the sub \ms precision required to detect potentially habitable worlds around nearby stars.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/13/the-harps-terra-project-i-description-of-the-algorithms-performance-and-new-measurements-on-a-few-remarkable-stars-observed-by-harps/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Citizen Science: Contributions to Astronomy Research</title>
		<link>http://voxcharta.org/2012/02/13/citizen-science-contributions-to-astronomy-research/</link>
		<comments>http://voxcharta.org/2012/02/13/citizen-science-contributions-to-astronomy-research/#comments</comments>
		<pubDate>Tue, 14 Feb 2012 02:02:35 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[19th century]]></category>
		<category><![CDATA[adoption]]></category>
		<category><![CDATA[amateurs]]></category>
		<category><![CDATA[astronomy research]]></category>
		<category><![CDATA[birdwatching]]></category>
		<category><![CDATA[citizen science]]></category>
		<category><![CDATA[endeavor]]></category>
		<category><![CDATA[entific]]></category>
		<category><![CDATA[participatory projects]]></category>
		<category><![CDATA[pipeline]]></category>
		<category><![CDATA[sci]]></category>
		<category><![CDATA[science contributions]]></category>
		<category><![CDATA[science cs]]></category>
		<category><![CDATA[scientist]]></category>
		<category><![CDATA[volunteers]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/13/citizen-science-contributions-to-astronomy-research/</guid>
		<description><![CDATA[The contributions of everyday individuals to significant research has grown dramatically beyond the early days of classical birdwatching and endeavors of amateurs of the 19th century. Now people who are casually interested in science can participate directly in research covering diverse scientific fields. Regarding astronomy, volunteers, either as individuals or as networks of people, are [...]]]></description>
			<content:encoded><![CDATA[<p>The contributions of everyday individuals to significant research has grown dramatically beyond the early days of classical birdwatching and endeavors of amateurs of the 19th century. Now people who are casually interested in science can participate directly in research covering diverse scientific fields. Regarding astronomy, volunteers, either as individuals or as networks of people, are involved in a variety of types of studies. Citizen Science is intuitive, engaging, yet necessarily robust in its adoption of sci-entific principles and methods. Herein, we discuss Citizen Science, focusing on fully participatory projects such as Zooniverse (by several of the au-thors CL, AS, LF, SB), with mention of other programs. In particular, we make the case that citizen science (CS) can be an important aspect of the scientific data analysis pipelines provided to scientists by observatories.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/13/citizen-science-contributions-to-astronomy-research/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Characterization of the Hamamatsu R11410-10 3-Inch Photomultiplier Tube for Dark Matter Direct Detection Experiments [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/13/characterization-of-the-hamamatsu-r11410-10-3-inch-photomultiplier-tube-for-dark-matter-direct-detection-experiments-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/13/characterization-of-the-hamamatsu-r11410-10-3-inch-photomultiplier-tube-for-dark-matter-direct-detection-experiments-cross-listing/#comments</comments>
		<pubDate>Tue, 14 Feb 2012 01:56:17 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[50 hz]]></category>
		<category><![CDATA[characterization]]></category>
		<category><![CDATA[conjunction]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[dual phase]]></category>
		<category><![CDATA[hamamatsu]]></category>
		<category><![CDATA[low temperature]]></category>
		<category><![CDATA[photomultiplier tube]]></category>
		<category><![CDATA[photosensor]]></category>
		<category><![CDATA[pmt]]></category>
		<category><![CDATA[quantum efficiency]]></category>
		<category><![CDATA[radioactivity]]></category>
		<category><![CDATA[scintillation]]></category>
		<category><![CDATA[threshold]]></category>
		<category><![CDATA[ucla]]></category>
		<category><![CDATA[wavelength]]></category>
		<category><![CDATA[xenon]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/13/characterization-of-the-hamamatsu-r11410-10-3-inch-photomultiplier-tube-for-dark-matter-direct-detection-experiments-cross-listing/</guid>
		<description><![CDATA[The Hamamatsu R11410-10 PMT has been tested extensively at UCLA and Hamamatsu for use in future ton-scale dual-phase xenon dark matter detectors. The R11410-10 PMT has been shown to have a quantum efficiency of greater than 30% at xenon scintillation wavelengths, a radioactivity of 20.4 mBq/piece and a dark count rate of 50 Hz at [...]]]></description>
			<content:encoded><![CDATA[<p>The Hamamatsu R11410-10 PMT has been tested extensively at UCLA and Hamamatsu for use in future ton-scale dual-phase xenon dark matter detectors. The R11410-10 PMT has been shown to have a quantum efficiency of greater than 30% at xenon scintillation wavelengths, a radioactivity of 20.4 mBq/piece and a dark count rate of 50 Hz at 0.3 photoelectron threshold. These results in conjunction with the high gain (up to 10^7), good single photoelectron resolution and stability at low temperature provide a satisfactory photosensor for the future of low background event searches.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/13/characterization-of-the-hamamatsu-r11410-10-3-inch-photomultiplier-tube-for-dark-matter-direct-detection-experiments-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Discovery &amp; Depth</title>
		<link>http://voxcharta.org/2012/02/13/discovery-depth/</link>
		<comments>http://voxcharta.org/2012/02/13/discovery-depth/#comments</comments>
		<pubDate>Tue, 14 Feb 2012 01:50:01 +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[aspiration]]></category>
		<category><![CDATA[assets]]></category>
		<category><![CDATA[benefit ratio]]></category>
		<category><![CDATA[boundary condition]]></category>
		<category><![CDATA[decade]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[national science foundation]]></category>
		<category><![CDATA[optical astronomy]]></category>
		<category><![CDATA[simple arithmetic]]></category>
		<category><![CDATA[united states]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/13/discovery-depth/</guid>
		<description><![CDATA[In the United States, the National Science Foundation (NSF), anticipating the no growth in funding, has commissioned a review of NSF-funded astronomy assets with the goal of determining how to best allocate funding for this decade. Inputs from members of the US community were sought. It is a matter of simple arithmetic that for a [...]]]></description>
			<content:encoded><![CDATA[<p>In the United States, the National Science Foundation (NSF), anticipating the no growth in funding, has commissioned a review of NSF-funded astronomy assets with the goal of determining how to best allocate funding for this decade. Inputs from members of the US community were sought. It is a matter of simple arithmetic that for a fixed level of funding many significant aspirations of Astro2010 cannot be met. Here, accepting the boundary conditions posed above, I have focused on fields centered on optical astronomy which offer the best opportunity for progress in this decade and thus offer the highest cost-benefit ratio. Readers may profit from reading the first seven sections.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/13/discovery-depth/feed/</wfw:commentRss>
		<slash:comments>1</slash:comments>
		</item>
		<item>
		<title>Astrophysics datamining in the classroom: Exploring real data with new software tools and robotic telescopes [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/13/astrophysics-datamining-in-the-classroom-exploring-real-data-with-new-software-tools-and-robotic-telescopes-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/13/astrophysics-datamining-in-the-classroom-exploring-real-data-with-new-software-tools-and-robotic-telescopes-cross-listing/#comments</comments>
		<pubDate>Tue, 14 Feb 2012 01:48:09 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astronomical image]]></category>
		<category><![CDATA[astronomy]]></category>
		<category><![CDATA[astrophysics]]></category>
		<category><![CDATA[backbone]]></category>
		<category><![CDATA[curricula]]></category>
		<category><![CDATA[electromagnetism]]></category>
		<category><![CDATA[endeavour]]></category>
		<category><![CDATA[exercise]]></category>
		<category><![CDATA[flexibility]]></category>
		<category><![CDATA[gravitational dynamics]]></category>
		<category><![CDATA[high schools]]></category>
		<category><![CDATA[image manipulation]]></category>
		<category><![CDATA[new software tools]]></category>
		<category><![CDATA[nuclear fusion]]></category>
		<category><![CDATA[robotic telescope]]></category>
		<category><![CDATA[salsa]]></category>
		<category><![CDATA[software web]]></category>
		<category><![CDATA[space observatory]]></category>
		<category><![CDATA[target]]></category>
		<category><![CDATA[web tool]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/13/astrophysics-datamining-in-the-classroom-exploring-real-data-with-new-software-tools-and-robotic-telescopes-cross-listing/</guid>
		<description><![CDATA[Within the efforts to bring frontline interactive astrophysics and astronomy to the classroom, the Hands on Universe (HOU) developed a set of exercises and platform using real data obtained by some of the most advanced ground and space observatories. The backbone of this endeavour is a new free software Web tool &#8211; Such a Lovely [...]]]></description>
			<content:encoded><![CDATA[<p>Within the efforts to bring frontline interactive astrophysics and astronomy to the classroom, the Hands on Universe (HOU) developed a set of exercises and platform using real data obtained by some of the most advanced ground and space observatories. The backbone of this endeavour is a new free software Web tool &#8211; Such a Lovely Software for Astronomy based on Image J (Salsa J). It is student-friendly and developed specifically for the HOU project and targets middle and high schools. It allows students to display, analyze, and explore professionally obtained astronomical images, while learning concepts on gravitational dynamics, kinematics, nuclear fusion, electromagnetism. The continuous evolving set of exercises and tutorials is being completed with real (professionally obtained) data to download and detailed tutorials. The flexibility of the Salsa J platform tool enables students and teachers to extend the exercises with their own observations. The software developed for the HOU program has been designed to be a multi-platform, multi-lingual experience for image manipulation and analysis in the classroom. Its design enables easy implementation of new facilities (extensions and plugins), minimal in-situ maintenance and flexibility for exercise plugin. Here, we describe some of the most advanced exercises about astrophysics in the classroom, addressing particular examples on gravitational dynamics, concepts currently introduced in most sciences curricula in middle and high schools.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/13/astrophysics-datamining-in-the-classroom-exploring-real-data-with-new-software-tools-and-robotic-telescopes-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Status of the IceTop air shower array at the South Pole</title>
		<link>http://voxcharta.org/2012/02/13/status-of-the-icetop-air-shower-array-at-the-south-pole/</link>
		<comments>http://voxcharta.org/2012/02/13/status-of-the-icetop-air-shower-array-at-the-south-pole/#comments</comments>
		<pubDate>Tue, 14 Feb 2012 01:47:52 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[array]]></category>
		<category><![CDATA[coincidence]]></category>
		<category><![CDATA[cosmic ray composition]]></category>
		<category><![CDATA[current status]]></category>
		<category><![CDATA[eev]]></category>
		<category><![CDATA[energy range]]></category>
		<category><![CDATA[geographic south pole]]></category>
		<category><![CDATA[IceCube]]></category>
		<category><![CDATA[neutrino observatory]]></category>
		<category><![CDATA[physics results]]></category>
		<category><![CDATA[TeV]]></category>
		<category><![CDATA[underground detector]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/13/status-of-the-icetop-air-shower-array-at-the-south-pole/</guid>
		<description><![CDATA[The IceTop air shower array is the surface component of the IceCube Neutrino Observatory at the geographic South Pole. The combination of IceTop and IceCube provides a new and powerful tool to measure cosmic ray composition in the energy range between about 300 TeV and 1 EeV by detecting the electromagnetic component at the surface [...]]]></description>
			<content:encoded><![CDATA[<p>The IceTop air shower array is the surface component of the IceCube Neutrino Observatory at the geographic South Pole. The combination of IceTop and IceCube provides a new and powerful tool to measure cosmic ray composition in the energy range between about 300 TeV and 1 EeV by detecting the electromagnetic component at the surface in coincidence with the muon bundle in the deep underground detector. The paper will give an overview of the current status of the detector and the first physics results will be presented.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/13/status-of-the-icetop-air-shower-array-at-the-south-pole/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Interactions of exotic particles with ordinary matter [Replacement]</title>
		<link>http://voxcharta.org/2012/02/13/interactions-of-exotic-particles-with-ordinary-matter-replacement/</link>
		<comments>http://voxcharta.org/2012/02/13/interactions-of-exotic-particles-with-ordinary-matter-replacement/#comments</comments>
		<pubDate>Tue, 14 Feb 2012 01:39:02 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[clarification]]></category>
		<category><![CDATA[crystal axes]]></category>
		<category><![CDATA[crystalline silicon]]></category>
		<category><![CDATA[energy loss]]></category>
		<category><![CDATA[evolution of the universe]]></category>
		<category><![CDATA[exotic particles]]></category>
		<category><![CDATA[experimental result]]></category>
		<category><![CDATA[hypothetical particle]]></category>
		<category><![CDATA[massive particle]]></category>
		<category><![CDATA[mechanisms]]></category>
		<category><![CDATA[neutron]]></category>
		<category><![CDATA[nuclear interaction]]></category>
		<category><![CDATA[peculiarity]]></category>
		<category><![CDATA[penetration]]></category>
		<category><![CDATA[quantities]]></category>
		<category><![CDATA[recoil]]></category>
		<category><![CDATA[scenarios]]></category>
		<category><![CDATA[strangelet]]></category>
		<category><![CDATA[wimp]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/13/interactions-of-exotic-particles-with-ordinary-matter-replacement/</guid>
		<description><![CDATA[Weakly interacting massive particles (WIMPs) and strangelets are two classes of &#8220;exotic&#8221; particles not yet discovered, and in agreement with theoretical scenarios most probably produced in different early stages of evolution of the Universe. Some peculiarities of their energy loss in the electronic and nuclear interactions with ordinary matter are investigated. For the direct detection [...]]]></description>
			<content:encoded><![CDATA[<p>Weakly interacting massive particles (WIMPs) and strangelets are two classes of &#8220;exotic&#8221; particles not yet discovered, and in agreement with theoretical scenarios most probably produced in different early stages of evolution of the Universe. Some peculiarities of their energy loss in the electronic and nuclear interactions with ordinary matter are investigated. For the direct detection of WIMPs the signals produced by the stopping of recoils in matter are used for their identification. The influence of the orientation of the recoil in respect to crystal axes for crystalline silicon (as material for detectors) is analysed as average quantities: energy loss, and as transient thermal effects. For strangelets, the mechanisms of picking-up neutrons during their penetration into matter and the effects on electronic and nuclear stopping are considered. The clarification of the aspects related to the stopping of these hypothetical particles in matter will permit a better interpretation of some experimental results and could also contribute to the search for new techniques or materials for their detection, if they exist.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/13/interactions-of-exotic-particles-with-ordinary-matter-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A generalized likelihood ratio test statistic for Cherenkov telescope data [Replacement]</title>
		<link>http://voxcharta.org/2012/02/13/a-generalized-likelihood-ratio-test-statistic-for-cherenkov-telescope-data-replacement/</link>
		<comments>http://voxcharta.org/2012/02/13/a-generalized-likelihood-ratio-test-statistic-for-cherenkov-telescope-data-replacement/#comments</comments>
		<pubDate>Tue, 14 Feb 2012 01:38:32 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[air shower]]></category>
		<category><![CDATA[astrophysical sources]]></category>
		<category><![CDATA[carlo simulations]]></category>
		<category><![CDATA[cherenkov radiation]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[few degrees]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[generalization]]></category>
		<category><![CDATA[likelihood ratio test]]></category>
		<category><![CDATA[numerical test]]></category>
		<category><![CDATA[point spread function]]></category>
		<category><![CDATA[robust test]]></category>
		<category><![CDATA[systematic uncertainty]]></category>
		<category><![CDATA[telescope data]]></category>
		<category><![CDATA[telescope observations]]></category>
		<category><![CDATA[test statistic]]></category>
		<category><![CDATA[tev gamma rays]]></category>
		<category><![CDATA[type instruments]]></category>
		<category><![CDATA[wobble]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/13/a-generalized-likelihood-ratio-test-statistic-for-cherenkov-telescope-data-replacement/</guid>
		<description><![CDATA[Astrophysical sources of TeV gamma rays are usually established by Cherenkov telescope observations. These counting type instruments have a field of view of few degrees in diameter and record large numbers of particle air showers via their Cherenkov radiation in the atmosphere. The showers are either induced by gamma rays or diffuse cosmic ray background. [...]]]></description>
			<content:encoded><![CDATA[<p>Astrophysical sources of TeV gamma rays are usually established by Cherenkov telescope observations. These counting type instruments have a field of view of few degrees in diameter and record large numbers of particle air showers via their Cherenkov radiation in the atmosphere. The showers are either induced by gamma rays or diffuse cosmic ray background. The commonly used test statistic to evaluate a possible gamma-ray excess is Li and Ma (1983), Eq. 17, which can be applied to independent on- and off-source observations, or scenarios that can be approximated as such. This formula however is unsuitable if the data are taken in so-called &#8220;wobble&#8221; mode (pointing to several offset positions around the source), if at the same time the acceptance shape is irregular or even depends on operating parameters such as the pointing direction or telescope multiplicity. To provide a robust test statistic in such cases, this paper explores a possible generalization of the likelihood ratio concept on which the formula of Li and Ma is based. In doing so, the multi-pointing nature of the data and the typically known instrument point spread function are fully exploited to derive a new, semi-numerical test statistic. Due to its flexibility and robustness against systematic uncertainties, it is not only useful for detection purposes, but also for skymapping and source shape fitting. SimplifiedMonte Carlo simulations are presented to verify the results, and several applications and further generalizations of the concept are discussed.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/13/a-generalized-likelihood-ratio-test-statistic-for-cherenkov-telescope-data-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Multiscale probability mapping: groups, clusters and an algorithmic search for filaments in SDSS [Replacement]</title>
		<link>http://voxcharta.org/2012/02/13/multiscale-probability-mapping-groups-clusters-and-an-algorithmic-search-for-filaments-in-sdss-replacement/</link>
		<comments>http://voxcharta.org/2012/02/13/multiscale-probability-mapping-groups-clusters-and-an-algorithmic-search-for-filaments-in-sdss-replacement/#comments</comments>
		<pubDate>Tue, 14 Feb 2012 01:38:09 +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[cluster]]></category>
		<category><![CDATA[cluster environment]]></category>
		<category><![CDATA[density estimation]]></category>
		<category><![CDATA[density field]]></category>
		<category><![CDATA[digital sky survey]]></category>
		<category><![CDATA[dispersion]]></category>
		<category><![CDATA[elongation]]></category>
		<category><![CDATA[filament]]></category>
		<category><![CDATA[galaxy data]]></category>
		<category><![CDATA[galaxy distribution]]></category>
		<category><![CDATA[mapping technique]]></category>
		<category><![CDATA[mpc]]></category>
		<category><![CDATA[radii]]></category>
		<category><![CDATA[sdss]]></category>
		<category><![CDATA[sky survey data]]></category>
		<category><![CDATA[sloan digital]]></category>
		<category><![CDATA[statistic]]></category>
		<category><![CDATA[structure identification]]></category>
		<category><![CDATA[structure size]]></category>
		<category><![CDATA[velocity dispersion]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/13/multiscale-probability-mapping-groups-clusters-and-an-algorithmic-search-for-filaments-in-sdss-replacement/</guid>
		<description><![CDATA[We have developed a multiscale structure identification algorithm for the detection of overdensities in galaxy data that identifies structures having radii within a user-defined range. Our &#8220;multiscale probability mapping&#8221; technique combines density estimation with a shape statistic to identify local peaks in the density field. This technique takes advantage of a user-defined range of scale [...]]]></description>
			<content:encoded><![CDATA[<p>We have developed a multiscale structure identification algorithm for the detection of overdensities in galaxy data that identifies structures having radii within a user-defined range. Our &#8220;multiscale probability mapping&#8221; technique combines density estimation with a shape statistic to identify local peaks in the density field. This technique takes advantage of a user-defined range of scale sizes, which are used in constructing a coarse-grained map of the underlying fine-grained galaxy distribution, from which overdense structures are then identified. In this study we have compiled a catalogue of groups and clusters at 0.025 &lt; z &lt; 0.24 based on the Sloan Digital Sky Survey, Data Release 7, quantifying their significance and comparing with other catalogues. Most measured velocity dispersions for these structures lie between 50 and 400 km/s. A clear trend of increasing velocity dispersion with radius from 0.2 to 1 Mpc/h is detected, confirming the lack of a sharp division between groups and clusters. A method for quantifying elongation is also developed to measure the elongation of group and cluster environments. By using our group and cluster catalogue as a coarse-grained representation of the galaxy distribution for structure sizes of &lt;~ 1 Mpc/h, we identify 53 filaments (from an algorithmically-derived set of 100 candidates) as elongated unions of groups and clusters at 0.025 &lt; z &lt; 0.13. These filaments have morphologies that are consistent with previous samples studied.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/13/multiscale-probability-mapping-groups-clusters-and-an-algorithmic-search-for-filaments-in-sdss-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A New Analysis Method for WIMP searches with Dual-Phase Liquid Xe TPCs [Replacement]</title>
		<link>http://voxcharta.org/2012/02/13/a-new-analysis-method-for-wimp-searches-with-dual-phase-liquid-xe-tpcs-replacement/</link>
		<comments>http://voxcharta.org/2012/02/13/a-new-analysis-method-for-wimp-searches-with-dual-phase-liquid-xe-tpcs-replacement/#comments</comments>
		<pubDate>Tue, 14 Feb 2012 01:31:33 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[background rejection]]></category>
		<category><![CDATA[dark matter search]]></category>
		<category><![CDATA[dual phase]]></category>
		<category><![CDATA[electron]]></category>
		<category><![CDATA[energy resolution]]></category>
		<category><![CDATA[estimators]]></category>
		<category><![CDATA[independent energy]]></category>
		<category><![CDATA[phase space]]></category>
		<category><![CDATA[recoil energy]]></category>
		<category><![CDATA[scintillation light]]></category>
		<category><![CDATA[superior energy]]></category>
		<category><![CDATA[target]]></category>
		<category><![CDATA[tpc]]></category>
		<category><![CDATA[vertex]]></category>
		<category><![CDATA[wimp dark matter]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/13/a-new-analysis-method-for-wimp-searches-with-dual-phase-liquid-xe-tpcs-replacement/</guid>
		<description><![CDATA[A new data analysis method based on physical observables for WIMP dark matter searches with noble liquid Xe dual-phase TPCs is presented. Traditionally, the nuclear recoil energy from a scatter in the liquid target has been estimated by means of the initial prompt scintillation light (S1) produced at the interaction vertex. The ionization charge (C2), [...]]]></description>
			<content:encoded><![CDATA[<p>A new data analysis method based on physical observables for WIMP dark matter searches with noble liquid Xe dual-phase TPCs is presented. Traditionally, the nuclear recoil energy from a scatter in the liquid target has been estimated by means of the initial prompt scintillation light (S1) produced at the interaction vertex. The ionization charge (C2), or its secondary scintillation (S2), is combined with the primary scintillation in Log(S2/S1) vs. S1 only as a discrimination parameter against electron recoil background. Arguments in favor of C2 as the more reliable nuclear recoil energy estimator than S1 are presented. The new phase space of Log(S1/C2) vs. C2 is introduced as more efficient for nuclear recoil acceptance and exhibiting superior energy resolution. This is achieved without compromising the discrimination power of the LXe TPC, nor its 3D event reconstruction and fiducialization capability, as is the case for analyses that exploit only the ionization channel. Finally, the concept of two independent energy estimators for background rejection is presented: E2 as the primary (based on C2) and E1 as the secondary (based on S1). Log(E1/E2) vs. E2 is shown to be the most appropriate phase space in which to evaluate WIMP signal candidates.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/13/a-new-analysis-method-for-wimp-searches-with-dual-phase-liquid-xe-tpcs-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Towards a New Kind of Asteroseismic Grid Fitting</title>
		<link>http://voxcharta.org/2012/02/12/towards-a-new-kind-of-asteroseismic-grid-fitting/</link>
		<comments>http://voxcharta.org/2012/02/12/towards-a-new-kind-of-asteroseismic-grid-fitting/#comments</comments>
		<pubDate>Mon, 13 Feb 2012 01:42:49 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bayesian approach]]></category>
		<category><![CDATA[corot]]></category>
		<category><![CDATA[discrete nature]]></category>
		<category><![CDATA[frequency shift]]></category>
		<category><![CDATA[frequency spectra]]></category>
		<category><![CDATA[kepler]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[main sequence]]></category>
		<category><![CDATA[mode identification]]></category>
		<category><![CDATA[model physics]]></category>
		<category><![CDATA[new ways]]></category>
		<category><![CDATA[probability]]></category>
		<category><![CDATA[random behaviour]]></category>
		<category><![CDATA[recent developments]]></category>
		<category><![CDATA[sequence phase]]></category>
		<category><![CDATA[solar age]]></category>
		<category><![CDATA[stellar pulsation]]></category>
		<category><![CDATA[surface effect]]></category>
		<category><![CDATA[surface layer]]></category>
		<category><![CDATA[systematic error]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/12/towards-a-new-kind-of-asteroseismic-grid-fitting/</guid>
		<description><![CDATA[Recent developments in instrumentation (e.g., in particular the Kepler &#38; CoRoT satellites) provide a new opportunity to improve the models of stellar pulsations. Surface layers, rotation, and magnetic fields imprint erratic frequency shifts, trends, and other non-random behaviour in the frequency spectra. As our observational uncertainties become smaller, these are increasingly important and difficult to [...]]]></description>
			<content:encoded><![CDATA[<p>Recent developments in instrumentation (e.g., in particular the Kepler &amp; CoRoT satellites) provide a new opportunity to improve the models of stellar pulsations. Surface layers, rotation, and magnetic fields imprint erratic frequency shifts, trends, and other non-random behaviour in the frequency spectra. As our observational uncertainties become smaller, these are increasingly important and difficult to deal with using standard fitting techniques. To improve the models, new ways to compare their predictions with observations need to be conceived. In this paper we present a completely probabilistic (Bayesian) approach to asteroseismic model fitting. It allows for varying degrees of prior mode identification, corrections for the discrete nature of the grid, and most importantly implements a treatment of systematic errors, such as the &#8220;surface effects.&#8221; It removes the need to apply semi- empirical corrections to the observations prior to fitting them to the models and results in a consistent set of probabilities with which the model physics can be probed and compared. As an example, we show a detailed asteroseismic analysis of the Sun. We find a most probable solar age, including a 35 +- 5 million year pre-main sequence phase, of 4.591 billion years, and initial element mass fractions of X_0 = 0.72, Y_0 = 0.264, Z_0 = 0.016, consistent with recent asteroseismic and non-asteroseismic studies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/12/towards-a-new-kind-of-asteroseismic-grid-fitting/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Efficiency of a wide-area survey in achieving short- and long-term warning for small impactors [Replacement]</title>
		<link>http://voxcharta.org/2012/02/12/efficiency-of-a-wide-area-survey-in-achieving-short-and-long-term-warning-for-small-impactors-replacement/</link>
		<comments>http://voxcharta.org/2012/02/12/efficiency-of-a-wide-area-survey-in-achieving-short-and-long-term-warning-for-small-impactors-replacement/#comments</comments>
		<pubDate>Mon, 13 Feb 2012 01:39:07 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[asteroids]]></category>
		<category><![CDATA[discovery effort]]></category>
		<category><![CDATA[earth object]]></category>
		<category><![CDATA[efficiency]]></category>
		<category><![CDATA[impactor]]></category>
		<category><![CDATA[mitigation actions]]></category>
		<category><![CDATA[neo discovery]]></category>
		<category><![CDATA[observable sky]]></category>
		<category><![CDATA[population]]></category>
		<category><![CDATA[probability]]></category>
		<category><![CDATA[Telescope]]></category>
		<category><![CDATA[telescopes]]></category>
		<category><![CDATA[tunguska]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/12/efficiency-of-a-wide-area-survey-in-achieving-short-and-long-term-warning-for-small-impactors-replacement/</guid>
		<description><![CDATA[We consider a network of telescopes capable of scanning all the observable sky each night and targeting Near-Earth objects (NEOs) in the size range of the Tunguska-like asteroids, from 160 m down to 10 m. We measure the performance of this telescope network in terms of the time needed to discover at least 50% of [...]]]></description>
			<content:encoded><![CDATA[<p>We consider a network of telescopes capable of scanning all the observable sky each night and targeting Near-Earth objects (NEOs) in the size range of the Tunguska-like asteroids, from 160 m down to 10 m. We measure the performance of this telescope network in terms of the time needed to discover at least 50% of the impactors in the considered population with a warning time large enough to undertake proper mitigation actions. The warning times are described by a trimodal distribution and the telescope network has a 50% probability of discovering an impactor of the Tunguska class with at least one week of advance already in the first 10 yr of operations of the survey. These results suggest that the studied survey would be a significant addition to the current NEO discovery efforts.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/12/efficiency-of-a-wide-area-survey-in-achieving-short-and-long-term-warning-for-small-impactors-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Readout system with on-board demodulation for CMB polarization experiments using coherent polarimeter arrays [Replacement]</title>
		<link>http://voxcharta.org/2012/02/12/readout-system-with-on-board-demodulation-for-cmb-polarization-experiments-using-coherent-polarimeter-arrays-replacement-2/</link>
		<comments>http://voxcharta.org/2012/02/12/readout-system-with-on-board-demodulation-for-cmb-polarization-experiments-using-coherent-polarimeter-arrays-replacement-2/#comments</comments>
		<pubDate>Mon, 13 Feb 2012 01:36:57 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[adc]]></category>
		<category><![CDATA[array]]></category>
		<category><![CDATA[clock]]></category>
		<category><![CDATA[clock modules]]></category>
		<category><![CDATA[cosmic microwave background]]></category>
		<category><![CDATA[demodulation]]></category>
		<category><![CDATA[generic strategy]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[master clock]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[modes]]></category>
		<category><![CDATA[modula]]></category>
		<category><![CDATA[modulation]]></category>
		<category><![CDATA[polarimeter]]></category>
		<category><![CDATA[polarization]]></category>
		<category><![CDATA[signature]]></category>
		<category><![CDATA[smoking gun]]></category>
		<category><![CDATA[statistic]]></category>
		<category><![CDATA[system component]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/12/readout-system-with-on-board-demodulation-for-cmb-polarization-experiments-using-coherent-polarimeter-arrays-replacement-2/</guid>
		<description><![CDATA[B-modes are special patterns in cosmic microwave background (CMB) polarization. The detection of them is a smoking-gun signature of primordial gravitational waves. The generic strategy of the CMB polarization experiments is to employ a large number of polarimeters for improving the statistics. The Q/U Imaging ExperimenT-II (QUIET-II) has been proposed to detect the B-modes using [...]]]></description>
			<content:encoded><![CDATA[<p>B-modes are special patterns in cosmic microwave background (CMB) polarization. The detection of them is a smoking-gun signature of primordial gravitational waves. The generic strategy of the CMB polarization experiments is to employ a large number of polarimeters for improving the statistics. The Q/U Imaging ExperimenT-II (QUIET-II) has been proposed to detect the B-modes using the world&#8217;s largest coherent polarimeter array (2,000 channels). An unique detection technique using QUIET&#8217;s polarimeters, which is a modula- tion/demodulation scheme, enables us directly extracting the polarization signal. The extracted signal is free from non- polarized components and intrinsic 1/f noise. We developed a data readout system with on-board demodulation functions for the QUIET-II experiment. We employed a &#8220;master&#8221; clock strategy. This strategy guarantees phase matching between the modulation by the polarimeters and the demodulation by ADC modules. The single master generates all carrier clocks and distributes them to each module. The developed electronics, clock modules, and the ADC modules fulfill requirements. Tests with a setup similar to that of the real experiment proved that the system works properly. The performance of all system components are validated to be suitable for B-mode measurements.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/12/readout-system-with-on-board-demodulation-for-cmb-polarization-experiments-using-coherent-polarimeter-arrays-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The KELT-South Telescope</title>
		<link>http://voxcharta.org/2012/02/09/the-kelt-south-telescope/</link>
		<comments>http://voxcharta.org/2012/02/09/the-kelt-south-telescope/#comments</comments>
		<pubDate>Fri, 10 Feb 2012 01:56:11 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[aperture]]></category>
		<category><![CDATA[automated telescope]]></category>
		<category><![CDATA[bright star]]></category>
		<category><![CDATA[degree field]]></category>
		<category><![CDATA[hot jupiters]]></category>
		<category><![CDATA[kelt]]></category>
		<category><![CDATA[main sequence star]]></category>
		<category><![CDATA[south africa]]></category>
		<category><![CDATA[southern sky]]></category>
		<category><![CDATA[sutherland]]></category>
		<category><![CDATA[system hardware]]></category>
		<category><![CDATA[target]]></category>
		<category><![CDATA[transiting planet]]></category>
		<category><![CDATA[transits]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/09/the-kelt-south-telescope/</guid>
		<description><![CDATA[The Kilodegree Extremely Little Telescope (KELT) project is a survey for new transiting planets around bright stars. KELT-South is a small-aperture, wide-field automated telescope located at Sutherland, South Africa. The telescope surveys a set of 26 degree by 26 degree fields around the southern sky, and targets stars in the range of 8 &#60; V [...]]]></description>
			<content:encoded><![CDATA[<p>The Kilodegree Extremely Little Telescope (KELT) project is a survey for new transiting planets around bright stars. KELT-South is a small-aperture, wide-field automated telescope located at Sutherland, South Africa. The telescope surveys a set of 26 degree by 26 degree fields around the southern sky, and targets stars in the range of 8 &lt; V &lt; 10 mag, searching for transits by Hot Jupiters. This paper describes the KELT-South system hardware and software and discusses the quality of the observations. We show that KELT-South is able to achieve the necessary photometric precision to detect transits of Hot Jupiters around solar-type main-sequence stars.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/09/the-kelt-south-telescope/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Generation of a 650 nm &#8211; 2000 nm Laser Frequency Comb based on an Erbium-Doped Fiber Laser [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/09/generation-of-a-650-nm-2000-nm-laser-frequency-comb-based-on-an-erbium-doped-fiber-laser-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/09/generation-of-a-650-nm-2000-nm-laser-frequency-comb-based-on-an-erbium-doped-fiber-laser-cross-listing/#comments</comments>
		<pubDate>Fri, 10 Feb 2012 01:53:55 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[amplification]]></category>
		<category><![CDATA[bandwidth]]></category>
		<category><![CDATA[coherence]]></category>
		<category><![CDATA[comb]]></category>
		<category><![CDATA[erbium doped fiber laser]]></category>
		<category><![CDATA[fiber extension]]></category>
		<category><![CDATA[interferometry]]></category>
		<category><![CDATA[laser frequency]]></category>
		<category><![CDATA[laser light]]></category>
		<category><![CDATA[pulses]]></category>
		<category><![CDATA[terahertz]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/09/generation-of-a-650-nm-2000-nm-laser-frequency-comb-based-on-an-erbium-doped-fiber-laser-cross-listing/</guid>
		<description><![CDATA[We present a laser frequency comb based upon a 250 MHz mode-locked erbium-doped fiber laser that spans more than 300 terahertz of bandwidth, from 660 nm to 2000 nm. The system generates 1.2 nJ, 70 fs pulses at 1050 nm by amplifying the 1580 nm laser light in Er:fiber, followed by nonlinear broadening to 1050 [...]]]></description>
			<content:encoded><![CDATA[<p>We present a laser frequency comb based upon a 250 MHz mode-locked erbium-doped fiber laser that spans more than 300 terahertz of bandwidth, from 660 nm to 2000 nm. The system generates 1.2 nJ, 70 fs pulses at 1050 nm by amplifying the 1580 nm laser light in Er:fiber, followed by nonlinear broadening to 1050 nm and amplification in Yb:fiber. Extension of the frequency comb into the visible is achieved by supercontinuum generation from the 1050 nm light. Comb coherence is verified with cascaded f-2f interferometry and comparison to a frequency stabilized laser.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/09/generation-of-a-650-nm-2000-nm-laser-frequency-comb-based-on-an-erbium-doped-fiber-laser-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A New Analysis Method for WIMP searches with Dual-Phase Liquid Xe TPCs</title>
		<link>http://voxcharta.org/2012/02/09/a-new-analysis-method-for-wimp-searches-with-dual-phase-liquid-xe-tpcs/</link>
		<comments>http://voxcharta.org/2012/02/09/a-new-analysis-method-for-wimp-searches-with-dual-phase-liquid-xe-tpcs/#comments</comments>
		<pubDate>Fri, 10 Feb 2012 01:50:05 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[background rejection]]></category>
		<category><![CDATA[dark matter search]]></category>
		<category><![CDATA[dual phase]]></category>
		<category><![CDATA[electron]]></category>
		<category><![CDATA[energy resolution]]></category>
		<category><![CDATA[estimators]]></category>
		<category><![CDATA[independent energy]]></category>
		<category><![CDATA[phase space]]></category>
		<category><![CDATA[recoil energy]]></category>
		<category><![CDATA[scintillation light]]></category>
		<category><![CDATA[superior energy]]></category>
		<category><![CDATA[target]]></category>
		<category><![CDATA[tpc]]></category>
		<category><![CDATA[vertex]]></category>
		<category><![CDATA[wimp dark matter]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/09/a-new-analysis-method-for-wimp-searches-with-dual-phase-liquid-xe-tpcs/</guid>
		<description><![CDATA[A new data analysis method based on physical observables for WIMP dark matter searches with noble liquid Xe dual-phase TPCs is presented. Traditionally, the nuclear recoil energy from a scatter in the liquid target has been estimated by means of the initial prompt scintillation light (S1) produced at the interaction vertex. The ionization charge (C2), [...]]]></description>
			<content:encoded><![CDATA[<p>A new data analysis method based on physical observables for WIMP dark matter searches with noble liquid Xe dual-phase TPCs is presented. Traditionally, the nuclear recoil energy from a scatter in the liquid target has been estimated by means of the initial prompt scintillation light (S1) produced at the interaction vertex. The ionization charge (C2), or its secondary scintillation (S2), is combined with the primary scintillation in Log(S2/S1) vs. S1 only as a discrimination parameter against electron recoil background. Arguments in favor of C2 as the more reliable nuclear recoil energy estimator than S1 are presented. The new phase space of Log(S1/C2) vs. C2 is introduced as more e?cient for nuclear recoil acceptance and exhibiting superior energy resolution. This is achieved without compromising the discrimination power of the LXe TPC, nor its 3D event reconstruction and ?ducialization capability, as is the case for analyses that exploit only the ionization channel. Finally, the concept of two independent energy estimators for background rejection is presented: E2 as the primary (based on C2) and E1 as the secondary (based on S1). Log(E1/E2) vs. E2 is shown to be the most appropriate phase space in which to evaluate WIMP signal candidates.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/09/a-new-analysis-method-for-wimp-searches-with-dual-phase-liquid-xe-tpcs/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Calibration of Photomultiplier Tubes for the Fluorescence Detector of Telescope Array Experiment using a Rayleigh Scattered Laser Beam</title>
		<link>http://voxcharta.org/2012/02/09/calibration-of-photomultiplier-tubes-for-the-fluorescence-detector-of-telescope-array-experiment-using-a-rayleigh-scattered-laser-beam/</link>
		<comments>http://voxcharta.org/2012/02/09/calibration-of-photomultiplier-tubes-for-the-fluorescence-detector-of-telescope-array-experiment-using-a-rayleigh-scattered-laser-beam/#comments</comments>
		<pubDate>Fri, 10 Feb 2012 01:48:44 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[calibration]]></category>
		<category><![CDATA[experimental setup]]></category>
		<category><![CDATA[laser beam]]></category>
		<category><![CDATA[measurement procedure]]></category>
		<category><![CDATA[nitrogen laser]]></category>
		<category><![CDATA[photomultiplier tube]]></category>
		<category><![CDATA[photon]]></category>
		<category><![CDATA[pmt]]></category>
		<category><![CDATA[readout electronics]]></category>
		<category><![CDATA[systematic uncertainty]]></category>
		<category><![CDATA[telescope array]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/09/calibration-of-photomultiplier-tubes-for-the-fluorescence-detector-of-telescope-array-experiment-using-a-rayleigh-scattered-laser-beam/</guid>
		<description><![CDATA[We performed photometric calibration of the PhotoMultiplier Tube (PMT) and readout electronics used for the new fluorescence detectors of the Telescope Array (TA) experiment using Rayleigh scattered photons from a pulsed nitrogen laser beam. The experimental setup, measurement procedure, and results of calibration are described. The total systematic uncertainty of the calibration is estimated to [...]]]></description>
			<content:encoded><![CDATA[<p>We performed photometric calibration of the PhotoMultiplier Tube (PMT) and readout electronics used for the new fluorescence detectors of the Telescope Array (TA) experiment using Rayleigh scattered photons from a pulsed nitrogen laser beam. The experimental setup, measurement procedure, and results of calibration are described. The total systematic uncertainty of the calibration is estimated to be 7.5%. An additional uncertainty of 3.7% is introduced by the transport of the calibrated PMTs from the laboratory to the TA experimental site.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/09/calibration-of-photomultiplier-tubes-for-the-fluorescence-detector-of-telescope-array-experiment-using-a-rayleigh-scattered-laser-beam/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Fast Integrated Spectra Analyzer: A New Computational Tool For Age and Reddening Determination of Small Angular Diameter Open Clusters</title>
		<link>http://voxcharta.org/2012/02/09/fast-integrated-spectra-analyzer-a-new-computational-tool-for-age-and-reddening-determination-of-small-angular-diameter-open-clusters/</link>
		<comments>http://voxcharta.org/2012/02/09/fast-integrated-spectra-analyzer-a-new-computational-tool-for-age-and-reddening-determination-of-small-angular-diameter-open-clusters/#comments</comments>
		<pubDate>Fri, 10 Feb 2012 01:47:06 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[aa range]]></category>
		<category><![CDATA[angular diameter]]></category>
		<category><![CDATA[basic assumption]]></category>
		<category><![CDATA[computational tool]]></category>
		<category><![CDATA[determinations]]></category>
		<category><![CDATA[fisa]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[implementation]]></category>
		<category><![CDATA[libraries]]></category>
		<category><![CDATA[magellanic cloud]]></category>
		<category><![CDATA[numerical algorithm]]></category>
		<category><![CDATA[open cluster]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectroscopic technique]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[spectrum]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/09/fast-integrated-spectra-analyzer-a-new-computational-tool-for-age-and-reddening-determination-of-small-angular-diameter-open-clusters/</guid>
		<description><![CDATA[We present a new algorithm called &#8216;Fast Integrated Spectra Analyzer&#8221; (FISA) that permits fast and reasonably accurate age and reddening determinations for small angular diameter open clusters by using their integrated spectra in the (3600-7400) \AA \ range and currently available template spectrum libraries. This algorithm and its implementation help to achieve astrophysical results in [...]]]></description>
			<content:encoded><![CDATA[<p>We present a new algorithm called &#8216;Fast Integrated Spectra Analyzer&#8221; (FISA) that permits fast and reasonably accurate age and reddening determinations for small angular diameter open clusters by using their integrated spectra in the (3600-7400) \AA \ range and currently available template spectrum libraries. This algorithm and its implementation help to achieve astrophysical results in shorter times than from other methods. A brief review is given of the integrated spectroscopic technique applied to the study of open clusters as well as the basic assumptions that justify its use. We describe the numerical algorithm employed in detail, show examples of its application, and provide a link to the code. Our method has successfully been applied to integrated spectroscopy of open clusters, both in the Galaxy and in the Magellanic Clouds, to determine ages and reddenings.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/09/fast-integrated-spectra-analyzer-a-new-computational-tool-for-age-and-reddening-determination-of-small-angular-diameter-open-clusters/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Likelihood Ratio as a tool for Radio Continuum Surveys with SKA precursor telescopes</title>
		<link>http://voxcharta.org/2012/02/09/the-likelihood-ratio-as-a-tool-for-radio-continuum-surveys-with-ska-precursor-telescopes/</link>
		<comments>http://voxcharta.org/2012/02/09/the-likelihood-ratio-as-a-tool-for-radio-continuum-surveys-with-ska-precursor-telescopes/#comments</comments>
		<pubDate>Fri, 10 Feb 2012 01:46:52 +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[baseline]]></category>
		<category><![CDATA[catalogues]]></category>
		<category><![CDATA[completeness]]></category>
		<category><![CDATA[counterpart]]></category>
		<category><![CDATA[hemisphere]]></category>
		<category><![CDATA[infrared data]]></category>
		<category><![CDATA[likelihood ratio]]></category>
		<category><![CDATA[map]]></category>
		<category><![CDATA[meerkat]]></category>
		<category><![CDATA[pathfinder]]></category>
		<category><![CDATA[peak flux]]></category>
		<category><![CDATA[precursor]]></category>
		<category><![CDATA[radio catalogue]]></category>
		<category><![CDATA[radio continuum]]></category>
		<category><![CDATA[radio observation]]></category>
		<category><![CDATA[radio source]]></category>
		<category><![CDATA[ratio method]]></category>
		<category><![CDATA[telescopes]]></category>
		<category><![CDATA[video survey]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/09/the-likelihood-ratio-as-a-tool-for-radio-continuum-surveys-with-ska-precursor-telescopes/</guid>
		<description><![CDATA[In this paper we investigate the performance of the likelihood ratio method as a tool for identifying optical and infrared counterparts to proposed radio continuum surveys with SKA precursor and pathfinder telescopes. We present a comparison of the infrared counterparts identified by the likelihood ratio in the VISTA Deep Extragalactic Observations (VIDEO) survey to radio [...]]]></description>
			<content:encoded><![CDATA[<p>In this paper we investigate the performance of the likelihood ratio method as a tool for identifying optical and infrared counterparts to proposed radio continuum surveys with SKA precursor and pathfinder telescopes. We present a comparison of the infrared counterparts identified by the likelihood ratio in the VISTA Deep Extragalactic Observations (VIDEO) survey to radio observations with 6, 10 and 15 arcsec resolution. We cross-match a deep radio catalogue consisting of radio sources with peak flux density $&gt;$ 60 $\mu$Jy with deep near-infrared data limited to $K_{\mathrm{s}}\lesssim$ 22.6. Comparing the infrared counterparts from this procedure to those obtained when cross-matching a set of simulated lower resolution radio catalogues indicates that degrading the resolution from 6 arcsec to 10 and 15 arcsec decreases the completeness of the cross-matched catalogue by approximately 3 and 7 percent respectively. When matching against shallower infrared data, comparable to that achieved by the VISTA Hemisphere Survey, the fraction of radio sources with reliably identified counterparts drops from $\sim$89%, at $K_{\mathrm{s}}\lesssim$22.6, to 47% with $K_{\mathrm{s}}\lesssim$20.0. Decreasing the resolution at this shallower infrared limit does not result in any further decrease in the completeness produced by the likelihood ratio matching procedure. However, we note that radio continuum surveys with the MeerKAT and eventually the SKA, will require long baselines in order to ensure that the resulting maps are not limited by instrumental confusion noise.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/09/the-likelihood-ratio-as-a-tool-for-radio-continuum-surveys-with-ska-precursor-telescopes/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Building a Model Astrolabe</title>
		<link>http://voxcharta.org/2012/02/09/building-a-model-astrolabe/</link>
		<comments>http://voxcharta.org/2012/02/09/building-a-model-astrolabe/#comments</comments>
		<pubDate>Fri, 10 Feb 2012 01:45:22 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astrolabe]]></category>
		<category><![CDATA[deg]]></category>
		<category><![CDATA[file archive]]></category>
		<category><![CDATA[images]]></category>
		<category><![CDATA[latitude]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[scripts]]></category>
		<category><![CDATA[single model]]></category>
		<category><![CDATA[vector graphics]]></category>
		<category><![CDATA[working model]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/09/building-a-model-astrolabe/</guid>
		<description><![CDATA[This paper presents a hands-on introduction to the medieval astrolabe, based around a working model which can be constructed from photocopies of the supplied figures. As well as describing how to assemble the model, I also provide a brief explanation of how each of its various parts might be used. The printed version of this [...]]]></description>
			<content:encoded><![CDATA[<p>This paper presents a hands-on introduction to the medieval astrolabe, based around a working model which can be constructed from photocopies of the supplied figures. As well as describing how to assemble the model, I also provide a brief explanation of how each of its various parts might be used. The printed version of this paper includes only the parts needed to build a single model prepared for use at latitudes around 52{\deg}N, but an accompanying electronic file archive includes equivalent images which can be used to build models prepared for use at any other latitude. The vector graphics scripts used to generate the models are also available for download, allowing customised astrolabes to be made.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/09/building-a-model-astrolabe/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>From Hipparcos to Gaia</title>
		<link>http://voxcharta.org/2012/02/09/from-hipparcos-to-gaia/</link>
		<comments>http://voxcharta.org/2012/02/09/from-hipparcos-to-gaia/#comments</comments>
		<pubDate>Fri, 10 Feb 2012 01:42:40 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accuracy]]></category>
		<category><![CDATA[astronomical knowledge]]></category>
		<category><![CDATA[astrophysics]]></category>
		<category><![CDATA[celestial object]]></category>
		<category><![CDATA[constituent]]></category>
		<category><![CDATA[cornerstone mission]]></category>
		<category><![CDATA[distance]]></category>
		<category><![CDATA[eighties]]></category>
		<category><![CDATA[gaia]]></category>
		<category><![CDATA[hipparcos satellite]]></category>
		<category><![CDATA[hundred times]]></category>
		<category><![CDATA[motion]]></category>
		<category><![CDATA[one billion]]></category>
		<category><![CDATA[planets]]></category>
		<category><![CDATA[position accuracy]]></category>
		<category><![CDATA[solar system]]></category>
		<category><![CDATA[space mission]]></category>
		<category><![CDATA[spectroscopic data]]></category>
		<category><![CDATA[star number]]></category>
		<category><![CDATA[variability]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/09/from-hipparcos-to-gaia/</guid>
		<description><![CDATA[The measurement of the positions, distances, motions and luminosities of stars represents the foundations of modern astronomical knowledge. Launched at the end of the eighties, the ESA Hipparcos satellite was the first space mission dedicated to such measurements. Hipparcos improved position accuracies by a factor of 100 compared to typical ground-based results and provided astrometric [...]]]></description>
			<content:encoded><![CDATA[<p>The measurement of the positions, distances, motions and luminosities of stars represents the foundations of modern astronomical knowledge. Launched at the end of the eighties, the ESA Hipparcos satellite was the first space mission dedicated to such measurements. Hipparcos improved position accuracies by a factor of 100 compared to typical ground-based results and provided astrometric and photometric multi-epoch observations of 118,000 stars over the entire sky. The impact of Hipparcos on astrophysics has been extremely valuable and diverse. Building on this important European success, the ESA Gaia cornerstone mission promises an even more impressive advance. Compared to Hipparcos, it will bring a gain of a factor 50 to 100 in position accuracy and of a factor of 10,000 in star number, collecting photometric, spectrophotometric and spectroscopic data for one billion celestial objects. During its 5-year flight, Gaia will measure objects repeatedly, up to a few hundred times, providing an unprecedented database to study the variability of all types of celestial objects. Gaia will bring outstanding contributions, directly or indirectly, to most fields of research in astrophysics, such as the study of our Galaxy and of its stellar constituents, the search for planets outside the solar system.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/09/from-hipparcos-to-gaia/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>IONORT: a Windows software tool to calculate the HF ray tracing in the ionosphere [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/09/ionort-a-windows-software-tool-to-calculate-the-hf-ray-tracing-in-the-ionosphere-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/09/ionort-a-windows-software-tool-to-calculate-the-hf-ray-tracing-in-the-ionosphere-cross-listing/#comments</comments>
		<pubDate>Fri, 10 Feb 2012 01:42:12 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[coordinates]]></category>
		<category><![CDATA[data input]]></category>
		<category><![CDATA[dependent variable]]></category>
		<category><![CDATA[dimensional electron]]></category>
		<category><![CDATA[dimensional visualization]]></category>
		<category><![CDATA[electron]]></category>
		<category><![CDATA[electron density]]></category>
		<category><![CDATA[first order differential equation]]></category>
		<category><![CDATA[frequency waves]]></category>
		<category><![CDATA[graphical user interface]]></category>
		<category><![CDATA[high frequency]]></category>
		<category><![CDATA[independent variable]]></category>
		<category><![CDATA[input output]]></category>
		<category><![CDATA[ionosphere]]></category>
		<category><![CDATA[neutral particle]]></category>
		<category><![CDATA[numerical data]]></category>
		<category><![CDATA[software tool]]></category>
		<category><![CDATA[wave vector]]></category>
		<category><![CDATA[windows operating systems]]></category>
		<category><![CDATA[windows software]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/09/ionort-a-windows-software-tool-to-calculate-the-hf-ray-tracing-in-the-ionosphere-cross-listing/</guid>
		<description><![CDATA[This paper describes an applicative software tool, named IONORT (IONOspheric Ray Tracing), for calculating a three-dimensional ray tracing of high frequency waves in the ionospheric medium. This tool runs under Windows operating systems and its friendly graphical user interface facilitates both the numerical data input/output and the two/three-dimensional visualization of the ray path. In order [...]]]></description>
			<content:encoded><![CDATA[<p>This paper describes an applicative software tool, named IONORT (IONOspheric Ray Tracing), for calculating a three-dimensional ray tracing of high frequency waves in the ionospheric medium. This tool runs under Windows operating systems and its friendly graphical user interface facilitates both the numerical data input/output and the two/three-dimensional visualization of the ray path. In order to calculate the coordinates of the ray and the three components of the wave vector along the path as dependent variables, the core of the program solves a system of six first order differential equations, the group path being the independent variable of integration. IONORT uses a three-dimensional electron density specification of the ionosphere, as well as by geomagnetic field and neutral particles-electrons collision frequency models having validity in the area of interest.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/09/ionort-a-windows-software-tool-to-calculate-the-hf-ray-tracing-in-the-ionosphere-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Needlet-Whittle Estimates on the Unit Sphere [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/09/needlet-whittle-estimates-on-the-unit-sphere-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/09/needlet-whittle-estimates-on-the-unit-sphere-cross-listing/#comments</comments>
		<pubDate>Fri, 10 Feb 2012 01:34:22 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[asymptotic behaviour]]></category>
		<category><![CDATA[asymptotic results]]></category>
		<category><![CDATA[consistency]]></category>
		<category><![CDATA[fourier analysis]]></category>
		<category><![CDATA[frequency limit]]></category>
		<category><![CDATA[high frequency]]></category>
		<category><![CDATA[maximum likelihood estimator]]></category>
		<category><![CDATA[monte carlo study]]></category>
		<category><![CDATA[random field]]></category>
		<category><![CDATA[spectral parameters]]></category>
		<category><![CDATA[unit sphere]]></category>
		<category><![CDATA[whittle]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/09/needlet-whittle-estimates-on-the-unit-sphere-cross-listing/</guid>
		<description><![CDATA[We study the asymptotic behaviour of needlets-based approximate maximum likelihood estimators for the spectral parameters of Gaussian and isotropic spherical random fields. We prove consistency and asymptotic Gaussianity, in the high-frequency limit, thus generalizing earlier results by Durastanti et al. (2011) based upon standard Fourier analysis on the sphere. The asymptotic results are then illustrated [...]]]></description>
			<content:encoded><![CDATA[<p>We study the asymptotic behaviour of needlets-based approximate maximum likelihood estimators for the spectral parameters of Gaussian and isotropic spherical random fields. We prove consistency and asymptotic Gaussianity, in the high-frequency limit, thus generalizing earlier results by Durastanti et al. (2011) based upon standard Fourier analysis on the sphere. The asymptotic results are then illustrated by an extensive Monte Carlo study.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/09/needlet-whittle-estimates-on-the-unit-sphere-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>MEMS practice, from the lab to the telescope</title>
		<link>http://voxcharta.org/2012/02/08/mems-practice-from-the-lab-to-the-telescope/</link>
		<comments>http://voxcharta.org/2012/02/08/mems-practice-from-the-lab-to-the-telescope/#comments</comments>
		<pubDate>Thu, 09 Feb 2012 01:53:10 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astronomical adaptive optics]]></category>
		<category><![CDATA[decade]]></category>
		<category><![CDATA[economy]]></category>
		<category><![CDATA[end users]]></category>
		<category><![CDATA[imager]]></category>
		<category><![CDATA[maturity]]></category>
		<category><![CDATA[micro electro mechanical systems]]></category>
		<category><![CDATA[open loop control]]></category>
		<category><![CDATA[sky]]></category>
		<category><![CDATA[Telescope]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/08/mems-practice-from-the-lab-to-the-telescope/</guid>
		<description><![CDATA[Micro-electro-mechanical systems (MEMS) technology can provide for deformable mirrors (DMs) with excellent performance within a favorable economy of scale. Large MEMS-based astronomical adaptive optics (AO) systems such as the Gemini Planet Imager are coming on-line soon. As MEMS DM end-users, we discuss our decade of practice with the micromirrors, from inspecting and characterizing devices to [...]]]></description>
			<content:encoded><![CDATA[<p>Micro-electro-mechanical systems (MEMS) technology can provide for deformable mirrors (DMs) with excellent performance within a favorable economy of scale. Large MEMS-based astronomical adaptive optics (AO) systems such as the Gemini Planet Imager are coming on-line soon. As MEMS DM end-users, we discuss our decade of practice with the micromirrors, from inspecting and characterizing devices to evaluating their performance in the lab. We also show MEMS wavefront correction on-sky with the &#8220;Villages&#8221; AO system on a 1-m telescope, including open-loop control and visible-light imaging. Our work demonstrates the maturity of MEMS technology for astronomical adaptive optics.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/08/mems-practice-from-the-lab-to-the-telescope/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Genetic algorithms in astronomy and astrophysics</title>
		<link>http://voxcharta.org/2012/02/08/genetic-algorithms-in-astronomy-and-astrophysics/</link>
		<comments>http://voxcharta.org/2012/02/08/genetic-algorithms-in-astronomy-and-astrophysics/#comments</comments>
		<pubDate>Thu, 09 Feb 2012 01:49:22 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astronomy and astrophysics]]></category>
		<category><![CDATA[biological evolution]]></category>
		<category><![CDATA[genetic algorithm]]></category>
		<category><![CDATA[optimisation problems]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/08/genetic-algorithms-in-astronomy-and-astrophysics/</guid>
		<description><![CDATA[Genetic algorithms (GAs) emulate the process of biological evolution, in a computational setting, in order to generate good solutions to difficult search and optimisation problems. GA-based optimisers tend to be extremely robust and versatile compared to most traditional techniques used to solve optimisation problems. This review paper provides a very brief introduction to GAs and [...]]]></description>
			<content:encoded><![CDATA[<p>Genetic algorithms (GAs) emulate the process of biological evolution, in a computational setting, in order to generate good solutions to difficult search and optimisation problems. GA-based optimisers tend to be extremely robust and versatile compared to most traditional techniques used to solve optimisation problems. This review paper provides a very brief introduction to GAs and outlines their utility in astronomy and astrophysics.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/08/genetic-algorithms-in-astronomy-and-astrophysics/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>XMM-Newton (X-Ray Mulit-Mirror Mission) Observatory</title>
		<link>http://voxcharta.org/2012/02/08/xmm-newton-x-ray-mulit-mirror-mission-observatory/</link>
		<comments>http://voxcharta.org/2012/02/08/xmm-newton-x-ray-mulit-mirror-mission-observatory/#comments</comments>
		<pubDate>Thu, 09 Feb 2012 01:48:14 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astronomy mission]]></category>
		<category><![CDATA[cameras]]></category>
		<category><![CDATA[european space agency]]></category>
		<category><![CDATA[mirror]]></category>
		<category><![CDATA[mulit]]></category>
		<category><![CDATA[observatory]]></category>
		<category><![CDATA[optical telescope]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[payload]]></category>
		<category><![CDATA[ray astronomy]]></category>
		<category><![CDATA[reflecting telescopes]]></category>
		<category><![CDATA[replication technology]]></category>
		<category><![CDATA[space telescope]]></category>
		<category><![CDATA[spectrometer]]></category>
		<category><![CDATA[subject terms]]></category>
		<category><![CDATA[unprecedented combination]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xmm newton]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/08/xmm-newton-x-ray-mulit-mirror-mission-observatory/</guid>
		<description><![CDATA[X-ray Multi-Mirror Mission (XMM-Newton) has been one of the most successful astronomy missions launched by the European Space Agency. It exploits innovative use of replication technology for the X-ray reflecting telescopes that has resulted in an unprecedented combination of effective area and resolution. Three telescopes are equipped with imaging cameras and spectrometers that operate simultaneously, [...]]]></description>
			<content:encoded><![CDATA[<p>X-ray Multi-Mirror Mission (XMM-Newton) has been one of the most successful astronomy missions launched by the European Space Agency. It exploits innovative use of replication technology for the X-ray reflecting telescopes that has resulted in an unprecedented combination of effective area and resolution. Three telescopes are equipped with imaging cameras and spectrometers that operate simultaneously, together with a coaligned optical telescope. The key features of the payload are described, and the in-orbit performance and scientific achievements are summarised. Subject terms or keywords: XMM-Newton, X-ray astronomy, space telescopes</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/08/xmm-newton-x-ray-mulit-mirror-mission-observatory/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Calculating the transfer function of noise removal by principal component analysis and application to AzTEC observations [Replacement]</title>
		<link>http://voxcharta.org/2012/02/08/calculating-the-transfer-function-of-noise-removal-by-principal-component-analysis-and-application-to-aztec-observations-replacement/</link>
		<comments>http://voxcharta.org/2012/02/08/calculating-the-transfer-function-of-noise-removal-by-principal-component-analysis-and-application-to-aztec-observations-replacement/#comments</comments>
		<pubDate>Thu, 09 Feb 2012 01:37:41 +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[array]]></category>
		<category><![CDATA[atacama]]></category>
		<category><![CDATA[bolometer]]></category>
		<category><![CDATA[catalogues]]></category>
		<category><![CDATA[iterative technique]]></category>
		<category><![CDATA[james clerk maxwell]]></category>
		<category><![CDATA[lockman hole]]></category>
		<category><![CDATA[map]]></category>
		<category><![CDATA[noise removal]]></category>
		<category><![CDATA[photometry]]></category>
		<category><![CDATA[point source]]></category>
		<category><![CDATA[principal component analysis]]></category>
		<category><![CDATA[principal component analysis pca]]></category>
		<category><![CDATA[scales]]></category>
		<category><![CDATA[signal]]></category>
		<category><![CDATA[signal to noise]]></category>
		<category><![CDATA[source flux]]></category>
		<category><![CDATA[spatial extent]]></category>
		<category><![CDATA[Telescope]]></category>
		<category><![CDATA[xmm newton]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/08/calculating-the-transfer-function-of-noise-removal-by-principal-component-analysis-and-application-to-aztec-observations-replacement/</guid>
		<description><![CDATA[Instruments using arrays of many bolometers have become increasingly common in the past decade. The maps produced by such instruments typically include the filtering effects of the instrument as well as those from subsequent steps performed in the reduction of the data. Therefore interpretation of the maps is dependent upon accurately calculating the transfer function [...]]]></description>
			<content:encoded><![CDATA[<p>Instruments using arrays of many bolometers have become increasingly common in the past decade. The maps produced by such instruments typically include the filtering effects of the instrument as well as those from subsequent steps performed in the reduction of the data. Therefore interpretation of the maps is dependent upon accurately calculating the transfer function of the chosen reduction technique on the signal of interest. Many of these instruments use non-linear and iterative techniques to reduce their data because such methods can offer improved signal-to-noise over those that are purely linear, particularly for signals at scales comparable to that subtended by the array. We discuss a general approach for measuring the transfer function of principal component analysis (PCA) on point sources that are small compared to the spatial extent seen by any single bolometer within the array. The results are applied to previously released AzTEC catalogues of the COSMOS, Lockman Hole, Subaru XMM-Newton Deep Field, GOODS-North and GOODS-South fields. Source flux density and noise estimates increase by roughly +10 per cent for fields observed while AzTEC was installed at the Atacama Submillimeter Telescope Experiment and +15-25 per cent while AzTEC was installed at the James Clerk Maxwell Telescope. Detection significance is, on average, unaffected by the revised technique. The revised photometry technique will be used in subsequent AzTEC releases.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/08/calculating-the-transfer-function-of-noise-removal-by-principal-component-analysis-and-application-to-aztec-observations-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The XENON100 Dark Matter Experiment [Replacement]</title>
		<link>http://voxcharta.org/2012/02/08/the-xenon100-dark-matter-experiment-replacement/</link>
		<comments>http://voxcharta.org/2012/02/08/the-xenon100-dark-matter-experiment-replacement/#comments</comments>
		<pubDate>Thu, 09 Feb 2012 01:36:14 +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[cm 2]]></category>
		<category><![CDATA[dark matter search]]></category>
		<category><![CDATA[design goal]]></category>
		<category><![CDATA[first science]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[laboratori nazionali del gran sasso]]></category>
		<category><![CDATA[liquid xenon]]></category>
		<category><![CDATA[lngs]]></category>
		<category><![CDATA[lxe]]></category>
		<category><![CDATA[massive particle]]></category>
		<category><![CDATA[matter experiment]]></category>
		<category><![CDATA[photomultiplier tube]]></category>
		<category><![CDATA[radiation shield]]></category>
		<category><![CDATA[radioactivity]]></category>
		<category><![CDATA[recoil]]></category>
		<category><![CDATA[stainless steel vessel]]></category>
		<category><![CDATA[target]]></category>
		<category><![CDATA[time projection chamber]]></category>
		<category><![CDATA[ultimate design]]></category>
		<category><![CDATA[wimp]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/08/the-xenon100-dark-matter-experiment-replacement/</guid>
		<description><![CDATA[The XENON100 dark matter experiment uses liquid xenon (LXe) in a time projection chamber (TPC) to search for Xe nuclear recoils resulting from the scattering of dark matter Weakly Interacting Massive Particles (WIMPs). In this paper we present a detailed description of the detector design and present performance results, as established during the commissioning phase [...]]]></description>
			<content:encoded><![CDATA[<p>The XENON100 dark matter experiment uses liquid xenon (LXe) in a time projection chamber (TPC) to search for Xe nuclear recoils resulting from the scattering of dark matter Weakly Interacting Massive Particles (WIMPs). In this paper we present a detailed description of the detector design and present performance results, as established during the commissioning phase and during the first science runs.   The active target of XENON100 contains 62 kg of LXe, surrounded by an LXe veto of 99 kg, both instrumented with photomultiplier tubes (PMTs) operating inside the liquid or in Xe gas. The LXe target and veto are contained in a low-radioactivity stainless steel vessel, embedded in a passive radiation shield. The experiment is installed underground at the Laboratori Nazionali del Gran Sasso (LNGS), Italy and has recently published results from a 100 live-days dark matter search. The ultimate design goal of XENON100 is to achieve a spin-independent WIMP-nucleon scattering cross section sensitivity of \sigma = 2&#215;10^-45 cm^2 for a 100 GeV/c^2 WIMP.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/08/the-xenon100-dark-matter-experiment-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Review Article: Physics and Monte Carlo Techniques as Relevant to Cryogenic, Phonon and Ionization Readout of CDMS Radiation-Detectors [Replacement]</title>
		<link>http://voxcharta.org/2012/02/08/review-article-physics-and-monte-carlo-techniques-as-relevant-to-cryogenic-phonon-and-ionization-readout-of-cdms-radiation-detectors-replacement/</link>
		<comments>http://voxcharta.org/2012/02/08/review-article-physics-and-monte-carlo-techniques-as-relevant-to-cryogenic-phonon-and-ionization-readout-of-cdms-radiation-detectors-replacement/#comments</comments>
		<pubDate>Thu, 09 Feb 2012 01:34:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[band structure]]></category>
		<category><![CDATA[charge transport]]></category>
		<category><![CDATA[circuit description]]></category>
		<category><![CDATA[cryogenic dark matter]]></category>
		<category><![CDATA[cumulative distribution function]]></category>
		<category><![CDATA[cumulative distribution function cdf]]></category>
		<category><![CDATA[dark matter search]]></category>
		<category><![CDATA[detector physics]]></category>
		<category><![CDATA[numerical constant]]></category>
		<category><![CDATA[phase separation]]></category>
		<category><![CDATA[phonon]]></category>
		<category><![CDATA[phonon transport]]></category>
		<category><![CDATA[radiation detector]]></category>
		<category><![CDATA[sampling method]]></category>
		<category><![CDATA[superconducting films]]></category>
		<category><![CDATA[superconducting phase]]></category>
		<category><![CDATA[thermal diffusion]]></category>
		<category><![CDATA[thermal processes]]></category>
		<category><![CDATA[transport physics]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/08/review-article-physics-and-monte-carlo-techniques-as-relevant-to-cryogenic-phonon-and-ionization-readout-of-cdms-radiation-detectors-replacement/</guid>
		<description><![CDATA[This review discusses detector physics and Monte Carlo techniques for cryogenic, radiation detectors that utilize combined phonon and ionization readout. A general review of cryogenic phonon and charge transport is provided along with specific details of the Cryogenic Dark Matter Search detector instrumentation. In particular this review covers quasidiffusive phonon transport, which includes phonon focusing, [...]]]></description>
			<content:encoded><![CDATA[<p>This review discusses detector physics and Monte Carlo techniques for cryogenic, radiation detectors that utilize combined phonon and ionization readout. A general review of cryogenic phonon and charge transport is provided along with specific details of the Cryogenic Dark Matter Search detector instrumentation. In particular this review covers quasidiffusive phonon transport, which includes phonon focusing, anharmonic decay and isotope scattering. The interaction of phonons in the detector surface is discussed along with the downconversion of phonons in superconducting films. The charge transport physics include a mass tensor which results from the crystal band structure and is modeled with a Herring Vogt transformation. Charge scattering processes involve the creation of Neganov-Luke phonons. Transition-edge-sensor (TES) simulations include a full electric circuit description and all thermal processes including Joule heating, cooling to the substrate and thermal diffusion within the TES, the latter of which is necessary to model normal-superconducting phase separation. Relevant numerical constants are provided for these physical processes in germanium, silicon, aluminum and tungsten. Random number sampling methods including inverse cumulative distribution function (CDF) and rejection techniques are reviewed. To improve the efficiency of charge transport modeling, an additional second order inverse CDF method is developed here along with an efficient barycentric coordinate sampling method of electric fields. Results are provided in a manner that is convenient for use in Monte Carlo and references are provided for validation of these models.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/08/review-article-physics-and-monte-carlo-techniques-as-relevant-to-cryogenic-phonon-and-ionization-readout-of-cdms-radiation-detectors-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Precision Pointing of IBEX-Lo Observations</title>
		<link>http://voxcharta.org/2012/02/07/precision-pointing-of-ibex-lo-observations/</link>
		<comments>http://voxcharta.org/2012/02/07/precision-pointing-of-ibex-lo-observations/#comments</comments>
		<pubDate>Wed, 08 Feb 2012 01:49:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acs]]></category>
		<category><![CDATA[attitude control system]]></category>
		<category><![CDATA[axis]]></category>
		<category><![CDATA[boresight]]></category>
		<category><![CDATA[flow parameters]]></category>
		<category><![CDATA[flow properties]]></category>
		<category><![CDATA[gas flow]]></category>
		<category><![CDATA[geometry]]></category>
		<category><![CDATA[interstellar gas]]></category>
		<category><![CDATA[launch]]></category>
		<category><![CDATA[neutral gas]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[precise determination]]></category>
		<category><![CDATA[redundancy]]></category>
		<category><![CDATA[reference system]]></category>
		<category><![CDATA[sensor data]]></category>
		<category><![CDATA[spacecraft attitude control]]></category>
		<category><![CDATA[star catalog]]></category>
		<category><![CDATA[star observation]]></category>
		<category><![CDATA[star sensor]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/07/precision-pointing-of-ibex-lo-observations/</guid>
		<description><![CDATA[Post-launch boresight of the IBEX-Lo instrument onboard the Interstellar Boundary Explorer (IBEX) is determined based on IBEX-Lo Star Sensor observations. Accurate information on the boresight of the neutral gas camera is essential for precise determination of interstellar gas flow parameters. Utilizing spin-phase information from the spacecraft attitude control system (ACS), positions of stars observed by [...]]]></description>
			<content:encoded><![CDATA[<p>Post-launch boresight of the IBEX-Lo instrument onboard the Interstellar Boundary Explorer (IBEX) is determined based on IBEX-Lo Star Sensor observations. Accurate information on the boresight of the neutral gas camera is essential for precise determination of interstellar gas flow parameters. Utilizing spin-phase information from the spacecraft attitude control system (ACS), positions of stars observed by the Star Sensor during two years of IBEX measurements were analyzed and compared with positions obtained from a star catalog. No statistically significant differences were observed beyond those expected from the pre-launch uncertainty in the Star Sensor mounting. Based on the star observations and their positions in the spacecraft reference system, pointing of the IBEX satellite spin axis was determined and compared with the pointing obtained from the ACS. Again, no statistically significant deviations were observed. We conclude that no systematic correction for boresight geometry is needed in the analysis of IBEX-Lo observations to determine neutral interstellar gas flow properties. A stack-up of uncertainties in attitude knowledge shows that the instantaneous IBEX-Lo pointing is determined to within $\sim 0.1\degr$ in both spin angle and elevation using either the Star Sensor or the ACS. Further, the Star Sensor can be used to independently determine the spacecraft spin axis. Thus, Star Sensor data can be used reliably to correct the spin phase when the Star Tracker (used by the ACS) is disabled by bright objects in its field-of-view. The Star Sensor can also determine the spin axis during most orbits and thus provides redundancy for the Star Tracker.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/07/precision-pointing-of-ibex-lo-observations/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Approximate Bayesian Computation for Astronomical Model Analysis: A Case Study in Galaxy Demographics and Morphological Transformation at High Redshift</title>
		<link>http://voxcharta.org/2012/02/07/approximate-bayesian-computation-for-astronomical-model-analysis-a-case-study-in-galaxy-demographics-and-morphological-transformation-at-high-redshift/</link>
		<comments>http://voxcharta.org/2012/02/07/approximate-bayesian-computation-for-astronomical-model-analysis-a-case-study-in-galaxy-demographics-and-morphological-transformation-at-high-redshift/#comments</comments>
		<pubDate>Wed, 08 Feb 2012 01:46:07 +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[abc analysis]]></category>
		<category><![CDATA[bayesian computation]]></category>
		<category><![CDATA[complex stochastic systems]]></category>
		<category><![CDATA[early universe]]></category>
		<category><![CDATA[input parameter]]></category>
		<category><![CDATA[latter condition]]></category>
		<category><![CDATA[markov chain monte]]></category>
		<category><![CDATA[markov chain monte carlo]]></category>
		<category><![CDATA[mcmc]]></category>
		<category><![CDATA[model analysis]]></category>
		<category><![CDATA[monte carlo simulation]]></category>
		<category><![CDATA[posterior probability]]></category>
		<category><![CDATA[probability density]]></category>
		<category><![CDATA[redshift galaxies]]></category>
		<category><![CDATA[statistical algorithm]]></category>
		<category><![CDATA[statistical inference]]></category>
		<category><![CDATA[stochastic model]]></category>
		<category><![CDATA[summary statistic]]></category>
		<category><![CDATA[target sequence]]></category>
		<category><![CDATA[tight constraints]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/07/approximate-bayesian-computation-for-astronomical-model-analysis-a-case-study-in-galaxy-demographics-and-morphological-transformation-at-high-redshift/</guid>
		<description><![CDATA[&#8220;Approximate Bayesian Computation&#8221; (ABC) represents a powerful methodology for the analysis of complex stochastic systems for which the likelihood of the observed data under an arbitrary set of input parameters may be entirely intractable-the latter condition rendering useless the standard machinery of tractable likelihood-based, Bayesian statistical inference (e.g. conventional Markov Chain Monte Carlo simulation; MCMC). [...]]]></description>
			<content:encoded><![CDATA[<p>&#8220;Approximate Bayesian Computation&#8221; (ABC) represents a powerful methodology for the analysis of complex stochastic systems for which the likelihood of the observed data under an arbitrary set of input parameters may be entirely intractable-the latter condition rendering useless the standard machinery of tractable likelihood-based, Bayesian statistical inference (e.g. conventional Markov Chain Monte Carlo simulation; MCMC). In this article we demonstrate the potential of ABC for astronomical model analysis by application to a case study in the morphological transformation of high redshift galaxies. To this end we develop, first, a stochastic model for the competing processes of merging and secular evolution in the early Universe; and second, through an ABC-based comparison against the observed demographics of the first generation of massive (M_gal &gt; 10^11 M_sun) galaxies (at 1.5 &lt; z &lt; 3) in the CANDELS/EGS dataset we derive posterior probability densities for the key parameters of this model. The &quot;Sequential Monte Carlo&quot; (SMC) implementation of ABC exhibited herein, featuring both a self-generating target sequence and self-refining MCMC kernel, is amongst the most efficient of contemporary approaches to this important statistical algorithm. We highlight as well through our chosen case study the value of careful summary statistic selection, and demonstrate two modern strategies for assessment and optimisation in this regard. Ultimately, our ABC analysis of the high redshift morphological mix returns tight constraints on the evolving merger rate in the early Universe and reveals merging, rather than secular evolution, as the most important mechanism for building up the first generation of bulges in early-type disks.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/07/approximate-bayesian-computation-for-astronomical-model-analysis-a-case-study-in-galaxy-demographics-and-morphological-transformation-at-high-redshift/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Rotating Disks and Non-Kinematic Double Peaks</title>
		<link>http://voxcharta.org/2012/02/07/rotating-disks-and-non-kinematic-double-peaks/</link>
		<comments>http://voxcharta.org/2012/02/07/rotating-disks-and-non-kinematic-double-peaks/#comments</comments>
		<pubDate>Wed, 08 Feb 2012 01:44:57 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[circumstance]]></category>
		<category><![CDATA[emergence]]></category>
		<category><![CDATA[exact solution]]></category>
		<category><![CDATA[hallmark]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[line emission]]></category>
		<category><![CDATA[line profile]]></category>
		<category><![CDATA[opacity]]></category>
		<category><![CDATA[rotation velocity]]></category>
		<category><![CDATA[thin keplerian disks]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/07/rotating-disks-and-non-kinematic-double-peaks/</guid>
		<description><![CDATA[Double-peaked line profiles are commonly considered a hallmark of rotating disks, with the distance between the peaks a measure of the rotation velocity. However, double-peaks can arise also from radiative transfer effects in optically thick non-rotating sources. Utilizing exact solutions of the line transfer problem we present a detailed study of line emission from geometrically [...]]]></description>
			<content:encoded><![CDATA[<p>Double-peaked line profiles are commonly considered a hallmark of rotating disks, with the distance between the peaks a measure of the rotation velocity. However, double-peaks can arise also from radiative transfer effects in optically thick non-rotating sources. Utilizing exact solutions of the line transfer problem we present a detailed study of line emission from geometrically thin Keplerian disks. We derive the conditions for emergence of kinematic double peaks in optically thin and thick disks, and find that it is generally impossible to disentangle the effects of kinematics and line opacity in observed double-peaked profiles. Unless supplemented by additional information, a double-peaked profile alone is not a reliable indicator of a rotating disk. In certain circumstances, triple and quadruple profiles might be better indicators of rotation in optically thick disks.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/07/rotating-disks-and-non-kinematic-double-peaks/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Close Companions to Young Stars. I. A Large Spectroscopic Survey in Chamaeleon I and Taurus-Auriga [Replacement]</title>
		<link>http://voxcharta.org/2012/02/07/close-companions-to-young-stars-i-a-large-spectroscopic-survey-in-chamaeleon-i-and-taurus-auriga-replacement/</link>
		<comments>http://voxcharta.org/2012/02/07/close-companions-to-young-stars-i-a-large-spectroscopic-survey-in-chamaeleon-i-and-taurus-auriga-replacement/#comments</comments>
		<pubDate>Wed, 08 Feb 2012 01:34:09 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[aur]]></category>
		<category><![CDATA[auriga star]]></category>
		<category><![CDATA[chamaeleon]]></category>
		<category><![CDATA[companion]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[field star]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[jupiter]]></category>
		<category><![CDATA[magellan]]></category>
		<category><![CDATA[main source]]></category>
		<category><![CDATA[multiplicity]]></category>
		<category><![CDATA[new discovery]]></category>
		<category><![CDATA[radial velocity variations]]></category>
		<category><![CDATA[resolution spectra]]></category>
		<category><![CDATA[rotators]]></category>
		<category><![CDATA[spectroscopic survey]]></category>
		<category><![CDATA[taurus]]></category>
		<category><![CDATA[young stars]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/07/close-companions-to-young-stars-i-a-large-spectroscopic-survey-in-chamaeleon-i-and-taurus-auriga-replacement/</guid>
		<description><![CDATA[We present the results of a multiplicity survey of 212 T Tauri stars in the Chamaeleon I and Taurus-Auriga star-forming regions, based on high-resolution spectra from the Magellan Clay 6.5 m telescope. From these data, we achieved a typical radial velocity precision of ~80 m/s with slower rotators yielding better precision, in general. For 174 [...]]]></description>
			<content:encoded><![CDATA[<p>We present the results of a multiplicity survey of 212 T Tauri stars in the Chamaeleon I and Taurus-Auriga star-forming regions, based on high-resolution spectra from the Magellan Clay 6.5 m telescope. From these data, we achieved a typical radial velocity precision of ~80 m/s with slower rotators yielding better precision, in general. For 174 of these stars, we obtained multi-epoch data with sufficient time baselines to identify binaries based on radial velocity variations. We identified eight close binaries and four close triples, of which three and two, respectively, are new discoveries. The spectroscopic multiplicity fractions we find for Cha I (7%) and Tau-Aur (6%) are similar to each other, and to the results of field star surveys in the same mass and period regime. However, unlike the results from imaging surveys, the frequency of systems with close companions in our sample is not seen to depend on primary mass. Additionally, we do not find a strong correlation between accretion and close multiplicity. This implies that close companions are not likely the main source of the accretion shut down observed in weak-lined T Tauri stars. Our results also suggest that sufficient radial velocity precision can be achieved for at least a subset of slowly rotating young stars to search for hot Jupiter planets.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Vertical structure of a supernova-driven turbulent magnetized ISM [Replacement]</title>
		<link>http://voxcharta.org/2012/02/07/vertical-structure-of-a-supernova-driven-turbulent-magnetized-ism-replacement/</link>
		<comments>http://voxcharta.org/2012/02/07/vertical-structure-of-a-supernova-driven-turbulent-magnetized-ism-replacement/#comments</comments>
		<pubDate>Wed, 08 Feb 2012 01:31:53 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[atomic gas]]></category>
		<category><![CDATA[flash code]]></category>
		<category><![CDATA[initial condition]]></category>
		<category><![CDATA[interstellar medium]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetic pressure]]></category>
		<category><![CDATA[magnetohydrodynamic simulation]]></category>
		<category><![CDATA[mhd]]></category>
		<category><![CDATA[myr]]></category>
		<category><![CDATA[oscillation]]></category>
		<category><![CDATA[positivity]]></category>
		<category><![CDATA[solar circle]]></category>
		<category><![CDATA[stable temperature]]></category>
		<category><![CDATA[temperature regimes]]></category>
		<category><![CDATA[tension force]]></category>
		<category><![CDATA[vertical column]]></category>
		<category><![CDATA[vertical distribution]]></category>
		<category><![CDATA[vertical stratification]]></category>
		<category><![CDATA[vertical structure]]></category>
		<category><![CDATA[vertical support]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/07/vertical-structure-of-a-supernova-driven-turbulent-magnetized-ism-replacement/</guid>
		<description><![CDATA[Stellar feedback drives the circulation of matter from the disk to the halo of galaxies. We perform three-dimensional magnetohydrodynamic simulations of a vertical column of the interstellar medium with initial conditions typical of the solar circle in which supernovae drive turbulence and determine the vertical stratification of the medium. The simulations were run using a [...]]]></description>
			<content:encoded><![CDATA[<p>Stellar feedback drives the circulation of matter from the disk to the halo of galaxies. We perform three-dimensional magnetohydrodynamic simulations of a vertical column of the interstellar medium with initial conditions typical of the solar circle in which supernovae drive turbulence and determine the vertical stratification of the medium. The simulations were run using a stable, positivity-preserving scheme for ideal MHD implemented in the FLASH code. We find that the majority (\approx 90 %) of the mass is contained in thermally-stable temperature regimes of cold molecular and atomic gas at T &lt; 200 K or warm atomic and ionized gas at 5000 K &lt; T &lt; 10^{4.2} K, with strong peaks in probability distribution functions of temperature in both the cold and warm regimes. The 200 &#8211; 10^{4.2} K gas fills 50-60 % of the volume near the plane, with hotter gas associated with supernova remnants (30-40 %) and cold clouds ( 3 kpc. The magnetic field in our models has no significant impact on the scale heights of gas in each temperature regime; the magnetic tension force is approximately equal to and opposite the magnetic pressure, so the addition of the field does not significantly affect the vertical support of the gas. The addition of a magnetic field does reduce the fraction of gas in the cold (&lt; 200 K) regime with a corresponding increase in the fraction of warm (~ 10^4 K) gas. However, our models lack rotational shear and thus have no large-scale dynamo, which reduces the role of the field in the models compared to reality. The supernovae drive oscillations in the vertical distribution of halo gas, with the period of the oscillations ranging from ~ 30 Myr in the T &lt; 200 K gas to ~ 100 Myr in the 10^6 K gas, in line with predictions by Walters &amp; Cox.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/07/vertical-structure-of-a-supernova-driven-turbulent-magnetized-ism-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Laser frequency comb techniques for precise astronomical spectroscopy</title>
		<link>http://voxcharta.org/2012/02/06/laser-frequency-comb-techniques-for-precise-astronomical-spectroscopy/</link>
		<comments>http://voxcharta.org/2012/02/06/laser-frequency-comb-techniques-for-precise-astronomical-spectroscopy/#comments</comments>
		<pubDate>Tue, 07 Feb 2012 02:11:30 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astronomical spectroscopy]]></category>
		<category><![CDATA[australian telescope]]></category>
		<category><![CDATA[ccd]]></category>
		<category><![CDATA[ccd exposure]]></category>
		<category><![CDATA[comb techniques]]></category>
		<category><![CDATA[deviates]]></category>
		<category><![CDATA[fundamental constant]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[laser frequency]]></category>
		<category><![CDATA[solar planet]]></category>
		<category><![CDATA[spectrograph]]></category>
		<category><![CDATA[spectroscopic analyses]]></category>
		<category><![CDATA[stellar radial velocities]]></category>
		<category><![CDATA[systematic error]]></category>
		<category><![CDATA[uniform sensitivity]]></category>
		<category><![CDATA[variability]]></category>
		<category><![CDATA[variation]]></category>
		<category><![CDATA[wavelength calibration]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/06/laser-frequency-comb-techniques-for-precise-astronomical-spectroscopy/</guid>
		<description><![CDATA[Precise astronomical spectroscopic analyses routinely assume that individual pixels in charge-coupled devices (CCDs) have uniform sensitivity to photons. Intra-pixel sensitivity (IPS) variations may already cause small systematic errors in, for example, studies of extra-solar planets via stellar radial velocities and cosmological variability in fundamental constants via quasar spectroscopy, but future experiments requiring velocity precisions approaching [...]]]></description>
			<content:encoded><![CDATA[<p>Precise astronomical spectroscopic analyses routinely assume that individual pixels in charge-coupled devices (CCDs) have uniform sensitivity to photons. Intra-pixel sensitivity (IPS) variations may already cause small systematic errors in, for example, studies of extra-solar planets via stellar radial velocities and cosmological variability in fundamental constants via quasar spectroscopy, but future experiments requiring velocity precisions approaching ~1 cm/s will be more strongly affected. Laser frequency combs have been shown to provide highly precise wavelength calibration for astronomical spectrographs, but here we show that they can also be used to measure IPS variations in astronomical CCDs in situ. We successfully tested a laser frequency comb system on the Ultra-High Resolution Facility spectrograph at the Anglo-Australian Telescope. By modelling the 2-dimensional comb signal recorded in a single CCD exposure, we find that the average IPS deviates by &lt;8 per cent if it is assumed to vary symmetrically about the pixel centre. We also demonstrate that series of comb exposures with absolutely known offsets between them can yield tighter constraints on symmetric IPS variations from ~100 pixels. We discuss measurement of asymmetric IPS variations and absolute wavelength calibration of astronomical spectrographs and CCDs using frequency combs.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/06/laser-frequency-comb-techniques-for-precise-astronomical-spectroscopy/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Advanced Multi-beam Spectrometer for the Green Bank Telescope</title>
		<link>http://voxcharta.org/2012/02/06/advanced-multi-beam-spectrometer-for-the-green-bank-telescope/</link>
		<comments>http://voxcharta.org/2012/02/06/advanced-multi-beam-spectrometer-for-the-green-bank-telescope/#comments</comments>
		<pubDate>Tue, 07 Feb 2012 02:06:54 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[adc]]></category>
		<category><![CDATA[bandwidth]]></category>
		<category><![CDATA[beams]]></category>
		<category><![CDATA[capability]]></category>
		<category><![CDATA[casper]]></category>
		<category><![CDATA[focal plane]]></category>
		<category><![CDATA[gbt]]></category>
		<category><![CDATA[green bank telescope]]></category>
		<category><![CDATA[new science]]></category>
		<category><![CDATA[nrao]]></category>
		<category><![CDATA[science project]]></category>
		<category><![CDATA[spectrometer]]></category>
		<category><![CDATA[university of california]]></category>
		<category><![CDATA[university of california berkeley]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/06/advanced-multi-beam-spectrometer-for-the-green-bank-telescope/</guid>
		<description><![CDATA[A new spectrometer for the Green Bank Telescope (GBT) is being built jointly by the NRAO and the CASPER, University of California, Berkeley. The spectrometer uses 8 bit ADCs and will be capable of processing up to 1.25 GHz bandwidth from 8 dual polarized beams. This mode will be used to process data from focal [...]]]></description>
			<content:encoded><![CDATA[<p>A new spectrometer for the Green Bank Telescope (GBT) is being built jointly by the NRAO and the CASPER, University of California, Berkeley. The spectrometer uses 8 bit ADCs and will be capable of processing up to 1.25 GHz bandwidth from 8 dual polarized beams. This mode will be used to process data from focal plane arrays. The spectrometer supports observing mode with 8 tunable digital sub-bands within the 1.25 GHz bandwidth. The spectrometer can also be configured to process a bandwidth of up to 10 GHz with 64 tunable sub-bands from a dual polarized beam. The vastly enhanced backend capabilities will support several new science projects with the GBT.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/06/advanced-multi-beam-spectrometer-for-the-green-bank-telescope/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Practices in Code Discoverability</title>
		<link>http://voxcharta.org/2012/02/06/practices-in-code-discoverability/</link>
		<comments>http://voxcharta.org/2012/02/06/practices-in-code-discoverability/#comments</comments>
		<pubDate>Tue, 07 Feb 2012 02:04:31 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[ascl]]></category>
		<category><![CDATA[astrophysics source code library]]></category>
		<category><![CDATA[attempts]]></category>
		<category><![CDATA[computer source]]></category>
		<category><![CDATA[discipline]]></category>
		<category><![CDATA[falsifiability]]></category>
		<category><![CDATA[implementation]]></category>
		<category><![CDATA[poster paper]]></category>
		<category><![CDATA[preprint]]></category>
		<category><![CDATA[reliability]]></category>
		<category><![CDATA[repository]]></category>
		<category><![CDATA[reproducibility]]></category>
		<category><![CDATA[resistance]]></category>
		<category><![CDATA[scientist]]></category>
		<category><![CDATA[source code]]></category>
		<category><![CDATA[source code library]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/06/practices-in-code-discoverability/</guid>
		<description><![CDATA[Much of scientific progress now hinges on the reliability, falsifiability and reproducibility of computer source codes. Astrophysics in particular is a discipline that today leads other sciences in making useful scientific components freely available online, including data, abstracts, preprints, and fully published papers, yet even today many astrophysics source codes remain hidden from public view. [...]]]></description>
			<content:encoded><![CDATA[<p>Much of scientific progress now hinges on the reliability, falsifiability and reproducibility of computer source codes. Astrophysics in particular is a discipline that today leads other sciences in making useful scientific components freely available online, including data, abstracts, preprints, and fully published papers, yet even today many astrophysics source codes remain hidden from public view. We review the importance and history of source codes in astrophysics and previous efforts to develop ways in which information about astrophysics codes can be shared. We also discuss why some scientist coders resist sharing or publishing their codes, the reasons for and importance of overcoming this resistance, and alert the community to a reworking of one of the first attempts for sharing codes, the Astrophysics Source Code Library (ASCL). We discuss the implementation of the ASCL in an accompanying poster paper. We suggest that code could be given a similar level of referencing as data gets in repositories such as ADS.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/06/practices-in-code-discoverability/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Practices in Code Discoverability: Astrophysics Source Code Library</title>
		<link>http://voxcharta.org/2012/02/06/practices-in-code-discoverability-astrophysics-source-code-library/</link>
		<comments>http://voxcharta.org/2012/02/06/practices-in-code-discoverability-astrophysics-source-code-library/#comments</comments>
		<pubDate>Tue, 07 Feb 2012 02:04:19 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[advisory committee]]></category>
		<category><![CDATA[ascl]]></category>
		<category><![CDATA[astrophysics source code library]]></category>
		<category><![CDATA[comprehensive listing]]></category>
		<category><![CDATA[download site]]></category>
		<category><![CDATA[future plans]]></category>
		<category><![CDATA[marketing plan]]></category>
		<category><![CDATA[refereed journal]]></category>
		<category><![CDATA[source code]]></category>
		<category><![CDATA[source code library]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/06/practices-in-code-discoverability-astrophysics-source-code-library/</guid>
		<description><![CDATA[Here we describe the Astrophysics Source Code Library (ASCL), which takes an active approach to sharing astrophysical source code. ASCL&#8217;s editor seeks out both new and old peer-reviewed papers that describe methods or experiments that involve the development or use of source code, and adds entries for the found codes to the library. This approach [...]]]></description>
			<content:encoded><![CDATA[<p>Here we describe the Astrophysics Source Code Library (ASCL), which takes an active approach to sharing astrophysical source code. ASCL&#8217;s editor seeks out both new and old peer-reviewed papers that describe methods or experiments that involve the development or use of source code, and adds entries for the found codes to the library. This approach ensures that source codes are added without requiring authors to actively submit them, resulting in a comprehensive listing that covers a significant number of the astrophysics source codes used in peer-reviewed studies. The ASCL now has over 340 codes in it and continues to grow. In 2011, the ASCL (<a href="http://ascl.net">http://ascl.net</a>) has on average added 19 new codes per month. An advisory committee has been established to provide input and guide the development and expansion of the new site, and a marketing plan has been developed and is being executed. All ASCL source codes have been used to generate results published in or submitted to a refereed journal and are freely available either via a download site or from an identified source.   This paper provides the history and description of the ASCL. It lists the requirements for including codes, examines the benefits of the ASCL, and outlines some of its future plans.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/06/practices-in-code-discoverability-astrophysics-source-code-library/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>MIS: a MIRIAD Interferometry Singledish toolkit</title>
		<link>http://voxcharta.org/2012/02/06/mis-a-miriad-interferometry-singledish-toolkit/</link>
		<comments>http://voxcharta.org/2012/02/06/mis-a-miriad-interferometry-singledish-toolkit/#comments</comments>
		<pubDate>Tue, 07 Feb 2012 02:03:28 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[ALMA]]></category>
		<category><![CDATA[array]]></category>
		<category><![CDATA[astronomy]]></category>
		<category><![CDATA[calibration]]></category>
		<category><![CDATA[collaborators]]></category>
		<category><![CDATA[continuum]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[cvs]]></category>
		<category><![CDATA[dish]]></category>
		<category><![CDATA[interferometer]]></category>
		<category><![CDATA[interferometry]]></category>
		<category><![CDATA[map]]></category>
		<category><![CDATA[millimeter wave]]></category>
		<category><![CDATA[NGC]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[pipeline infrastructure]]></category>
		<category><![CDATA[scripts]]></category>
		<category><![CDATA[small group]]></category>
		<category><![CDATA[spectral line]]></category>
		<category><![CDATA[uniform data]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/06/mis-a-miriad-interferometry-singledish-toolkit/</guid>
		<description><![CDATA[Building on the &#8220;drPACS&#8221; contribution at ADASS XX of a simple Unix pipeline infrastructure, we implemented a pipeline toolkit using the package MIRIAD to combine Interferometric and Single Dish data (MIS). This was prompted by our observations made with the Combined Array For Research in Millimeter-wave Astronomy (CARMA) interferometer of the star-forming region NGC 1333, [...]]]></description>
			<content:encoded><![CDATA[<p>Building on the &#8220;drPACS&#8221; contribution at ADASS XX of a simple Unix pipeline infrastructure, we implemented a pipeline toolkit using the package MIRIAD to combine Interferometric and Single Dish data (MIS). This was prompted by our observations made with the Combined Array For Research in Millimeter-wave Astronomy (CARMA) interferometer of the star-forming region NGC 1333, a large survey highlighting the new 23-element and singledish observing modes. The project consists of 20 CARMA datasets each containing interferometric as well as simultaneously obtained single dish data, for 3 molecular spectral lines and continuum, in 527 different pointings, covering an area of about 8 by 11 arcminutes. A small group of collaborators then shared this toolkit and their parameters via CVS, and scripts were developed to ensure uniform data reduction across the group. The pipeline was run end-to-end each night as new observations were obtained, producing maps that contained all the data to date. We will show examples of the scripts and data products. This approach could serve as a model for repeated calibration and mapping of large mixed-mode correlation datasets from ALMA.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/06/mis-a-miriad-interferometry-singledish-toolkit/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Spectral components analysis of diffuse emission processes</title>
		<link>http://voxcharta.org/2012/02/06/spectral-components-analysis-of-diffuse-emission-processes/</link>
		<comments>http://voxcharta.org/2012/02/06/spectral-components-analysis-of-diffuse-emission-processes/#comments</comments>
		<pubDate>Tue, 07 Feb 2012 02:02:33 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[appendix]]></category>
		<category><![CDATA[closeness]]></category>
		<category><![CDATA[combinations]]></category>
		<category><![CDATA[diffuse emission]]></category>
		<category><![CDATA[energy spectra]]></category>
		<category><![CDATA[foreground]]></category>
		<category><![CDATA[generalization]]></category>
		<category><![CDATA[likelihood function]]></category>
		<category><![CDATA[map]]></category>
		<category><![CDATA[novel method]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[spatial distribution]]></category>
		<category><![CDATA[spectral components]]></category>
		<category><![CDATA[templates]]></category>
		<category><![CDATA[yeas]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/06/spectral-components-analysis-of-diffuse-emission-processes/</guid>
		<description><![CDATA[We develop a novel method to separate the components of a diffuse emission process based on an association with the energy spectra. Most of the existing methods use some information about the spatial distribution of components, e.g., closeness to an external template, independence of components etc., in order to separate them. In this paper we [...]]]></description>
			<content:encoded><![CDATA[<p>We develop a novel method to separate the components of a diffuse emission process based on an association with the energy spectra. Most of the existing methods use some information about the spatial distribution of components, e.g., closeness to an external template, independence of components etc., in order to separate them. In this paper we propose a method where one puts conditions on the spectra only. The advantages of our method are: 1) it is internal: the maps of the components are constructed as combinations of data in different energy bins, 2) the components may be correlated among each other, 3) the method is semi-blind: in many cases, it is sufficient to assume a functional form of the spectra and determine the parameters from a maximization of a likelihood function. As an example, we derive the CMB map and the foreground maps for seven yeas of WMAP data. In an Appendix, we present a generalization of the method, where one can also add a number of external templates.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/06/spectral-components-analysis-of-diffuse-emission-processes/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The astrometric recognition of the solar Clementine gnomon (1702) [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/02/06/the-astrometric-recognition-of-the-solar-clementine-gnomon-1702-cross-listing/</link>
		<comments>http://voxcharta.org/2012/02/06/the-astrometric-recognition-of-the-solar-clementine-gnomon-1702-cross-listing/#comments</comments>
		<pubDate>Tue, 07 Feb 2012 01:59:34 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[azimuth]]></category>
		<category><![CDATA[bianchini]]></category>
		<category><![CDATA[centuries]]></category>
		<category><![CDATA[clementine]]></category>
		<category><![CDATA[deviations]]></category>
		<category><![CDATA[diameter]]></category>
		<category><![CDATA[ecliptic latitude]]></category>
		<category><![CDATA[ephemerides]]></category>
		<category><![CDATA[gnomon]]></category>
		<category><![CDATA[historical instruments]]></category>
		<category><![CDATA[meridian line]]></category>
		<category><![CDATA[obliquity]]></category>
		<category><![CDATA[oval shape]]></category>
		<category><![CDATA[pinhole]]></category>
		<category><![CDATA[restauration]]></category>
		<category><![CDATA[solar image]]></category>
		<category><![CDATA[solar spots]]></category>
		<category><![CDATA[systematic error]]></category>
		<category><![CDATA[true line]]></category>
		<category><![CDATA[true north]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/06/the-astrometric-recognition-of-the-solar-clementine-gnomon-1702-cross-listing/</guid>
		<description><![CDATA[The Clementine gnomon has been built in 1702 to measure the Earth&#8217;s obliquity variation. For this reason the pinhole was located in the walls of Diocletian&#8217;s times (305 a. D.) in order to remain stable along the centuries, but its original form and position have been modified. We used an astrometric method to recover the [...]]]></description>
			<content:encoded><![CDATA[<p>The Clementine gnomon has been built in 1702 to measure the Earth&#8217;s obliquity variation. For this reason the pinhole was located in the walls of Diocletian&#8217;s times (305 a. D.) in order to remain stable along the centuries, but its original form and position have been modified. We used an astrometric method to recover the original position of the pinhole: reshaping the pinhole to a circle of 1.5 cm of diameter, the positions of the Northern and Southern limbs have been compared with the ephemerides. A sistematic shift of 4.5 mm Southward of the whole solar image shows that the original pinhole was 4.5 mm North of the actual position, as the images in the Bianchini&#8217;s book (1703) suggest. The oval shape of the actual pinhole is also wrong. Using a circle the larger solar spots are clearly visible. Some reference stars of the catalogue of Philippe de la Hire (1702), used originally for measuring the ecliptic latitude of the Sun, are written next to the meridian line, but after the last restauration (2000), four of them are wrongly located. Finally the deviation from the true North, of the meridian line&#8217;s azimuth confirms the value recovered in 1750. This, with the local deviations of a true line, will remain as systematic error, like for all these historical instruments.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/06/the-astrometric-recognition-of-the-solar-clementine-gnomon-1702-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>On The Doppler Velocity of Emission Line Profiles Formed in the &quot;Coronal Contraflow&quot; that is the Chromosphere-Corona Mass Cycle</title>
		<link>http://voxcharta.org/2012/02/06/on-the-doppler-velocity-of-emission-line-profiles-formed-in-the-coronal-contraflow-that-is-the-chromosphere-corona-mass-cycle/</link>
		<comments>http://voxcharta.org/2012/02/06/on-the-doppler-velocity-of-emission-line-profiles-formed-in-the-coronal-contraflow-that-is-the-chromosphere-corona-mass-cycle/#comments</comments>
		<pubDate>Tue, 07 Feb 2012 01:49:44 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[asymmetry]]></category>
		<category><![CDATA[chromosphere]]></category>
		<category><![CDATA[contraflow]]></category>
		<category><![CDATA[corona]]></category>
		<category><![CDATA[coronal structure]]></category>
		<category><![CDATA[doppler velocity]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[image sequence]]></category>
		<category><![CDATA[line profile]]></category>
		<category><![CDATA[loop structure]]></category>
		<category><![CDATA[red shift]]></category>
		<category><![CDATA[red wing]]></category>
		<category><![CDATA[resolution element]]></category>
		<category><![CDATA[return flow]]></category>
		<category><![CDATA[spectroscopic diagnostics]]></category>
		<category><![CDATA[spectroscopic observation]]></category>
		<category><![CDATA[temporal resolution]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/06/on-the-doppler-velocity-of-emission-line-profiles-formed-in-the-coronal-contraflow-that-is-the-chromosphere-corona-mass-cycle/</guid>
		<description><![CDATA[This analysis begins to explore the complex chromosphere-corona mass cycle using a blend of imaging and spectroscopic diagnostics. Single Gaussian fits to hot emission line profiles (formed above 1MK) at the base of coronal loop structures indicate material blue-shifts of 5-10km/s while cool emission line profiles (formed below 1MK) yield red-shifts of a similar magnitude [...]]]></description>
			<content:encoded><![CDATA[<p>This analysis begins to explore the complex chromosphere-corona mass cycle using a blend of imaging and spectroscopic diagnostics. Single Gaussian fits to hot emission line profiles (formed above 1MK) at the base of coronal loop structures indicate material blue-shifts of 5-10km/s while cool emission line profiles (formed below 1MK) yield red-shifts of a similar magnitude &#8211; indicating, to zeroth order, that a temperature-dependent bifurcating flow exists on coronal structures. Image sequences of the same region reveal weakly emitting upward propagating disturbances in both hot and cool emission with apparent speeds of 50-150km/s. Spectroscopic observations indicate that these propagating disturbances produce a weak emission component in the blue wing at commensurate speed, but that they contribute only a few percent to the (ensemble) emission line profile in a single spatio-temporal resolution element. Subsequent analysis of imaging data shows material &#8220;draining&#8221; slowly (~10km/s) out of the corona, but only in the cooler passbands. We interpret the draining as the return-flow of coronal material at the end of the complex chromosphere-corona mass cycle. Further, we suggest that the efficient radiative cooling of the draining material produces a significant contribution to the red wing of cool emission lines that is ultimately responsible for their systematic red-shift as derived from a single Gaussian fit when compared to those formed in hotter (conductively dominated) domains. The presence of counter-streaming flows complicates the line profiles, their interpretation, and asymmetry diagnoses, but allows a different physical picture of the lower corona to develop.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/06/on-the-doppler-velocity-of-emission-line-profiles-formed-in-the-coronal-contraflow-that-is-the-chromosphere-corona-mass-cycle/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Solar astrometry: the status of art in 2011 [Replacement]</title>
		<link>http://voxcharta.org/2012/02/06/solar-astrometry-the-status-of-art-in-2011-replacement/</link>
		<comments>http://voxcharta.org/2012/02/06/solar-astrometry-the-status-of-art-in-2011-replacement/#comments</comments>
		<pubDate>Tue, 07 Feb 2012 01:34:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astrometry]]></category>
		<category><![CDATA[balloon]]></category>
		<category><![CDATA[climate studies]]></category>
		<category><![CDATA[decade]]></category>
		<category><![CDATA[drift scan]]></category>
		<category><![CDATA[evolutionary stage]]></category>
		<category><![CDATA[Measurement]]></category>
		<category><![CDATA[meridian]]></category>
		<category><![CDATA[paramount importance]]></category>
		<category><![CDATA[radius]]></category>
		<category><![CDATA[relationship]]></category>
		<category><![CDATA[satellite]]></category>
		<category><![CDATA[scan mode]]></category>
		<category><![CDATA[shape]]></category>
		<category><![CDATA[solar diameter]]></category>
		<category><![CDATA[space measurement]]></category>
		<category><![CDATA[telescopes]]></category>
		<category><![CDATA[total solar irradiance]]></category>
		<category><![CDATA[transits]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/06/solar-astrometry-the-status-of-art-in-2011-replacement/</guid>
		<description><![CDATA[Solar astrometry deals with the accurate measumerent of the solar diameter, and in general with the measurement of the shape of the Sun. During the last decades several techniques have been developed to monitor the radius and the irradiance of the Sun: meridian transits, telescopes in drift-scan mode, solar astrolabes, balloons, and satellites dedicated to [...]]]></description>
			<content:encoded><![CDATA[<p>Solar astrometry deals with the accurate measumerent of the solar diameter, and in general with the measurement of the shape of the Sun. During the last decades several techniques have been developed to monitor the radius and the irradiance of the Sun: meridian transits, telescopes in drift-scan mode, solar astrolabes, balloons, and satellites dedicated to the measurements of the solar diameter, and space measurements of the total solar irradiance are now performed to know the relationship radius-luminosity for the Sun in this evolutionary stage of its life. The feedback of solar astrometry in climate studies is of paramount importance. The status of art in the various fields of research here adressed is outlined.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
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		<title>Gerbert of Aurillac: astronomy and geometry in tenth century Europe [Replacement]</title>
		<link>http://voxcharta.org/2012/02/06/gerbert-of-aurillac-astronomy-and-geometry-in-tenth-century-europe-replacement-2/</link>
		<comments>http://voxcharta.org/2012/02/06/gerbert-of-aurillac-astronomy-and-geometry-in-tenth-century-europe-replacement-2/#comments</comments>
		<pubDate>Tue, 07 Feb 2012 01:33:35 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abacus]]></category>
		<category><![CDATA[arabic numbers]]></category>
		<category><![CDATA[astronomer]]></category>
		<category><![CDATA[astronomical observation]]></category>
		<category><![CDATA[constantine]]></category>
		<category><![CDATA[didactical]]></category>
		<category><![CDATA[equatorial mount]]></category>
		<category><![CDATA[equilateral triangle area]]></category>
		<category><![CDATA[equinox]]></category>
		<category><![CDATA[fleury]]></category>
		<category><![CDATA[mathematician]]></category>
		<category><![CDATA[north celestial pole]]></category>
		<category><![CDATA[observing the sun]]></category>
		<category><![CDATA[organ builder]]></category>
		<category><![CDATA[polaris]]></category>
		<category><![CDATA[rational approximation]]></category>
		<category><![CDATA[silvester]]></category>
		<category><![CDATA[solstice]]></category>
		<category><![CDATA[tenth century]]></category>
		<category><![CDATA[xii century]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/06/gerbert-of-aurillac-astronomy-and-geometry-in-tenth-century-europe-replacement-2/</guid>
		<description><![CDATA[Gerbert of Aurillac was the most prominent personality of the tenth century: astronomer, organ builder and music theoretician, mathematician, philosopher, and finally pope with the name of Silvester II (999-1003). Gerbert introduced firstly the arabic numbers in Europe, invented an abacus for speeding the calculations and found a rational approximation for the equilateral triangle area, [...]]]></description>
			<content:encoded><![CDATA[<p>Gerbert of Aurillac was the most prominent personality of the tenth century: astronomer, organ builder and music theoretician, mathematician, philosopher, and finally pope with the name of Silvester II (999-1003). Gerbert introduced firstly the arabic numbers in Europe, invented an abacus for speeding the calculations and found a rational approximation for the equilateral triangle area, in the letter to Adelbold here discussed. Gerbert described a semi-sphere to Constantine of Fleury with built-in sighting tubes, used for astronomical observations. The procedure to identify the star nearest to the North celestial pole is very accurate and still in use in the XII century, when &#8220;Computatrix&#8221; was the name of Polaris. For didactical purposes the Polaris would have been precise enough and much less time consuming, but here Gerbert was clearly aligning a precise equatorial mount for a fixed instrument for accurate daytime observations. Through the sighting tubes it was possible to detect equinoxes and solstices by observing the Sun in the corresponding days. The horalogium of Magdeburg was probably a big and fixed-mount nocturlabe, always pointing the star near the celestial pole.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/06/gerbert-of-aurillac-astronomy-and-geometry-in-tenth-century-europe-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Low frequency seeing and solar diameter measurements [Replacement]</title>
		<link>http://voxcharta.org/2012/02/06/low-frequency-seeing-and-solar-diameter-measurements-replacement/</link>
		<comments>http://voxcharta.org/2012/02/06/low-frequency-seeing-and-solar-diameter-measurements-replacement/#comments</comments>
		<pubDate>Tue, 07 Feb 2012 01:33:12 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[diameter measurement]]></category>
		<category><![CDATA[drift scan]]></category>
		<category><![CDATA[evidences]]></category>
		<category><![CDATA[image motion]]></category>
		<category><![CDATA[low frequency]]></category>
		<category><![CDATA[solar diameter]]></category>
		<category><![CDATA[Sun]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/06/low-frequency-seeing-and-solar-diameter-measurements-replacement/</guid>
		<description><![CDATA[The action of the atmospheric seeing is blurring, image stretching and image motion. This happens even to the image of the Sun which is more than half degree wide. Low frequency seeing components affect the solar diameter values measured either throught the drift-scan or the heliometer methods. We present evidences of image motion and stretching [...]]]></description>
			<content:encoded><![CDATA[<p>The action of the atmospheric seeing is blurring, image stretching and image motion. This happens even to the image of the Sun which is more than half degree wide. Low frequency seeing components affect the solar diameter values measured either throught the drift-scan or the heliometer methods. We present evidences of image motion and stretching down to 0.001 Hz.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/06/low-frequency-seeing-and-solar-diameter-measurements-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Vertical structure of a supernova-driven turbulent magnetized ISM</title>
		<link>http://voxcharta.org/2012/02/05/vertical-structure-of-a-supernova-driven-turbulent-magnetized-ism/</link>
		<comments>http://voxcharta.org/2012/02/05/vertical-structure-of-a-supernova-driven-turbulent-magnetized-ism/#comments</comments>
		<pubDate>Mon, 06 Feb 2012 01:47:43 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[atomic gas]]></category>
		<category><![CDATA[flash code]]></category>
		<category><![CDATA[initial condition]]></category>
		<category><![CDATA[interstellar medium]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetic pressure]]></category>
		<category><![CDATA[magnetohydrodynamic simulation]]></category>
		<category><![CDATA[mhd]]></category>
		<category><![CDATA[myr]]></category>
		<category><![CDATA[oscillation]]></category>
		<category><![CDATA[positivity]]></category>
		<category><![CDATA[solar circle]]></category>
		<category><![CDATA[stable temperature]]></category>
		<category><![CDATA[temperature regimes]]></category>
		<category><![CDATA[tension force]]></category>
		<category><![CDATA[vertical column]]></category>
		<category><![CDATA[vertical distribution]]></category>
		<category><![CDATA[vertical stratification]]></category>
		<category><![CDATA[vertical structure]]></category>
		<category><![CDATA[vertical support]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/05/vertical-structure-of-a-supernova-driven-turbulent-magnetized-ism/</guid>
		<description><![CDATA[Stellar feedback drives the circulation of matter from the disk to the halo of galaxies. We perform three-dimensional magnetohydrodynamic simulations of a vertical column of the interstellar medium with initial conditions typical of the solar circle in which supernovae drive turbulence and determine the vertical stratification of the medium. The simulations were run using a [...]]]></description>
			<content:encoded><![CDATA[<p>Stellar feedback drives the circulation of matter from the disk to the halo of galaxies. We perform three-dimensional magnetohydrodynamic simulations of a vertical column of the interstellar medium with initial conditions typical of the solar circle in which supernovae drive turbulence and determine the vertical stratification of the medium. The simulations were run using a stable, positivity-preserving scheme for ideal MHD implemented in the FLASH code. We find that the majority (\approx 90 %) of the mass is contained in thermally-stable temperature regimes of cold molecular and atomic gas at T &lt; 200 K or warm atomic and ionized gas at 5000 K &lt; T &lt; 10^{4.2} K, with strong peaks in probability distribution functions of temperature in both the cold and warm regimes. The 200 &#8211; 10^{4.2} K gas fills 50-60 % of the volume near the plane, with hotter gas associated with supernova remnants (30-40 %) and cold clouds ( 3 kpc. The magnetic field in our models has no significant impact on the scale heights of gas in each temperature regime; the magnetic tension force is approximately equal to and opposite the magnetic pressure, so the addition of the field does not significantly affect the vertical support of the gas. The addition of a magnetic field does reduce the fraction of gas in the cold (&lt; 200 K) regime with a corresponding increase in the fraction of warm (~ 10^4 K) gas. However, our models lack rotational shear and thus have no large-scale dynamo, which reduces the role of the field in the models compared to reality. The supernovae drive oscillations in the vertical distribution of halo gas, with the period of the oscillations ranging from ~ 30 Myr in the T &lt; 200 K gas to ~ 100 Myr in the 10^6 K gas, in line with predictions by Walters &amp; Cox.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Practical Methods for Continuous Gravitational Wave Detection using Pulsar Timing Data</title>
		<link>http://voxcharta.org/2012/02/05/practical-methods-for-continuous-gravitational-wave-detection-using-pulsar-timing-data/</link>
		<comments>http://voxcharta.org/2012/02/05/practical-methods-for-continuous-gravitational-wave-detection-using-pulsar-timing-data/#comments</comments>
		<pubDate>Mon, 06 Feb 2012 01:37:06 +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[amplitude]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[detection strategy]]></category>
		<category><![CDATA[distance]]></category>
		<category><![CDATA[efficacy]]></category>
		<category><![CDATA[einstein]]></category>
		<category><![CDATA[fabric]]></category>
		<category><![CDATA[frequency band]]></category>
		<category><![CDATA[frequency hz]]></category>
		<category><![CDATA[general relativity]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[gravitational wave detection]]></category>
		<category><![CDATA[hole binaries]]></category>
		<category><![CDATA[low frequency]]></category>
		<category><![CDATA[optimal quality]]></category>
		<category><![CDATA[pairwise]]></category>
		<category><![CDATA[ripple]]></category>
		<category><![CDATA[signal]]></category>
		<category><![CDATA[space time]]></category>
		<category><![CDATA[stochastic background]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/05/practical-methods-for-continuous-gravitational-wave-detection-using-pulsar-timing-data/</guid>
		<description><![CDATA[Gravitational Waves (GWs) are tiny ripples in the fabric of space-time predicted by Einstein&#8217;s General Relativity. Pulsar timing arrays (PTAs) are well poised to detect low frequency ($10^{-9}$ &#8212; $10^{-7}$ Hz) GWs in the near future. There has been a significant amount of research into the detection of a stochastic background of GWs from supermassive [...]]]></description>
			<content:encoded><![CDATA[<p>Gravitational Waves (GWs) are tiny ripples in the fabric of space-time predicted by Einstein&#8217;s General Relativity. Pulsar timing arrays (PTAs) are well poised to detect low frequency ($10^{-9}$ &#8212; $10^{-7}$ Hz) GWs in the near future. There has been a significant amount of research into the detection of a stochastic background of GWs from supermassive black hole binaries (SMBHBs). Recent work has shown that single continuous sources standing out above the background may be detectable by PTAs operating at a sensitivity sufficient to detect the stochastic background. The most likely sources of continuous GWs in the pulsar timing frequency band are extremely massive and/or nearby SMBHBs. In this paper we present detection strategies including various forms of matched filtering and power spectral summing. We determine the efficacy and computational cost of such strategies. It is shown that it is computationally infeasible to use an optimal matched filter including the poorly constrained pulsar distances with a grid based method. We show that an Earth-term-matched filter constructed using only the correlated signal terms is both computationally viable and highly sensitive to GW signals. This technique is only a factor of two less sensitive than the computationally unrealizable optimal matched filter and a factor of two more sensitive than a power spectral summing technique. We further show that a pairwise matched filter, taking the pulsar distances into account is comparable to the optimal matched filter for the single template case and comparable to the Earth-term-matched filter for many search templates. Finally, using simulated data optimal quality, we place a theoretical minimum detectable strain amplitude of $h&gt;2\times 10^{-15}$ from continuous GWs at frequencies on the order $\sim1/T_{\rm obs}$.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/05/practical-methods-for-continuous-gravitational-wave-detection-using-pulsar-timing-data/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Bayesian analysis of polarization measurements</title>
		<link>http://voxcharta.org/2012/02/02/bayesian-analysis-of-polarization-measurements/</link>
		<comments>http://voxcharta.org/2012/02/02/bayesian-analysis-of-polarization-measurements/#comments</comments>
		<pubDate>Fri, 03 Feb 2012 01:55:15 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[Measurement]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[polarization measurements]]></category>
		<category><![CDATA[signal to noise]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/02/bayesian-analysis-of-polarization-measurements/</guid>
		<description><![CDATA[A detailed and formal account of polarization measurements using Bayesian analysis is given based on the assumption of gaussian error for the Stokes parameters. This analysis is crucial for the measurement of the polarization degree and angle at very low (and very high) signal-to-noise. The treatment serves as a framework for customized analysis of data [...]]]></description>
			<content:encoded><![CDATA[<p>A detailed and formal account of polarization measurements using Bayesian analysis is given based on the assumption of gaussian error for the Stokes parameters. This analysis is crucial for the measurement of the polarization degree and angle at very low (and very high) signal-to-noise. The treatment serves as a framework for customized analysis of data based on a particular prior suited to the experiment.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Precise Infrared Radial Velocities from Keck/NIRSPEC and the Search for Young Planets</title>
		<link>http://voxcharta.org/2012/02/02/precise-infrared-radial-velocities-from-kecknirspec-and-the-search-for-young-planets/</link>
		<comments>http://voxcharta.org/2012/02/02/precise-infrared-radial-velocities-from-kecknirspec-and-the-search-for-young-planets/#comments</comments>
		<pubDate>Fri, 03 Feb 2012 01:54:43 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[beta pic]]></category>
		<category><![CDATA[dominant source]]></category>
		<category><![CDATA[field star]]></category>
		<category><![CDATA[hot jupiters]]></category>
		<category><![CDATA[hya]]></category>
		<category><![CDATA[infrared wavelength]]></category>
		<category><![CDATA[keck observatory]]></category>
		<category><![CDATA[mass companions]]></category>
		<category><![CDATA[measurement error]]></category>
		<category><![CDATA[optical observation]]></category>
		<category><![CDATA[radial velocity]]></category>
		<category><![CDATA[radial velocity measurements]]></category>
		<category><![CDATA[rotating stars]]></category>
		<category><![CDATA[spectroscopic binary]]></category>
		<category><![CDATA[spot noise]]></category>
		<category><![CDATA[star spot]]></category>
		<category><![CDATA[type star]]></category>
		<category><![CDATA[wavelength calibration]]></category>
		<category><![CDATA[young stars]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/02/precise-infrared-radial-velocities-from-kecknirspec-and-the-search-for-young-planets/</guid>
		<description><![CDATA[We present a high-precision infrared radial velocity study of late-type stars using spectra obtained with NIRSPEC at the W. M. Keck Observatory. Radial velocity precisions of 50 m/s are achieved for old field mid-M dwarfs using telluric features for precise wavelength calibration. Using this technique, 20 young stars in the {\beta} Pic (age ~12 Myr) [...]]]></description>
			<content:encoded><![CDATA[<p>We present a high-precision infrared radial velocity study of late-type stars using spectra obtained with NIRSPEC at the W. M. Keck Observatory. Radial velocity precisions of 50 m/s are achieved for old field mid-M dwarfs using telluric features for precise wavelength calibration. Using this technique, 20 young stars in the {\beta} Pic (age ~12 Myr) and TW Hya (age ~8 Myr) Associations were monitored over several years to search for low mass companions; we also included the chromospherically active field star GJ 873 (EV Lac) in this survey. Based on comparisons with previous optical observations of these young active stars, radial velocity measurements at infrared wavelengths mitigate the radial velocity noise caused by star spots by a factor of ~3. Nevertheless, star spot noise is still the dominant source of measurement error for young stars at 2.3 {\mu}m, and limits the precision to ~77 m/s for the slowest rotating stars (v sin i  12 km/s). The observations reveal both GJ 3305 and TWA 23 to be single-lined spectroscopic binaries; in the case of GJ 3305, the motion is likely caused by its 0.09&#8243; companion, identified after this survey began. The large amplitude, short-timescale variations of TWA 13A are indicative of a hot Jupiter-like companion, but the available data are insufficient to confirm this. We label it as a candidate radial velocity variable. For the remainder of the sample, these observations exclude the presence of any &#8216;hot&#8217; (P &lt; 3 days) companions more massive than 8 MJup, and any &#039;warm&#039; (P &lt; 30 days) companions more massive than 17 MJup, on average. Assuming an edge-on orbit for the edge-on disk system AU Mic, these observations exclude the presence of any hot Jupiters more massive than 1.8 MJup or warm Jupiters more massive than 3.9 MJup.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Bayesian mixture models for Poisson astronomical images</title>
		<link>http://voxcharta.org/2012/02/02/bayesian-mixture-models-for-poisson-astronomical-images/</link>
		<comments>http://voxcharta.org/2012/02/02/bayesian-mixture-models-for-poisson-astronomical-images/#comments</comments>
		<pubDate>Fri, 03 Feb 2012 01:50:25 +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[algorithm]]></category>
		<category><![CDATA[astronomical image]]></category>
		<category><![CDATA[background source]]></category>
		<category><![CDATA[chandra data]]></category>
		<category><![CDATA[cosmic background]]></category>
		<category><![CDATA[electromagnetic spectrum]]></category>
		<category><![CDATA[estimation]]></category>
		<category><![CDATA[feasibility study]]></category>
		<category><![CDATA[incompleteness]]></category>
		<category><![CDATA[intensity]]></category>
		<category><![CDATA[mixture model]]></category>
		<category><![CDATA[poisson statistics]]></category>
		<category><![CDATA[regime]]></category>
		<category><![CDATA[rosat]]></category>
		<category><![CDATA[separation technique]]></category>
		<category><![CDATA[source detection]]></category>
		<category><![CDATA[source separation]]></category>
		<category><![CDATA[steep gradient]]></category>
		<category><![CDATA[uncertainty]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/02/bayesian-mixture-models-for-poisson-astronomical-images/</guid>
		<description><![CDATA[Astronomical images in the Poisson regime are typically characterized by a spatially varying cosmic background, large variety of source morphologies and intensities, data incompleteness, steep gradients in the data, and few photon counts per pixel. The Background-Source separation technique is developed with the aim to detect faint and extended sources in astronomical images characterized by [...]]]></description>
			<content:encoded><![CDATA[<p>Astronomical images in the Poisson regime are typically characterized by a spatially varying cosmic background, large variety of source morphologies and intensities, data incompleteness, steep gradients in the data, and few photon counts per pixel. The Background-Source separation technique is developed with the aim to detect faint and extended sources in astronomical images characterized by Poisson statistics. The technique employs Bayesian mixture models to reliably detect the background as well as the sources with their respective uncertainties. Background estimation and source detection is achieved in a single algorithm. A large variety of source morphologies is revealed. The technique is applied in the X-ray part of the electromagnetic spectrum on ROSAT and Chandra data sets and it is under a feasibility study for the forthcoming eROSITA mission.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Applying the Background-Source separation algorithm to Chandra Deep Field South data</title>
		<link>http://voxcharta.org/2012/02/02/applying-the-background-source-separation-algorithm-to-chandra-deep-field-south-data/</link>
		<comments>http://voxcharta.org/2012/02/02/applying-the-background-source-separation-algorithm-to-chandra-deep-field-south-data/#comments</comments>
		<pubDate>Fri, 03 Feb 2012 01:50:00 +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[angular resolution]]></category>
		<category><![CDATA[background source]]></category>
		<category><![CDATA[celestial source]]></category>
		<category><![CDATA[Chandra]]></category>
		<category><![CDATA[diffuse background]]></category>
		<category><![CDATA[exposure time]]></category>
		<category><![CDATA[mixture model]]></category>
		<category><![CDATA[morphological parameters]]></category>
		<category><![CDATA[multi resolution analysis]]></category>
		<category><![CDATA[probability maps]]></category>
		<category><![CDATA[satellite]]></category>
		<category><![CDATA[source position]]></category>
		<category><![CDATA[source separation]]></category>
		<category><![CDATA[step algorithm]]></category>
		<category><![CDATA[thin plate]]></category>
		<category><![CDATA[time source]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/02/applying-the-background-source-separation-algorithm-to-chandra-deep-field-south-data/</guid>
		<description><![CDATA[A probabilistic two-component mixture model allows one to separate the diffuse background from the celestial sources within a one-step algorithm without data censoring. The background is modeled with a thin-plate spline combined with the satellite&#8217;s exposure time. Source probability maps are created in a multi-resolution analysis for revealing faint and extended sources. All detected sources [...]]]></description>
			<content:encoded><![CDATA[<p>A probabilistic two-component mixture model allows one to separate the diffuse background from the celestial sources within a one-step algorithm without data censoring. The background is modeled with a thin-plate spline combined with the satellite&#8217;s exposure time. Source probability maps are created in a multi-resolution analysis for revealing faint and extended sources. All detected sources are automatically parametrized to produce a list of source positions, fluxes and morphological parameters. The present analysis is applied to the Chandra Deep Field South 2 Ms public released data. Within its 1.884 ks of exposure time and its angular resolution (0.984 arcsec), the Chandra Deep Field South data are particularly suited for testing the Background-Source separation algorithm.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/02/applying-the-background-source-separation-algorithm-to-chandra-deep-field-south-data/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Gaia Universe Model Snapshot : A statistical analysis of the expected contents of the Gaia catalogue [Replacement]</title>
		<link>http://voxcharta.org/2012/02/02/gaia-universe-model-snapshot-a-statistical-analysis-of-the-expected-contents-of-the-gaia-catalogue-replacement/</link>
		<comments>http://voxcharta.org/2012/02/02/gaia-universe-model-snapshot-a-statistical-analysis-of-the-expected-contents-of-the-gaia-catalogue-replacement/#comments</comments>
		<pubDate>Fri, 03 Feb 2012 01:31:20 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[computational simulations]]></category>
		<category><![CDATA[detection efficiency]]></category>
		<category><![CDATA[dpac]]></category>
		<category><![CDATA[exoplanet]]></category>
		<category><![CDATA[gaia portal]]></category>
		<category><![CDATA[instrumental effects]]></category>
		<category><![CDATA[level observations]]></category>
		<category><![CDATA[model snapshot]]></category>
		<category><![CDATA[multiple star]]></category>
		<category><![CDATA[multiple star systems]]></category>
		<category><![CDATA[quasar]]></category>
		<category><![CDATA[rssd]]></category>
		<category><![CDATA[spectroscopic]]></category>
		<category><![CDATA[statistical analysis]]></category>
		<category><![CDATA[stellar content]]></category>
		<category><![CDATA[supernovas]]></category>
		<category><![CDATA[taking into consideration]]></category>
		<category><![CDATA[universe model]]></category>
		<category><![CDATA[variability]]></category>
		<category><![CDATA[variable star]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/02/gaia-universe-model-snapshot-a-statistical-analysis-of-the-expected-contents-of-the-gaia-catalogue-replacement/</guid>
		<description><![CDATA[Context. This study has been developed in the framework of the computational simulations executed for the preparation of the ESA Gaia astrometric mission. Aims. We focus on describing the objects and characteristics that Gaia will potentially observe without taking into consideration instrumental effects (detection efficiency, observing errors). Methods. The theoretical Universe Model prepared for the [...]]]></description>
			<content:encoded><![CDATA[<p>Context. This study has been developed in the framework of the computational simulations executed for the preparation of the ESA Gaia astrometric mission. Aims. We focus on describing the objects and characteristics that Gaia will potentially observe without taking into consideration instrumental effects (detection efficiency, observing errors). Methods. The theoretical Universe Model prepared for the Gaia simulation has been statistically analyzed at a given time. Ingredients of the model are described, giving most attention to the stellar content, the double and multiple stars, and variability. Results. In this simulation the errors have not been included yet. Hence we estimate the number of objects and their theoretical photometric, astrometric and spectroscopic characteristics in the case that they are perfectly detected. We show that Gaia will be able to potentially observe 1.1 billion of stars (single or part of multiple star systems) of which about 2% are variable stars, 3% have one or two exoplanets. At the extragalactic level, observations will be potentially composed by several millions of galaxies, half million to 1 million of quasars and about 50,000 supernovas that will occur during the 5 years of mission. The simulated catalogue will be made publicly available by the DPAC on the Gaia portal of the ESA web site <a href="http://www.rssd.esa.int/gaia/.">http://www.rssd.esa.int/gaia/.</a></p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/02/gaia-universe-model-snapshot-a-statistical-analysis-of-the-expected-contents-of-the-gaia-catalogue-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The GJ 436 System: Directly Determined Astrophysical Parameters of an M-Dwarf and Implications for the Transiting Hot Neptune</title>
		<link>http://voxcharta.org/2012/02/01/the-gj-436-system-directly-determined-astrophysical-parameters-of-an-m-dwarf-and-implications-for-the-transiting-hot-neptune/</link>
		<comments>http://voxcharta.org/2012/02/01/the-gj-436-system-directly-determined-astrophysical-parameters-of-an-m-dwarf-and-implications-for-the-transiting-hot-neptune/#comments</comments>
		<pubDate>Thu, 02 Feb 2012 01:46:58 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[curves]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[diameter]]></category>
		<category><![CDATA[efficiency]]></category>
		<category><![CDATA[gj 436]]></category>
		<category><![CDATA[light curve]]></category>
		<category><![CDATA[literature]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[neptune]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[planetary atmosphere]]></category>
		<category><![CDATA[planetary mass]]></category>
		<category><![CDATA[radius]]></category>
		<category><![CDATA[redistribution]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[stellar parameters]]></category>
		<category><![CDATA[system parameter]]></category>
		<category><![CDATA[time series data]]></category>
		<category><![CDATA[type dwarf]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/01/the-gj-436-system-directly-determined-astrophysical-parameters-of-an-m-dwarf-and-implications-for-the-transiting-hot-neptune/</guid>
		<description><![CDATA[The late-type dwarf GJ 436 is known to host a transiting Neptune-mass planet in a 2.6-day orbit. We present results of our interferometric measurements to directly determine the stellar diameter ($R_{\star} = 0.455 \pm 0.018 R_{\odot}$) and effective temperature ($T_{\rm EFF} = 3416 \pm 54$ K). We combine our stellar parameters with literature time-series data, [...]]]></description>
			<content:encoded><![CDATA[<p>The late-type dwarf GJ 436 is known to host a transiting Neptune-mass planet in a 2.6-day orbit. We present results of our interferometric measurements to directly determine the stellar diameter ($R_{\star} = 0.455 \pm 0.018 R_{\odot}$) and effective temperature ($T_{\rm EFF} = 3416 \pm 54$ K). We combine our stellar parameters with literature time-series data, which allows us to calculate physical and orbital system parameters, including GJ 436&#8217;s stellar mass ($M_{\star} = 0.472^{+ 0.0636}_{- 0.0566} M_{\odot}$), planetary radius ($R_{p} = 0.370^{+ 0.0149}_{- 0.0145} R_{Jupiter}$), planetary mass ($M_{p} = 0.075^{+ 0.0076}_{- 0.0072} M_{Jupiter}$), implying a mean planetary density of $\rho_{p} = 1.48^{+ 0.116}_{- 0.103} \rho_{Jupiter}$. These values are generally in good agreement with previous literature estimates based on assumed stellar mass and photometric light curve fitting. Finally, we examine the expected phase curves of the hot Neptune GJ 436b, based on various assumptions concerning the efficiency of energy redistribution in the planetary atmosphere, and find that it could be constrained with {\it Spitzer} monitoring observations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/01/the-gj-436-system-directly-determined-astrophysical-parameters-of-an-m-dwarf-and-implications-for-the-transiting-hot-neptune/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Dithering Strategies and Point-Source Photometry</title>
		<link>http://voxcharta.org/2012/02/01/dithering-strategies-and-point-source-photometry/</link>
		<comments>http://voxcharta.org/2012/02/01/dithering-strategies-and-point-source-photometry/#comments</comments>
		<pubDate>Thu, 02 Feb 2012 01:45:00 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accuracy]]></category>
		<category><![CDATA[distributions]]></category>
		<category><![CDATA[dither]]></category>
		<category><![CDATA[hardware configuration]]></category>
		<category><![CDATA[image reconstruction]]></category>
		<category><![CDATA[offsets]]></category>
		<category><![CDATA[pixel scale]]></category>
		<category><![CDATA[pixelization]]></category>
		<category><![CDATA[point source]]></category>
		<category><![CDATA[point spread function]]></category>
		<category><![CDATA[position determination]]></category>
		<category><![CDATA[psf]]></category>
		<category><![CDATA[rms]]></category>
		<category><![CDATA[rms value]]></category>
		<category><![CDATA[scales]]></category>
		<category><![CDATA[source flux]]></category>
		<category><![CDATA[spatial sampling]]></category>
		<category><![CDATA[survey source]]></category>
		<category><![CDATA[uncertainty]]></category>
		<category><![CDATA[wide field imaging]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/01/dithering-strategies-and-point-source-photometry/</guid>
		<description><![CDATA[The accuracy in the photometry of a point source depends on the point-spread function (PSF), detector pixelization, and observing strategy. The PSF and pixel response describe the spatial blurring of the source, the pixel scale describes the spatial sampling of a single exposure, and the observing strategy determines the set of dithered exposures with pointing [...]]]></description>
			<content:encoded><![CDATA[<p>The accuracy in the photometry of a point source depends on the point-spread function (PSF), detector pixelization, and observing strategy. The PSF and pixel response describe the spatial blurring of the source, the pixel scale describes the spatial sampling of a single exposure, and the observing strategy determines the set of dithered exposures with pointing offsets from which the source flux is inferred. In a wide-field imaging survey, sources of interest are randomly distributed within the field of view and hence are centered randomly within a pixel. A given hardware configuration and observing strategy therefore have a distribution of photometric uncertainty for sources of fixed flux that fall in the field. In this article we explore the ensemble behavior of photometric and position accuracies for different PSFs, pixel scales, and dithering patterns. We find that the average uncertainty in the flux determination depends slightly on dither strategy, whereas the position determination can be strongly dependent on the dithering. For cases with pixels much larger than the PSF, the uncertainty distributions can be non-Gaussian, with rms values that are particularly sensitive to the dither strategy. We also find that for these configurations with large pixels, pointings dithered by a fractional pixel amount do not always give minimal average uncertainties; this is in contrast to image reconstruction for which fractional dithers are optimal. When fractional pixel dithering is favored, a pointing accuracy of better than $\sim 0.15$ pixel width is required to maintain half the advantage over random dithers.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/01/dithering-strategies-and-point-source-photometry/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Gaia Universe Model Snapshot : A statistical analysis of the expected contents of the Gaia catalogue</title>
		<link>http://voxcharta.org/2012/02/01/gaia-universe-model-snapshot-a-statistical-analysis-of-the-expected-contents-of-the-gaia-catalogue/</link>
		<comments>http://voxcharta.org/2012/02/01/gaia-universe-model-snapshot-a-statistical-analysis-of-the-expected-contents-of-the-gaia-catalogue/#comments</comments>
		<pubDate>Thu, 02 Feb 2012 01:43:00 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[computational simulations]]></category>
		<category><![CDATA[detection efficiency]]></category>
		<category><![CDATA[dpac]]></category>
		<category><![CDATA[exoplanet]]></category>
		<category><![CDATA[gaia portal]]></category>
		<category><![CDATA[instrumental effects]]></category>
		<category><![CDATA[level observations]]></category>
		<category><![CDATA[model snapshot]]></category>
		<category><![CDATA[multiple star]]></category>
		<category><![CDATA[multiple star systems]]></category>
		<category><![CDATA[quasar]]></category>
		<category><![CDATA[rssd]]></category>
		<category><![CDATA[spectroscopic]]></category>
		<category><![CDATA[statistical analysis]]></category>
		<category><![CDATA[stellar content]]></category>
		<category><![CDATA[supernovas]]></category>
		<category><![CDATA[taking into consideration]]></category>
		<category><![CDATA[universe model]]></category>
		<category><![CDATA[variability]]></category>
		<category><![CDATA[variable star]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/01/gaia-universe-model-snapshot-a-statistical-analysis-of-the-expected-contents-of-the-gaia-catalogue/</guid>
		<description><![CDATA[Context. This study has been developed in the framework of the computational simulations executed for the preparation of the ESA Gaia astrometric mission. Aims. We focus on describing the objects and characteristics that Gaia will potentially observe without taking into consideration instrumental effects (detection efficiency, observing errors). Methods. The theoretical Universe Model prepared for the [...]]]></description>
			<content:encoded><![CDATA[<p>Context. This study has been developed in the framework of the computational simulations executed for the preparation of the ESA Gaia astrometric mission. Aims. We focus on describing the objects and characteristics that Gaia will potentially observe without taking into consideration instrumental effects (detection efficiency, observing errors). Methods. The theoretical Universe Model prepared for the Gaia simulation has been statistically analyzed at a given time. Ingredients of the model are described, giving most attention to the stellar content, the double and multiple stars, and variability. Results. In this simulation the errors have not been included yet. Hence we estimate the number of objects and their theoretical photometric, astrometric and spectroscopic characteristics in the case that they are perfectly detected. We show that Gaia will be able to potentially observe 1.1 billion of stars (single or part of multiple star systems) of which about 2% are variable stars, 3% have one or two exoplanets. At the extragalactic level, observations will be potentially composed by several millions of galaxies, half million to 1 million of quasars and about 50,000 supernovas that will occur during the 5 years of mission. The simulated catalogue will be made publicly available by the DPAC on the Gaia portal of the ESA web site <a href="http://www.rssd.esa.int/gaia/.">http://www.rssd.esa.int/gaia/.</a></p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/01/gaia-universe-model-snapshot-a-statistical-analysis-of-the-expected-contents-of-the-gaia-catalogue/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Estimations of the Distances of Stellar Collapses in the Galaxy by Analyzing the Energy Spectrum of Neutrino Bursts</title>
		<link>http://voxcharta.org/2012/02/01/estimations-of-the-distances-of-stellar-collapses-in-the-galaxy-by-analyzing-the-energy-spectrum-of-neutrino-bursts/</link>
		<comments>http://voxcharta.org/2012/02/01/estimations-of-the-distances-of-stellar-collapses-in-the-galaxy-by-analyzing-the-energy-spectrum-of-neutrino-bursts/#comments</comments>
		<pubDate>Thu, 02 Feb 2012 01:40:23 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[alternative methods]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[burst]]></category>
		<category><![CDATA[collapse]]></category>
		<category><![CDATA[distance]]></category>
		<category><![CDATA[energy spectrum]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gravitational binding energy]]></category>
		<category><![CDATA[neutrino data]]></category>
		<category><![CDATA[neutrino telescope]]></category>
		<category><![CDATA[optical counterpart]]></category>
		<category><![CDATA[preliminary results]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectral shape]]></category>
		<category><![CDATA[supernova explosion]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/01/estimations-of-the-distances-of-stellar-collapses-in-the-galaxy-by-analyzing-the-energy-spectrum-of-neutrino-bursts/</guid>
		<description><![CDATA[The neutrino telescopes of the present generation, depending on their specific features, can reconstruct the neutrino spectra from a galactic burst. Since the optical counterpart could be not available, it is desirable to have at hand alternative methods to estimate the distance of the supernova explosion using only the neutrino data. In this work we [...]]]></description>
			<content:encoded><![CDATA[<p>The neutrino telescopes of the present generation, depending on their specific features, can reconstruct the neutrino spectra from a galactic burst. Since the optical counterpart could be not available, it is desirable to have at hand alternative methods to estimate the distance of the supernova explosion using only the neutrino data. In this work we present preliminary results on the method we are proposing to estimate the distance from a galactic supernova based only on the spectral shape of the neutrino burst and assumptions on the gravitational binding energy released an a typical supernova explosion due to stellar collapses.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/01/estimations-of-the-distances-of-stellar-collapses-in-the-galaxy-by-analyzing-the-energy-spectrum-of-neutrino-bursts/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Improved visual detection of moving objects in astronomical images using color intensity projections with hue cycling</title>
		<link>http://voxcharta.org/2012/02/01/improved-visual-detection-of-moving-objects-in-astronomical-images-using-color-intensity-projections-with-hue-cycling/</link>
		<comments>http://voxcharta.org/2012/02/01/improved-visual-detection-of-moving-objects-in-astronomical-images-using-color-intensity-projections-with-hue-cycling/#comments</comments>
		<pubDate>Thu, 02 Feb 2012 01:36:57 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[algorithm]]></category>
		<category><![CDATA[artefact]]></category>
		<category><![CDATA[astronomical image]]></category>
		<category><![CDATA[ccd]]></category>
		<category><![CDATA[color image]]></category>
		<category><![CDATA[color intensity]]></category>
		<category><![CDATA[dead time]]></category>
		<category><![CDATA[exposure images]]></category>
		<category><![CDATA[fixed background]]></category>
		<category><![CDATA[flyby]]></category>
		<category><![CDATA[greyscale images]]></category>
		<category><![CDATA[hue]]></category>
		<category><![CDATA[intuitive way]]></category>
		<category><![CDATA[kuiper belt object]]></category>
		<category><![CDATA[moving objects]]></category>
		<category><![CDATA[new horizon]]></category>
		<category><![CDATA[pluto]]></category>
		<category><![CDATA[spacecraft]]></category>
		<category><![CDATA[subaru telescope]]></category>
		<category><![CDATA[test case]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/01/improved-visual-detection-of-moving-objects-in-astronomical-images-using-color-intensity-projections-with-hue-cycling/</guid>
		<description><![CDATA[While fully automated methods for detecting faint moving objects in astronomical images &#8211; such as Kuiper belt objects (KBOs) &#8211; are constantly improving, visual detection still has a role to play especially when the fixed background is cluttered with stars. Color intensity projections (CIPs) using hue cycling &#8211; which combines a sequence of greyscale images [...]]]></description>
			<content:encoded><![CDATA[<p>While fully automated methods for detecting faint moving objects in astronomical images &#8211; such as Kuiper belt objects (KBOs) &#8211; are constantly improving, visual detection still has a role to play especially when the fixed background is cluttered with stars. Color intensity projections (CIPs) using hue cycling &#8211; which combines a sequence of greyscale images into a single color image &#8211; aids in the visual detection of moving objects by highlighting them using color in an intuitive way. To demonstrate the usefulness of CIPs in detecting faint moving objects a sequence of 16 images from the SuprimeCam camera of the Subaru telescope were combined into a CIPs image. As well has making even faint moving objects easier to visually detect against a cluttered background, CCD artefacts were also more easily recognisable. The new Hyper SuprimeCam for the Subaru telescope &#8211; which will allow many short exposure images to be acquired with little dead time between images &#8211; should provide ideal data for use with the CIPs algorithm. In addition, the current search for KBOs to be targeted by the New Horizon&#8217;s spacecraft after its flyby of Pluto provides an excellent test case for the state of the art in faint moving object detection against a cluttered background.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/01/improved-visual-detection-of-moving-objects-in-astronomical-images-using-color-intensity-projections-with-hue-cycling/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Solving systems of transcendental equations involving the Heun functions [Replacement]</title>
		<link>http://voxcharta.org/2012/02/01/solving-systems-of-transcendental-equations-involving-the-heun-functions-replacement/</link>
		<comments>http://voxcharta.org/2012/02/01/solving-systems-of-transcendental-equations-involving-the-heun-functions-replacement/#comments</comments>
		<pubDate>Thu, 02 Feb 2012 01:31:53 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[21st century]]></category>
		<category><![CDATA[algorithm]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[complex variable]]></category>
		<category><![CDATA[extent]]></category>
		<category><![CDATA[filling the gaps]]></category>
		<category><![CDATA[heun]]></category>
		<category><![CDATA[kerr]]></category>
		<category><![CDATA[master equation]]></category>
		<category><![CDATA[modern physics]]></category>
		<category><![CDATA[modes]]></category>
		<category><![CDATA[Newton]]></category>
		<category><![CDATA[nonlinear]]></category>
		<category><![CDATA[numerical result]]></category>
		<category><![CDATA[numerical work]]></category>
		<category><![CDATA[qnm]]></category>
		<category><![CDATA[regge]]></category>
		<category><![CDATA[transcendental equation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/01/solving-systems-of-transcendental-equations-involving-the-heun-functions-replacement/</guid>
		<description><![CDATA[The Heun functions have wide application in modern physics and are expected to succeed the hypergeometrical functions in the physical problems of the 21st century. The numerical work with those functions, however, is complicated and requires filling the gaps in the theory of the Heun functions and also, creating new algorithms able to work with [...]]]></description>
			<content:encoded><![CDATA[<p>The Heun functions have wide application in modern physics and are expected to succeed the hypergeometrical functions in the physical problems of the 21st century. The numerical work with those functions, however, is complicated and requires filling the gaps in the theory of the Heun functions and also, creating new algorithms able to work with them efficiently.   We propose a new algorithm for solving a system of two nonlinear transcendental equations with two complex variables based on the M\&#8221;uller algorithm. The new algorithm is particularly useful in systems featuring the Heun functions and for them, the new algorithm gives distinctly better results than Newton&#8217;s and Broyden&#8217;s methods.   As an example for its application in physics, the new algorithm was used to find the quasi-normal modes (QNM) of Schwarzschild black hole described by the Regge-Wheeler equation. The numerical results obtained by our method are compared with the already published QNM frequencies and are found to coincide to a great extent with them. Also discussed are the QNM of the Kerr black hole, described by the Teukolsky Master equation.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/01/solving-systems-of-transcendental-equations-involving-the-heun-functions-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The relative significance of the H-index [Replacement]</title>
		<link>http://voxcharta.org/2012/02/01/the-relative-significance-of-the-h-index-replacement/</link>
		<comments>http://voxcharta.org/2012/02/01/the-relative-significance-of-the-h-index-replacement/#comments</comments>
		<pubDate>Thu, 02 Feb 2012 01:31:30 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astrophysics]]></category>
		<category><![CDATA[citation]]></category>
		<category><![CDATA[gross measure]]></category>
		<category><![CDATA[hirsch]]></category>
		<category><![CDATA[literature]]></category>
		<category><![CDATA[relative significance]]></category>
		<category><![CDATA[theoretical reasoning]]></category>
		<category><![CDATA[visibility]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/02/01/the-relative-significance-of-the-h-index-replacement/</guid>
		<description><![CDATA[Use of the Hirsch-index ($h$) as measure of an author&#8217;s visibility in the scientific literature has become popular as an alternative to a gross measure like total citations (c). I show that, at least in astrophysics, $h$ correlates tightly with overall citations. The mean relation is $h=0.5(\sqrt c+1)$. Outliers are few and not too far [...]]]></description>
			<content:encoded><![CDATA[<p>Use of the Hirsch-index ($h$) as measure of an author&#8217;s visibility in the scientific literature has become popular as an alternative to a gross measure like total citations (c). I show that, at least in astrophysics, $h$ correlates tightly with overall citations. The mean relation is $h=0.5(\sqrt c+1)$. Outliers are few and not too far from the mean, especially if `normalized&#8217; ADS citations are used for $c$ and $h$. Whatever the theoretical reasoning behind it, the Hirsch index in practice does not appear to measure something significantly new.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/02/01/the-relative-significance-of-the-h-index-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Technology Development for the Caltech Submillimeter Observatory Balanced Receivers</title>
		<link>http://voxcharta.org/2012/01/31/technology-development-for-the-caltech-submillimeter-observatory-balanced-receivers/</link>
		<comments>http://voxcharta.org/2012/01/31/technology-development-for-the-caltech-submillimeter-observatory-balanced-receivers/#comments</comments>
		<pubDate>Wed, 01 Feb 2012 01:53:57 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[atmospheric window]]></category>
		<category><![CDATA[balanced mixer]]></category>
		<category><![CDATA[caltech submillimeter observatory]]></category>
		<category><![CDATA[cso]]></category>
		<category><![CDATA[dual frequency]]></category>
		<category><![CDATA[facility instrumentation]]></category>
		<category><![CDATA[good weather]]></category>
		<category><![CDATA[incoming signal]]></category>
		<category><![CDATA[integrations]]></category>
		<category><![CDATA[line survey]]></category>
		<category><![CDATA[mauna kea]]></category>
		<category><![CDATA[mauna kea hawaii]]></category>
		<category><![CDATA[observation mode]]></category>
		<category><![CDATA[polarization]]></category>
		<category><![CDATA[receivers]]></category>
		<category><![CDATA[spectral line]]></category>
		<category><![CDATA[stage of development]]></category>
		<category><![CDATA[technology development]]></category>
		<category><![CDATA[throughput]]></category>
		<category><![CDATA[weather condition]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/31/technology-development-for-the-caltech-submillimeter-observatory-balanced-receivers/</guid>
		<description><![CDATA[The Caltech Submillimeter Observatory (CSO) is located on top of Mauna Kea, Hawaii, at an altitude of 4.2 km. The existing suite of facility heterodyne receivers covering the submillimeter band is rapidly aging and in need of replacement. To facilitate deep integrations and automated spectral line surveys, a family of remote programmable, synthesized, dual-frequency balanced [...]]]></description>
			<content:encoded><![CDATA[<p>The Caltech Submillimeter Observatory (CSO) is located on top of Mauna Kea, Hawaii, at an altitude of 4.2 km. The existing suite of facility heterodyne receivers covering the submillimeter band is rapidly aging and in need of replacement. To facilitate deep integrations and automated spectral line surveys, a family of remote programmable, synthesized, dual-frequency balanced receivers covering the astronomical important 180 &#8211; 720 GHz atmospheric windows is in an advanced stage of development. Installation of the first set of receivers is expected in the spring of 2012.   Dual-frequency observation will be an important mode of operation offered by the new facility instrumentation. Two band observations are accomplished by separating the H and V polarizations of the incoming signal and routing them via folded optics to the appropriate polarization sensitive balanced mixer. Scientifically this observation mode facilitates pointing for the higher receiver band under mediocre weather conditions and a doubling of scientific throughput (2 x 4 GHz) under good weather conditions.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/31/technology-development-for-the-caltech-submillimeter-observatory-balanced-receivers/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Low frequency seeing and solar diameter measurements</title>
		<link>http://voxcharta.org/2012/01/31/low-frequency-seeing-and-solar-diameter-measurements/</link>
		<comments>http://voxcharta.org/2012/01/31/low-frequency-seeing-and-solar-diameter-measurements/#comments</comments>
		<pubDate>Wed, 01 Feb 2012 01:49:12 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[diameter measurement]]></category>
		<category><![CDATA[drift scan]]></category>
		<category><![CDATA[evidences]]></category>
		<category><![CDATA[image motion]]></category>
		<category><![CDATA[low frequency]]></category>
		<category><![CDATA[solar diameter]]></category>
		<category><![CDATA[Sun]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/31/low-frequency-seeing-and-solar-diameter-measurements/</guid>
		<description><![CDATA[The action of the atmospheric seeing is blurring, image stretching and image motion. This happens even to the image of the Sun which is more than half degree wide. Low frequency seeing components affect the solar diameter values measured either throught the drift-scan or the heliometer methods. We present evidences of image motion and stretching [...]]]></description>
			<content:encoded><![CDATA[<p>The action of the atmospheric seeing is blurring, image stretching and image motion. This happens even to the image of the Sun which is more than half degree wide. Low frequency seeing components affect the solar diameter values measured either throught the drift-scan or the heliometer methods. We present evidences of image motion and stretching down to 0.01 Hz.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/31/low-frequency-seeing-and-solar-diameter-measurements/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Detection of radiation pressure from solar chameleons</title>
		<link>http://voxcharta.org/2012/01/31/detection-of-radiation-pressure-from-solar-chameleons/</link>
		<comments>http://voxcharta.org/2012/01/31/detection-of-radiation-pressure-from-solar-chameleons/#comments</comments>
		<pubDate>Wed, 01 Feb 2012 01:47:19 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[antenna]]></category>
		<category><![CDATA[chameleon]]></category>
		<category><![CDATA[detection of radiation]]></category>
		<category><![CDATA[fabry perot]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[photon radiation]]></category>
		<category><![CDATA[radiation pressure]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/31/detection-of-radiation-pressure-from-solar-chameleons/</guid>
		<description><![CDATA[The radiation pressure due to reflected chameleons is suggested for their detection. Sensitive photon radiation pressure or force measuring techniques could become the new antennas for chameleons or other particles with similar properties, with gravitational waves antennas being also of potential interest. This is eventually only at first sight a Gedankenexperiment. Also chameleon-through-a-wall experiments, in [...]]]></description>
			<content:encoded><![CDATA[<p>The radiation pressure due to reflected chameleons is suggested for their detection. Sensitive photon radiation pressure or force measuring techniques could become the new antennas for chameleons or other particles with similar properties, with gravitational waves antennas being also of potential interest. This is eventually only at first sight a Gedankenexperiment. Also chameleon-through-a-wall experiments, in particular when equipped with a Fabry-Perot resonator, could apply the suggested techniques.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/31/detection-of-radiation-pressure-from-solar-chameleons/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Limits on the Stochastic Gravitational Wave Background from the North American Nanohertz Observatory for Gravitational Waves</title>
		<link>http://voxcharta.org/2012/01/31/limits-on-the-stochastic-gravitational-wave-background-from-the-north-american-nanohertz-observatory-for-gravitational-waves/</link>
		<comments>http://voxcharta.org/2012/01/31/limits-on-the-stochastic-gravitational-wave-background-from-the-north-american-nanohertz-observatory-for-gravitational-waves/#comments</comments>
		<pubDate>Wed, 01 Feb 2012 01:42:41 +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[arecibo radio]]></category>
		<category><![CDATA[best root]]></category>
		<category><![CDATA[dataset]]></category>
		<category><![CDATA[dispersion]]></category>
		<category><![CDATA[fluctuation]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[gravitational wave signal]]></category>
		<category><![CDATA[observatory]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[pulsars]]></category>
		<category><![CDATA[pulse shape]]></category>
		<category><![CDATA[radio telescope]]></category>
		<category><![CDATA[residuals]]></category>
		<category><![CDATA[span]]></category>
		<category><![CDATA[spectral shape]]></category>
		<category><![CDATA[supermassive black hole]]></category>
		<category><![CDATA[timing model]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/31/limits-on-the-stochastic-gravitational-wave-background-from-the-north-american-nanohertz-observatory-for-gravitational-waves/</guid>
		<description><![CDATA[We present an analysis of high-precision pulsar timing data taken as part of the North American Nanohertz Observatory for Gravitational waves (NANOGrav) project. We have observed 17 pulsars for a span of roughly five years using the Green Bank and Arecibo radio telescopes. We analyze these data using standard pulsar timing models, with the addition [...]]]></description>
			<content:encoded><![CDATA[<p>We present an analysis of high-precision pulsar timing data taken as part of the North American Nanohertz Observatory for Gravitational waves (NANOGrav) project. We have observed 17 pulsars for a span of roughly five years using the Green Bank and Arecibo radio telescopes. We analyze these data using standard pulsar timing models, with the addition of time-variable dispersion measure and frequency-variable pulse shape terms. Sub-microsecond timing residuals are obtained in nearly all cases, and the best root-mean-square timing residuals in this set are ~30-50 ns. We present methods for analyzing post-fit timing residuals for the presence of a gravitational wave signal with a specified spectral shape. These optimally take into account the timing fluctuation power removed by the model fit, and can be applied to either data from a single pulsar, or to a set of pulsars to detect a correlated signal. We apply these methods to our dataset to set an upper limit on the strength of the nHz-frequency stochastic supermassive black hole gravitational wave background of h_c (1 yr^-1) &lt; 7&#215;10^-15 (95%). This result is dominated by the timing of the two best pulsars in the set, PSRs J1713+0747 and J1909-3744.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/31/limits-on-the-stochastic-gravitational-wave-background-from-the-north-american-nanohertz-observatory-for-gravitational-waves/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Kernel PCA for type Ia supernovae photometric classification</title>
		<link>http://voxcharta.org/2012/01/31/kernel-pca-for-type-ia-supernovae-photometric-classification/</link>
		<comments>http://voxcharta.org/2012/01/31/kernel-pca-for-type-ia-supernovae-photometric-classification/#comments</comments>
		<pubDate>Wed, 01 Feb 2012 01:40:58 +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[bia]]></category>
		<category><![CDATA[classification rate]]></category>
		<category><![CDATA[classification results]]></category>
		<category><![CDATA[classifier]]></category>
		<category><![CDATA[counterpart]]></category>
		<category><![CDATA[figure of merit]]></category>
		<category><![CDATA[fom]]></category>
		<category><![CDATA[information results]]></category>
		<category><![CDATA[kernel]]></category>
		<category><![CDATA[kpca]]></category>
		<category><![CDATA[light curve]]></category>
		<category><![CDATA[nearest neighbor algorithm]]></category>
		<category><![CDATA[pca]]></category>
		<category><![CDATA[probability]]></category>
		<category><![CDATA[purity]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[snr]]></category>
		<category><![CDATA[transients]]></category>
		<category><![CDATA[type ia]]></category>
		<category><![CDATA[variables]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/31/kernel-pca-for-type-ia-supernovae-photometric-classification/</guid>
		<description><![CDATA[The problem of photometric identification will be extremely important for large surveys in the next decade. In this work, we propose the use of KPCA combined with k = 1 nearest neighbor algorithm (KPCA+1NN) as a framework for SNe photometric classification. The method does not rely on information about redshift or local enviromental variables, so [...]]]></description>
			<content:encoded><![CDATA[<p>The problem of photometric identification will be extremely important for large surveys in the next decade. In this work, we propose the use of KPCA combined with k = 1 nearest neighbor algorithm (KPCA+1NN) as a framework for SNe photometric classification. The method does not rely on information about redshift or local enviromental variables, so it is less sensitive to bias than its template fitting counterparts. We applied the method to $\approx$ 20000 SNe light curve released after the \textit{Supernova Photometric Classification Challenge} (SNPCC). Results for the photometric sample achieved up to 89% efficiency (eff), 97% purity (pur), 96% successful classification (SC) rates and figure of merit (FoM) of 0.79 (SNR$\geq$5). If we impose no SNR cuts, we obtain up to 64% eff, 43% pur, 46% SC and FoM of 0.10. We also present the classification results using only pre-maximum epoches, obtaining 80% eff, 73% pur, 84% SC and FoM of 0.32 (SNR$\geq$5). Comparing the performance of our classifier with MLCS2k2 fit probability, we demonstrate that KPCA+1NN is able to improve the classification results of MLCS2k up to $\approx 15%$ without the need of redshift information. Results are sensitive to the information contained in each light curve, as a consequence, higher quality the data points lead to higher successfull classification rates. The method is flexible enough to be applied to other astrophysical transients, as long as a training and a template sample are provided.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/31/kernel-pca-for-type-ia-supernovae-photometric-classification/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Gerbert of Aurillac: astronomy and geometry in tenth century Europe [Replacement]</title>
		<link>http://voxcharta.org/2012/01/31/gerbert-of-aurillac-astronomy-and-geometry-in-tenth-century-europe-replacement/</link>
		<comments>http://voxcharta.org/2012/01/31/gerbert-of-aurillac-astronomy-and-geometry-in-tenth-century-europe-replacement/#comments</comments>
		<pubDate>Wed, 01 Feb 2012 01:33:26 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abacus]]></category>
		<category><![CDATA[arabic numbers]]></category>
		<category><![CDATA[astronomer]]></category>
		<category><![CDATA[astronomical observation]]></category>
		<category><![CDATA[constantine]]></category>
		<category><![CDATA[didactical]]></category>
		<category><![CDATA[equatorial mount]]></category>
		<category><![CDATA[equilateral triangle area]]></category>
		<category><![CDATA[equinox]]></category>
		<category><![CDATA[fleury]]></category>
		<category><![CDATA[mathematician]]></category>
		<category><![CDATA[north celestial pole]]></category>
		<category><![CDATA[observing the sun]]></category>
		<category><![CDATA[organ builder]]></category>
		<category><![CDATA[polaris]]></category>
		<category><![CDATA[rational approximation]]></category>
		<category><![CDATA[silvester]]></category>
		<category><![CDATA[solstice]]></category>
		<category><![CDATA[tenth century]]></category>
		<category><![CDATA[xii century]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/31/gerbert-of-aurillac-astronomy-and-geometry-in-tenth-century-europe-replacement/</guid>
		<description><![CDATA[Gerbert of Aurillac was the most prominent personality of the tenth century: astronomer, organ builder and music theoretician, mathematician, philosopher, and finally pope with the name of Silvester II (999-1003). Gerbert introduced firstly the arabic numbers in Europe, invented an abacus for speeding the calculations and found a rational approximation for the equilateral triangle area, [...]]]></description>
			<content:encoded><![CDATA[<p>Gerbert of Aurillac was the most prominent personality of the tenth century: astronomer, organ builder and music theoretician, mathematician, philosopher, and finally pope with the name of Silvester II (999-1003). Gerbert introduced firstly the arabic numbers in Europe, invented an abacus for speeding the calculations and found a rational approximation for the equilateral triangle area, in the letter to Adelbold here discussed. Gerbert described a semi-sphere to Constantine of Fleury with built-in sighting tubes, used for astronomical observations. The procedure to identify the star nearest to the North celestial pole is very accurate and still in use in the XII century, when Computatrix was the name of Polaris. For didactical purposes the Polaris would have been precise enough and much less time consuming, but here Gerbert was clearly aligning a precise equatorial mount for a fixed instrument for accurate daytime observations. Through the sighting tubes it was possible to detect equinoxes and solstices by observing the Sun in the corresponding days. The horalogium of Magdeburg was probably a big and fixed-mount nocturlabe, always pointing the star near the celestial pole.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/31/gerbert-of-aurillac-astronomy-and-geometry-in-tenth-century-europe-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>ARCONS: a highly multiplexed superconducting UV to near-IR camera</title>
		<link>http://voxcharta.org/2012/01/30/arcons-a-highly-multiplexed-superconducting-uv-to-near-ir-camera/</link>
		<comments>http://voxcharta.org/2012/01/30/arcons-a-highly-multiplexed-superconducting-uv-to-near-ir-camera/#comments</comments>
		<pubDate>Tue, 31 Jan 2012 02:08:56 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[array camera]]></category>
		<category><![CDATA[arrival time]]></category>
		<category><![CDATA[coude focus]]></category>
		<category><![CDATA[heart]]></category>
		<category><![CDATA[inch hale telescope]]></category>
		<category><![CDATA[infrared spectrophotometry]]></category>
		<category><![CDATA[microwave]]></category>
		<category><![CDATA[palomar observatory]]></category>
		<category><![CDATA[pixel scale]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/30/arcons-a-highly-multiplexed-superconducting-uv-to-near-ir-camera/</guid>
		<description><![CDATA[ARCONS, the Array Camera for Optical to Near-infrared Spectrophotometry, was recently commissioned at the Coude focus of the 200-inch Hale Telescope at the Palomar Observatory. At the heart of this unique instrument is a 1024-pixel Microwave Kinetic Inductance Detector (MKID), exploiting the Kinetic Inductance effect to measure the energy of the incoming photon to better [...]]]></description>
			<content:encoded><![CDATA[<p>ARCONS, the Array Camera for Optical to Near-infrared Spectrophotometry, was recently commissioned at the Coude focus of the 200-inch Hale Telescope at the Palomar Observatory. At the heart of this unique instrument is a 1024-pixel Microwave Kinetic Inductance Detector (MKID), exploiting the Kinetic Inductance effect to measure the energy of the incoming photon to better than several percent. The ground-breaking instrument is lens-coupled with a pixel scale of 0.23&#8243;/pixel, with each pixel recording the arrival time (&lt;2 microsec) and energy of a photon (~10%) in the optical to near-IR (0.4-1.1 microns) range. The scientific objectives of the instrument include the rapid follow-up and classification of the transient phenomena.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/30/arcons-a-highly-multiplexed-superconducting-uv-to-near-ir-camera/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Gerbert of Aurillac: astronomy and geometry in tenth century Europe [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/01/30/gerbert-of-aurillac-astronomy-and-geometry-in-tenth-century-europe-cross-listing/</link>
		<comments>http://voxcharta.org/2012/01/30/gerbert-of-aurillac-astronomy-and-geometry-in-tenth-century-europe-cross-listing/#comments</comments>
		<pubDate>Tue, 31 Jan 2012 01:51:09 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abacus]]></category>
		<category><![CDATA[arabic numbers]]></category>
		<category><![CDATA[astronomer]]></category>
		<category><![CDATA[astronomical observation]]></category>
		<category><![CDATA[constantine]]></category>
		<category><![CDATA[didactical]]></category>
		<category><![CDATA[equatorial mount]]></category>
		<category><![CDATA[equilateral triangle area]]></category>
		<category><![CDATA[equinox]]></category>
		<category><![CDATA[fleury]]></category>
		<category><![CDATA[mathematician]]></category>
		<category><![CDATA[north celestial pole]]></category>
		<category><![CDATA[observing the sun]]></category>
		<category><![CDATA[organ builder]]></category>
		<category><![CDATA[polaris]]></category>
		<category><![CDATA[rational approximation]]></category>
		<category><![CDATA[silvester]]></category>
		<category><![CDATA[solstice]]></category>
		<category><![CDATA[tenth century]]></category>
		<category><![CDATA[xii century]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/30/gerbert-of-aurillac-astronomy-and-geometry-in-tenth-century-europe-cross-listing/</guid>
		<description><![CDATA[Gerbert of Aurillac was the most prominent personality of the tenth century: astronomer, organ builder and music theoretician, mathematician, philosopher, and finally pope with the name of Silvester II (999-1003). Gerbert introduced firstly the arabic numbers in Europe, invented an abacus for speeding the calculations and found a rational approximation for the equilateral triangle area, [...]]]></description>
			<content:encoded><![CDATA[<p>Gerbert of Aurillac was the most prominent personality of the tenth century: astronomer, organ builder and music theoretician, mathematician, philosopher, and finally pope with the name of Silvester II (999-1003). Gerbert introduced firstly the arabic numbers in Europe, invented an abacus for speeding the calculations and found a rational approximation for the equilateral triangle area, in the letter to Adelbold here discussed. Gerbert described a semi-sphere to Constantine of Fleury with built-in sighting tubes, used for astronomical observations. The procedure to identify the star nearest to the North celestial pole is very accurate and still in use in the XII century, when Computarix was the name of Polaris. For didactical purposes the Polaris would have been precise enough and much less time consuming, but here Gerbert was clearly aligning a precise equatorial mount for a fixed instrument for accurate daytime observations. Through the sighting tubes it was possible to detect equinoxes and solstices by observing the Sun in the corresponding days. The horalogium of Magdeburg was probably a big and fixed-mount nocturlabe, always pointing the star near the celestial pole.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/30/gerbert-of-aurillac-astronomy-and-geometry-in-tenth-century-europe-cross-listing/feed/</wfw:commentRss>
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		<item>
		<title>Probing neutralino dark matter in the MSSM &amp; the NMSSM with directional detection [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/01/30/probing-neutralino-dark-matter-in-the-mssm-the-nmssm-with-directional-detection-cross-listing/</link>
		<comments>http://voxcharta.org/2012/01/30/probing-neutralino-dark-matter-in-the-mssm-the-nmssm-with-directional-detection-cross-listing/#comments</comments>
		<pubDate>Tue, 31 Jan 2012 01:48:09 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[capability]]></category>
		<category><![CDATA[complementarity]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[direct search]]></category>
		<category><![CDATA[fundamental parameters]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[lhc]]></category>
		<category><![CDATA[mimac]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[mssm]]></category>
		<category><![CDATA[nucleon]]></category>
		<category><![CDATA[search technique]]></category>
		<category><![CDATA[spheroidal galaxy]]></category>
		<category><![CDATA[standard model]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/30/probing-neutralino-dark-matter-in-the-mssm-the-nmssm-with-directional-detection-cross-listing/</guid>
		<description><![CDATA[We investigate the capability of directional detectors to probe neutralino dark matter in the Minimal Supersymmetric Standard Model and the Next-to-Minimal Supersymmetric Standard Model with parameters defined at the weak scale. We show that directional detectors such as the future MIMAC detector will probe spin dependent dark matter scattering on nucleons that are beyond the [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate the capability of directional detectors to probe neutralino dark matter in the Minimal Supersymmetric Standard Model and the Next-to-Minimal Supersymmetric Standard Model with parameters defined at the weak scale. We show that directional detectors such as the future MIMAC detector will probe spin dependent dark matter scattering on nucleons that are beyond the reach of current spin independent detectors. The complementarity between indirect searches, in particular using gamma rays from dwarf spheroidal galaxies, spin dependent and spin independent direct search techniques is emphasized. We comment on the impact of the negative results on squark searches at the LHC. Finally, we investigate how the fundamental parameters of the models can be constrained in the event of a dark matter signal.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/30/probing-neutralino-dark-matter-in-the-mssm-the-nmssm-with-directional-detection-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Code-division multiplexing for x-ray microcalorimeters [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/01/30/code-division-multiplexing-for-x-ray-microcalorimeters-cross-listing/</link>
		<comments>http://voxcharta.org/2012/01/30/code-division-multiplexing-for-x-ray-microcalorimeters-cross-listing/#comments</comments>
		<pubDate>Tue, 31 Jan 2012 01:43:26 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[code division multiplexing]]></category>
		<category><![CDATA[demonstration]]></category>
		<category><![CDATA[energy resolution]]></category>
		<category><![CDATA[keV]]></category>
		<category><![CDATA[sqrt]]></category>
		<category><![CDATA[term approach]]></category>
		<category><![CDATA[time division]]></category>
		<category><![CDATA[transition]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/30/code-division-multiplexing-for-x-ray-microcalorimeters-cross-listing/</guid>
		<description><![CDATA[We demonstrate the code-division multiplexed (CDM) readout of eight transition-edge sensor microcalorimeters. The energy resolution is 3.0 eV (full width at half-maximum) or better at 5.9 keV, with a best resolution of 2.3 eV and a mean of 2.6 eV over the seven modulated detectors. The flux-summing CDM system is described and compared with similar [...]]]></description>
			<content:encoded><![CDATA[<p>We demonstrate the code-division multiplexed (CDM) readout of eight transition-edge sensor microcalorimeters. The energy resolution is 3.0 eV (full width at half-maximum) or better at 5.9 keV, with a best resolution of 2.3 eV and a mean of 2.6 eV over the seven modulated detectors. The flux-summing CDM system is described and compared with similar time-division multiplexed (TDM) readout. We show that the sqrt(Npixels) multiplexing disadvantage associated with TDM is not present in CDM. This demonstration establishes CDM as both a simple route to higher performance in existing TDM microcalorimetric experiments and a long-term approach to reaching higher multiplexing factors.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>How well do STARLAB and NBODY compare? II: Hardware and accuracy</title>
		<link>http://voxcharta.org/2012/01/29/how-well-do-starlab-and-nbody-compare-ii-hardware-and-accuracy/</link>
		<comments>http://voxcharta.org/2012/01/29/how-well-do-starlab-and-nbody-compare-ii-hardware-and-accuracy/#comments</comments>
		<pubDate>Mon, 30 Jan 2012 01:47:02 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration]]></category>
		<category><![CDATA[basic quantities]]></category>
		<category><![CDATA[binary evolution]]></category>
		<category><![CDATA[body simulation]]></category>
		<category><![CDATA[bootstrap algorithm]]></category>
		<category><![CDATA[cluster model]]></category>
		<category><![CDATA[computational demands]]></category>
		<category><![CDATA[dynamical evolution]]></category>
		<category><![CDATA[functional dependencies]]></category>
		<category><![CDATA[graphic card]]></category>
		<category><![CDATA[hardware accelerators]]></category>
		<category><![CDATA[mass function]]></category>
		<category><![CDATA[massive star cluster]]></category>
		<category><![CDATA[purpose hardware]]></category>
		<category><![CDATA[quantitative comparison]]></category>
		<category><![CDATA[simulation result]]></category>
		<category><![CDATA[simulation time]]></category>
		<category><![CDATA[star cluster]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[time step]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/29/how-well-do-starlab-and-nbody-compare-ii-hardware-and-accuracy/</guid>
		<description><![CDATA[Most recent progress in understanding the dynamical evolution of star clusters relies on direct N-body simulations. Owing to the computational demands, and the desire to model more complex and more massive star clusters, hardware calculational accelerators, such as GRAPE special-purpose hardware or, more recently, GPUs (i.e. graphics cards), are generally utilised. In addition, simulations can [...]]]></description>
			<content:encoded><![CDATA[<p>Most recent progress in understanding the dynamical evolution of star clusters relies on direct N-body simulations. Owing to the computational demands, and the desire to model more complex and more massive star clusters, hardware calculational accelerators, such as GRAPE special-purpose hardware or, more recently, GPUs (i.e. graphics cards), are generally utilised. In addition, simulations can be accelerated by adjusting parameters determining the calculation accuracy (i.e. changing the internal simulation time step used for each star).   We extend our previous thorough comparison (Anders et al. 2009) of basic quantities as derived from simulations performed either with STARLAB/KIRA or NBODY6. Here we focus on differences arising from using different hardware accelerations (including the increasingly popular graphic card accelerations/GPUs) and different calculation accuracy settings.   We use the large number of star cluster models (for a fixed stellar mass function, without stellar/binary evolution, primordial binaries, external tidal fields etc) already used in the previous paper, evolve them with STARLAB/KIRA (and NBODY6, where required), analyse them in a consistent way and compare the averaged results quantitatively. For this quantitative comparison, we apply the bootstrap algorithm for functional dependencies developed in our previous study.   In general we find very high comparability of the simulation results, independent of the used computer hardware (including the hardware accelerators) and the used N-body code. For the tested accuracy settings we find that for reduced accuracy (i.e. time step at least a factor 2.5 larger than the standard setting) most simulation results deviate significantly from the results using standard settings. The remaining deviations are comprehensible and explicable.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A Feasibility Study for the Detection of Supernova Explosions with an Undersea Neutrino Telescope</title>
		<link>http://voxcharta.org/2012/01/29/a-feasibility-study-for-the-detection-of-supernova-explosions-with-an-undersea-neutrino-telescope/</link>
		<comments>http://voxcharta.org/2012/01/29/a-feasibility-study-for-the-detection-of-supernova-explosions-with-an-undersea-neutrino-telescope/#comments</comments>
		<pubDate>Mon, 30 Jan 2012 01:44:29 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[coincidence]]></category>
		<category><![CDATA[electron antineutrino]]></category>
		<category><![CDATA[explosion results]]></category>
		<category><![CDATA[feasibility study]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[neutrino]]></category>
		<category><![CDATA[neutrino telescope]]></category>
		<category><![CDATA[optical module]]></category>
		<category><![CDATA[photomultiplier tube]]></category>
		<category><![CDATA[signature]]></category>
		<category><![CDATA[sn explosion]]></category>
		<category><![CDATA[supernova explosion]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/29/a-feasibility-study-for-the-detection-of-supernova-explosions-with-an-undersea-neutrino-telescope/</guid>
		<description><![CDATA[We study the potential of a very large volume underwater Mediterranean neutrino telescope to observe neutrinos from supernova (SN) explosions within our galaxy. The intense neutrino burst emitted in a SN explosion results in a large number of MeV neutrinos inside the instrumented volume of the neutrino telescope that can be detected (mainly) via the [...]]]></description>
			<content:encoded><![CDATA[<p>We study the potential of a very large volume underwater Mediterranean neutrino telescope to observe neutrinos from supernova (SN) explosions within our galaxy. The intense neutrino burst emitted in a SN explosion results in a large number of MeV neutrinos inside the instrumented volume of the neutrino telescope that can be detected (mainly) via the reaction \nu_e-bar + p -&gt; e^+ + n . In this study we simulated the response of the underwater neutrino telescope to the electron antineutrino flux predicted by the Garching model for SN explosions. We assumed that the neutrino telescope comprises 6160 direction sensitive optical modules, each containing 31 small photomultiplier tubes. Multiple coincidences between the photomultiplier tubes of the same optical module are utilized to suppress the noise produced by $^{40}K$ radioactive decays and to establish a statistical significant signature of the SN explosion.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/29/a-feasibility-study-for-the-detection-of-supernova-explosions-with-an-undersea-neutrino-telescope/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Adaptive Optics for Astronomy</title>
		<link>http://voxcharta.org/2012/01/29/adaptive-optics-for-astronomy/</link>
		<comments>http://voxcharta.org/2012/01/29/adaptive-optics-for-astronomy/#comments</comments>
		<pubDate>Mon, 30 Jan 2012 01:42:45 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[adaptive optics]]></category>
		<category><![CDATA[astrophysical processes]]></category>
		<category><![CDATA[diffraction limit]]></category>
		<category><![CDATA[instrumentation suite]]></category>
		<category><![CDATA[multitude]]></category>
		<category><![CDATA[next generation]]></category>
		<category><![CDATA[observational astronomy]]></category>
		<category><![CDATA[observatory]]></category>
		<category><![CDATA[perspective]]></category>
		<category><![CDATA[prime example]]></category>
		<category><![CDATA[satellite]]></category>
		<category><![CDATA[science application]]></category>
		<category><![CDATA[spatial resolution]]></category>
		<category><![CDATA[technological development]]></category>
		<category><![CDATA[telescopes]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/29/adaptive-optics-for-astronomy/</guid>
		<description><![CDATA[Adaptive Optics is a prime example of how progress in observational astronomy can be driven by technological developments. At many observatories it is now considered to be part of a standard instrumentation suite, enabling ground-based telescopes to reach the diffraction limit and thus providing spatial resolution superior to that achievable from space with current or [...]]]></description>
			<content:encoded><![CDATA[<p>Adaptive Optics is a prime example of how progress in observational astronomy can be driven by technological developments. At many observatories it is now considered to be part of a standard instrumentation suite, enabling ground-based telescopes to reach the diffraction limit and thus providing spatial resolution superior to that achievable from space with current or planned satellites. In this review we consider adaptive optics from the astrophysical perspective. We show that adaptive optics has led to important advances in our understanding of a multitude of astrophysical processes, and describe how the requirements from science applications are now driving the development of the next generation of novel adaptive optics techniques.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>New ground-based observational methods and instrumentation for asteroseismology</title>
		<link>http://voxcharta.org/2012/01/29/new-ground-based-observational-methods-and-instrumentation-for-asteroseismology/</link>
		<comments>http://voxcharta.org/2012/01/29/new-ground-based-observational-methods-and-instrumentation-for-asteroseismology/#comments</comments>
		<pubDate>Mon, 30 Jan 2012 01:37:42 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[aim]]></category>
		<category><![CDATA[corot]]></category>
		<category><![CDATA[kepler]]></category>
		<category><![CDATA[methodology]]></category>
		<category><![CDATA[mode identification]]></category>
		<category><![CDATA[new ground]]></category>
		<category><![CDATA[observational methods]]></category>
		<category><![CDATA[precision data]]></category>
		<category><![CDATA[soho]]></category>
		<category><![CDATA[space instrumentation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/29/new-ground-based-observational-methods-and-instrumentation-for-asteroseismology/</guid>
		<description><![CDATA[Space instrumentation like SOHO, MOST, CoRoT and Kepler has been and is being built to attain very high precision data to be used for asteroseismic analysis. Nonetheless, there is a very strong need for providing additional information, especially on mode identification. With this contribution I will review the efforts been put on new ground-based instrumentation [...]]]></description>
			<content:encoded><![CDATA[<p>Space instrumentation like SOHO, MOST, CoRoT and Kepler has been and is being built to attain very high precision data to be used for asteroseismic analysis. Nonetheless, there is a very strong need for providing additional information, especially on mode identification. With this contribution I will review the efforts been put on new ground-based instrumentation and the methodology that can be used to achieve this aim.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>GalMass: A Smartphone Application for Estimating Galaxy Masses [Replacement]</title>
		<link>http://voxcharta.org/2012/01/29/galmass-a-smartphone-application-for-estimating-galaxy-masses-replacement/</link>
		<comments>http://voxcharta.org/2012/01/29/galmass-a-smartphone-application-for-estimating-galaxy-masses-replacement/#comments</comments>
		<pubDate>Mon, 30 Jan 2012 01:34:55 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[central galaxy]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[galaxy masses]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[mgas]]></category>
		<category><![CDATA[mstar]]></category>
		<category><![CDATA[note documents]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[stellar mass]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/29/galmass-a-smartphone-application-for-estimating-galaxy-masses-replacement/</guid>
		<description><![CDATA[This note documents the methods used by the smartphone application, &#8220;GalMass,&#8221; which has been released on the Android Market. GalMass estimates the halo virial mass (Mvir), stellar mass (Mstar), gas mass (Mgas), and galaxy gas fraction of a central galaxy as a function of redshift (z&#60;2), with any one of the above masses as an [...]]]></description>
			<content:encoded><![CDATA[<p>This note documents the methods used by the smartphone application, &#8220;GalMass,&#8221; which has been released on the Android Market. GalMass estimates the halo virial mass (Mvir), stellar mass (Mstar), gas mass (Mgas), and galaxy gas fraction of a central galaxy as a function of redshift (z&lt;2), with any one of the above masses as an input parameter. In order to convert between Mvir and Mstar (in either direction), GalMass uses fitting functions that approximate the abundance matching models of either Conroy &amp; Wechsler (2009), Moster et al. (2010), or Behroozi et al. (2010). GalMass uses a a semi-empirical fit to observed galaxy gas fractions to convert between Mstar and Mgas, as outlined in Stewart et al. (2009).</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Re-calibrated Generalized-Scidar measurements at Cerro Paranal (VLT&#8217;s site) [Replacement]</title>
		<link>http://voxcharta.org/2012/01/29/re-calibrated-generalized-scidar-measurements-at-cerro-paranal-vlts-site-replacement/</link>
		<comments>http://voxcharta.org/2012/01/29/re-calibrated-generalized-scidar-measurements-at-cerro-paranal-vlts-site-replacement/#comments</comments>
		<pubDate>Mon, 30 Jan 2012 01:34:33 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absolute error]]></category>
		<category><![CDATA[absolute terms]]></category>
		<category><![CDATA[autocorrelation]]></category>
		<category><![CDATA[cerro paranal]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[correspondent]]></category>
		<category><![CDATA[elt]]></category>
		<category><![CDATA[free atmosphere]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[median value]]></category>
		<category><![CDATA[normalization]]></category>
		<category><![CDATA[paranal observatory]]></category>
		<category><![CDATA[relative error]]></category>
		<category><![CDATA[slab]]></category>
		<category><![CDATA[statistic analysis]]></category>
		<category><![CDATA[Turbulence]]></category>
		<category><![CDATA[vlt]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/29/re-calibrated-generalized-scidar-measurements-at-cerro-paranal-vlts-site-replacement/</guid>
		<description><![CDATA[Generalized Scidar (GS) measurements taken at the Paranal Observatory in November/December 2007 in the context of a site qualification for the future European Extremely Large Telescope E-ELT are re-calibrated to overcome the bias induced on the CN2 profiles by a not correct normalization of the autocorrelation of the scintillation maps that has been recently identified [...]]]></description>
			<content:encoded><![CDATA[<p>Generalized Scidar (GS) measurements taken at the Paranal Observatory in November/December 2007 in the context of a site qualification for the future European Extremely Large Telescope E-ELT are re-calibrated to overcome the bias induced on the CN2 profiles by a not correct normalization of the autocorrelation of the scintillation maps that has been recently identified in the GS technique. A complete analysis of the GS corrected measurements as well as of the corrected errors is performed statistically as well as on individual nights and for each time during all nights. The relative errors of the CN2 profiles can reach up to 60% in some narrow temporal windows and some vertical slabs, the total seeing up to 12% and the total integrated turbulence J up to 21%. However, the statistic analysis tells us that the absolute errors of the median values of the total seeing is 0.06 arcsec (relative error 5.6%), for the boundary seeing 0.05 arcsec (relative error 5.6%) and for the seeing in the free atmosphere 0.04 arcsec (relative error 9%). We find that, in spite of the fact that the relative error increases with the height, the boundary and the free atmosphere seeing contribute in an equivalent way to the error on the total seeing in absolute terms. Besides, we find that there are no correlations between the relative errors and the value of the correspondent seeing. The absolute error of the median value of the isoplanatic angle is 0.13 arcsec (relative error 6.9%).</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
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		<item>
		<title>Kinetic inductance detectors for millimeter and submillimeter astronomy / D\&#8217;etecteurs \`a inductance cin\&#8217;etique pour l&#8217;astronomie millim\&#8217;etrique et sub-millim\&#8217;etrique [Replacement]</title>
		<link>http://voxcharta.org/2012/01/29/kinetic-inductance-detectors-for-millimeter-and-submillimeter-astronomy-detecteurs-a-inductance-cinetique-pour-lastronomie-millimetrique-et-sub-millimetrique-replacement/</link>
		<comments>http://voxcharta.org/2012/01/29/kinetic-inductance-detectors-for-millimeter-and-submillimeter-astronomy-detecteurs-a-inductance-cinetique-pour-lastronomie-millimetrique-et-sub-millimetrique-replacement/#comments</comments>
		<pubDate>Mon, 30 Jan 2012 01:31:35 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[array]]></category>
		<category><![CDATA[astronomical sources]]></category>
		<category><![CDATA[astronomie]]></category>
		<category><![CDATA[case study]]></category>
		<category><![CDATA[dual band]]></category>
		<category><![CDATA[eel]]></category>
		<category><![CDATA[ees]]></category>
		<category><![CDATA[etique]]></category>
		<category><![CDATA[field experiment]]></category>
		<category><![CDATA[imaging system]]></category>
		<category><![CDATA[meter telescope]]></category>
		<category><![CDATA[millimeter wave]]></category>
		<category><![CDATA[nika]]></category>
		<category><![CDATA[pico veleta]]></category>
		<category><![CDATA[readout electronics]]></category>
		<category><![CDATA[recent developments]]></category>
		<category><![CDATA[submillimeter astronomy]]></category>
		<category><![CDATA[subset]]></category>
		<category><![CDATA[tirer parti]]></category>
		<category><![CDATA[working principle]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/29/kinetic-inductance-detectors-for-millimeter-and-submillimeter-astronomy-detecteurs-a-inductance-cinetique-pour-lastronomie-millimetrique-et-sub-millimetrique-replacement/</guid>
		<description><![CDATA[We present recent developments in Kinetic Inductance Detectors (KID) for large arrays of detectors. The main application is ground-based millimeter wave astronomy. We focus in particular, as a case study, on our own experiment: NIKA (N\&#8217;eel IRAM KID Arrays). NIKA is today the best in-the-field experiment using KID-based instruments, and consists of a dual-band imaging [...]]]></description>
			<content:encoded><![CDATA[<p>We present recent developments in Kinetic Inductance Detectors (KID) for large arrays of detectors. The main application is ground-based millimeter wave astronomy. We focus in particular, as a case study, on our own experiment: NIKA (N\&#8217;eel IRAM KID Arrays). NIKA is today the best in-the-field experiment using KID-based instruments, and consists of a dual-band imaging system designed for the IRAM 30 meter telescope at Pico Veleta. We describe in this article, after a general context introduction, the KID working principle and the readout electronics, crucial to take advantage of the intrinsic KID multiplexability. We conclude with a small subset of the astronomical sources observed simultaneously at 2 mm and 1.4 mm by NIKA during the last run, held in October 2010.   Nous d\&#8217;ecrivons les r\&#8217;ecents d\&#8217;eveloppements concernant les grandes matrices de d\&#8217;etecteurs \`a inductance cin\&#8217;etique (KID) dont l&#8217;application principale est l&#8217;astronomie millim\&#8217;etrique au sol. Nous d\&#8217;etaillons en particulier notre propre cam\&#8217;era : NIKA (N\&#8217;eel IRAM KID Arrays) qui est aujourd&#8217;hui l&#8217;instrument le plus abouti mettant en oeuvre des KIDs. NIKA est une cam\&#8217;era bi-bande con\c{c}ue pour le radiot\&#8217;elescope de 30 m\`etres de l&#8217;IRAM \`a Pico Veleta. Apr\&#8217;es avoir d\&#8217;ecrit le contexte instrumental dans lequel ils s&#8217;inscrivent, nous expliquerons le principe de fonctionnement des KIDs et de leur \&#8217;electronique de lecture, cruciale pour pouvoir tirer parti de leur potentiel de muliplexage. Pour finir, nous pr\&#8217;esentons quelques exemples d&#8217;observations effectu\&#8217;ees par NIKA dans les bandes de 2 mm et 1,4 mm au cours de la derni\`ere campagne d&#8217;observation en octobre 2010.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/29/kinetic-inductance-detectors-for-millimeter-and-submillimeter-astronomy-detecteurs-a-inductance-cinetique-pour-lastronomie-millimetrique-et-sub-millimetrique-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Accelerating incoherent dedispersion</title>
		<link>http://voxcharta.org/2012/01/26/accelerating-incoherent-dedispersion/</link>
		<comments>http://voxcharta.org/2012/01/26/accelerating-incoherent-dedispersion/#comments</comments>
		<pubDate>Fri, 27 Jan 2012 01:59:06 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[c library]]></category>
		<category><![CDATA[computational speed]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[development time]]></category>
		<category><![CDATA[execution time]]></category>
		<category><![CDATA[goal in mind]]></category>
		<category><![CDATA[implementation]]></category>
		<category><![CDATA[insight gained from]]></category>
		<category><![CDATA[memory consumption]]></category>
		<category><![CDATA[modern graphics]]></category>
		<category><![CDATA[optimisation]]></category>
		<category><![CDATA[pipeline]]></category>
		<category><![CDATA[processing unit]]></category>
		<category><![CDATA[science results]]></category>
		<category><![CDATA[speed ups]]></category>
		<category><![CDATA[time trade]]></category>
		<category><![CDATA[trade offs]]></category>
		<category><![CDATA[ups]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/26/accelerating-incoherent-dedispersion/</guid>
		<description><![CDATA[Incoherent dedispersion is a computationally intensive problem that appears frequently in pulsar and transient astronomy. For current and future transient pipelines, dedispersion can dominate the total execution time, meaning its computational speed acts as a constraint on the quality and quantity of science results. It is thus critical that the algorithm be able to take [...]]]></description>
			<content:encoded><![CDATA[<p>Incoherent dedispersion is a computationally intensive problem that appears frequently in pulsar and transient astronomy. For current and future transient pipelines, dedispersion can dominate the total execution time, meaning its computational speed acts as a constraint on the quality and quantity of science results. It is thus critical that the algorithm be able to take advantage of trends in commodity computing hardware. With this goal in mind, we present analysis of the &#8216;direct&#8217;, &#8216;tree&#8217; and &#8217;sub-band&#8217; dedispersion algorithms with respect to their potential for efficient execution on modern graphics processing units (GPUs). We find all three to be excellent candidates, and proceed to describe implementations in C for CUDA using insight gained from the analysis. Using recent CPU and GPU hardware, the transition to the GPU provides a speed-up of 9x for the direct algorithm when compared to an optimised quad-core CPU code. For realistic recent survey parameters, these speeds are high enough that further optimisation is unnecessary to achieve real-time processing. Where further speed-ups are desirable, we find that the tree and sub-band algorithms are able to provide 3-7x better performance at the cost of certain smearing, memory consumption and development time trade-offs. We finish with a discussion of the implications of these results for future transient surveys. Our GPU dedispersion code is publicly available as a C library at: <a href="http://dedisp.googlecode.com/">http://dedisp.googlecode.com/</a></p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/26/accelerating-incoherent-dedispersion/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Allen Telescope Array Commensal Observing System</title>
		<link>http://voxcharta.org/2012/01/26/the-allen-telescope-array-commensal-observing-system/</link>
		<comments>http://voxcharta.org/2012/01/26/the-allen-telescope-array-commensal-observing-system/#comments</comments>
		<pubDate>Fri, 27 Jan 2012 01:53:12 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[allen telescope array]]></category>
		<category><![CDATA[codebase]]></category>
		<category><![CDATA[correlator]]></category>
		<category><![CDATA[design decisions]]></category>
		<category><![CDATA[existing system]]></category>
		<category><![CDATA[hibernation]]></category>
		<category><![CDATA[implementation]]></category>
		<category><![CDATA[infrastructure plan]]></category>
		<category><![CDATA[insiders]]></category>
		<category><![CDATA[modes]]></category>
		<category><![CDATA[observatory staff]]></category>
		<category><![CDATA[observing system]]></category>
		<category><![CDATA[rationale]]></category>
		<category><![CDATA[share infrastructure]]></category>
		<category><![CDATA[software infrastructure]]></category>
		<category><![CDATA[tension]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/26/the-allen-telescope-array-commensal-observing-system/</guid>
		<description><![CDATA[This memo describes the system used to conduct commensal correlator and beamformer observations at the Allen Telescope Array (ATA). This system was deployed for ~2 years until the ATA hibernation in 2011 and was responsible for collecting &#62;5 TB of data during thousands of hours of observations. The general system design is presented and the [...]]]></description>
			<content:encoded><![CDATA[<p>This memo describes the system used to conduct commensal correlator and beamformer observations at the Allen Telescope Array (ATA). This system was deployed for ~2 years until the ATA hibernation in 2011 and was responsible for collecting &gt;5 TB of data during thousands of hours of observations. The general system design is presented and the implementation is discussed in detail. I emphasize the rationale for various design decisions and attempt to document a few aspects of ATA operations that might not be obvious to non-insiders. I close with some recommendations from my experience developing the software infrastructure and managing the correlator observations. These include: reuse existing systems; solve, don&#8217;t avoid, tensions between projects, and share infrastructure; plan to make standalone observations to complement the commensal ones; and be considerate of observatory staff when deploying new and unusual observing modes. The structure of the software codebase is documented.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/26/the-allen-telescope-array-commensal-observing-system/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The relative significance of the H-index</title>
		<link>http://voxcharta.org/2012/01/26/the-relative-significance-of-the-h-index/</link>
		<comments>http://voxcharta.org/2012/01/26/the-relative-significance-of-the-h-index/#comments</comments>
		<pubDate>Fri, 27 Jan 2012 01:49:46 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astrophysics]]></category>
		<category><![CDATA[citation]]></category>
		<category><![CDATA[gross measure]]></category>
		<category><![CDATA[hirsch]]></category>
		<category><![CDATA[literature]]></category>
		<category><![CDATA[relative significance]]></category>
		<category><![CDATA[theoretical reasoning]]></category>
		<category><![CDATA[visibility]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/26/the-relative-significance-of-the-h-index/</guid>
		<description><![CDATA[Use of the Hirsch-index ($H$) as measure of an author&#8217;s visibility in the scientific literature has become popular as an alternative to a gross measure like total citations (c). I show that, at least in astrophysics, $H$ correlates tightly with overall citations. The mean relation is $H=0.5(\sqrt c+1)$. Outliers are few and not too far [...]]]></description>
			<content:encoded><![CDATA[<p>Use of the Hirsch-index ($H$) as measure of an author&#8217;s visibility in the scientific literature has become popular as an alternative to a gross measure like total citations (c). I show that, at least in astrophysics, $H$ correlates tightly with overall citations. The mean relation is $H=0.5(\sqrt c+1)$. Outliers are few and not too far from the mean, especially if `normalized&#8217; ADS citations are used for $c$ and $H$. Whatever the theoretical reasoning behind it, the Hirsch index in practice does not appear to measure something significantly new.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/26/the-relative-significance-of-the-h-index/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Kinetic inductance detectors for millimeter and submillimeter astronomy / D\&#8217;etecteurs \`a inductance cin\&#8217;etique pour l&#8217;astronomie millim\&#8217;etrique et sub-millim\&#8217;etrique</title>
		<link>http://voxcharta.org/2012/01/26/kinetic-inductance-detectors-for-millimeter-and-submillimeter-astronomy-detecteurs-a-inductance-cinetique-pour-lastronomie-millimetrique-et-sub-millimetrique/</link>
		<comments>http://voxcharta.org/2012/01/26/kinetic-inductance-detectors-for-millimeter-and-submillimeter-astronomy-detecteurs-a-inductance-cinetique-pour-lastronomie-millimetrique-et-sub-millimetrique/#comments</comments>
		<pubDate>Fri, 27 Jan 2012 01:48:44 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[array]]></category>
		<category><![CDATA[astronomical sources]]></category>
		<category><![CDATA[astronomie]]></category>
		<category><![CDATA[case study]]></category>
		<category><![CDATA[dual band]]></category>
		<category><![CDATA[eel]]></category>
		<category><![CDATA[ees]]></category>
		<category><![CDATA[etique]]></category>
		<category><![CDATA[field experiment]]></category>
		<category><![CDATA[imaging system]]></category>
		<category><![CDATA[meter telescope]]></category>
		<category><![CDATA[millimeter wave]]></category>
		<category><![CDATA[nika]]></category>
		<category><![CDATA[pico veleta]]></category>
		<category><![CDATA[readout electronics]]></category>
		<category><![CDATA[recent developments]]></category>
		<category><![CDATA[submillimeter astronomy]]></category>
		<category><![CDATA[subset]]></category>
		<category><![CDATA[tirer parti]]></category>
		<category><![CDATA[working principle]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/26/kinetic-inductance-detectors-for-millimeter-and-submillimeter-astronomy-detecteurs-a-inductance-cinetique-pour-lastronomie-millimetrique-et-sub-millimetrique/</guid>
		<description><![CDATA[We present recent developments in Kinetic Inductance Detectors (KID) for large arrays of detectors. The main application is ground-based millimeter wave astronomy. We focus in particular, as a case study, on our own experiment: NIKA (N\&#8217;eel IRAM KID Arrays). NIKA is today the best in-the-field experiment using KID-based instruments, and consists of a dual-band imaging [...]]]></description>
			<content:encoded><![CDATA[<p>We present recent developments in Kinetic Inductance Detectors (KID) for large arrays of detectors. The main application is ground-based millimeter wave astronomy. We focus in particular, as a case study, on our own experiment: NIKA (N\&#8217;eel IRAM KID Arrays). NIKA is today the best in-the-field experiment using KID-based instruments, and consists of a dual-band imaging system designed for the IRAM 30 meter telescope at Pico Veleta. We describe in this article, after a general context introduction, the KID working principle and the readout electronics, crucial to take advantage of the intrinsic KID multiplexability. We conclude with a small subset of the astronomical sources observed simultaneously at 2 mm and 1.4 mm by NIKA during the last run, held in October 2010.   Nous d\&#8217;ecrivons les r\&#8217;ecents d\&#8217;eveloppements concernant les grandes matrices de d\&#8217;etecteurs \`a inductance cin\&#8217;etique (KID) dont l&#8217;application principale est l&#8217;astronomie millim\&#8217;etrique au sol. Nous d\&#8217;etaillons en particulier notre propre cam\&#8217;era : NIKA (N\&#8217;eel IRAM KID Arrays) qui est aujourd&#8217;hui l&#8217;instrument le plus abouti mettant en oeuvre des KIDs. NIKA est une cam\&#8217;era bi-bande con\c{c}ue pour le radiot\&#8217;elescope de 30 m\`etres de l&#8217;IRAM \`a Pico Veleta. Apr\&#8217;es avoir d\&#8217;ecrit le contexte instrumental dans lequel ils s&#8217;inscrivent, nous expliquerons le principe de fonctionnement des KIDs et de leur \&#8217;electronique de lecture, cruciale pour pouvoir tirer parti de leur potentiel de muliplexage. Pour finir, nous pr\&#8217;esentons quelques exemples d&#8217;observations effectu\&#8217;ees par NIKA dans les bandes de 2 mm et 1,4 mm au cours de la derni\`ere campagne d&#8217;observation en octobre 2010.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/26/kinetic-inductance-detectors-for-millimeter-and-submillimeter-astronomy-detecteurs-a-inductance-cinetique-pour-lastronomie-millimetrique-et-sub-millimetrique/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Post-correlation filtering techniques for off-axis source and RFI removal</title>
		<link>http://voxcharta.org/2012/01/26/post-correlation-filtering-techniques-for-off-axis-source-and-rfi-removal/</link>
		<comments>http://voxcharta.org/2012/01/26/post-correlation-filtering-techniques-for-off-axis-source-and-rfi-removal/#comments</comments>
		<pubDate>Fri, 27 Jan 2012 01:43:02 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[axis]]></category>
		<category><![CDATA[baseline]]></category>
		<category><![CDATA[baseline data]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[data integration]]></category>
		<category><![CDATA[data quality]]></category>
		<category><![CDATA[element]]></category>
		<category><![CDATA[frequency direction]]></category>
		<category><![CDATA[ghost]]></category>
		<category><![CDATA[gridding]]></category>
		<category><![CDATA[initial test]]></category>
		<category><![CDATA[low pass filter]]></category>
		<category><![CDATA[novel]]></category>
		<category><![CDATA[peeling]]></category>
		<category><![CDATA[radio frequency interference]]></category>
		<category><![CDATA[radio observation]]></category>
		<category><![CDATA[rfi]]></category>
		<category><![CDATA[separation technique]]></category>
		<category><![CDATA[several factors]]></category>
		<category><![CDATA[source separation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/26/post-correlation-filtering-techniques-for-off-axis-source-and-rfi-removal/</guid>
		<description><![CDATA[Techniques to improve the data quality of interferometric radio observations are considered. Fundaments of fringe frequencies in the uv-plane are discussed and filters are used to attenuate radio-frequency interference (RFI) and off-axis sources. Several new applications of filters are introduced and tested. A low-pass filter in time and frequency direction on single baseline data is [...]]]></description>
			<content:encoded><![CDATA[<p>Techniques to improve the data quality of interferometric radio observations are considered. Fundaments of fringe frequencies in the uv-plane are discussed and filters are used to attenuate radio-frequency interference (RFI) and off-axis sources. Several new applications of filters are introduced and tested. A low-pass filter in time and frequency direction on single baseline data is successfully used to lower the noise in the area of interest and to remove sidelobes coming from unmodelled off-axis sources and RFI. Related side effects of data integration, averaging and gridding are analysed, and shown to be able to cause ghosts and an increase in noise, especially when using long baselines or interferometric elements that have a large field of view. A novel projected fringe low-pass filter is shown to be potentially useful for first order source separation. Initial tests show that the filters can be several factors faster compared to common source separation techniques such as peeling and a variant of peeling that is currently being tested on LOFAR observations called &#8220;demixed peeling&#8221;. Further testing is required to support the performance of the filters.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/26/post-correlation-filtering-techniques-for-off-axis-source-and-rfi-removal/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Evaluation of the discovery potential of an underwater Mediterranean neutrino telescope taking into account the estimated directional resolution and energy of the reconstructed tracks</title>
		<link>http://voxcharta.org/2012/01/26/evaluation-of-the-discovery-potential-of-an-underwater-mediterranean-neutrino-telescope-taking-into-account-the-estimated-directional-resolution-and-energy-of-the-reconstructed-tracks/</link>
		<comments>http://voxcharta.org/2012/01/26/evaluation-of-the-discovery-potential-of-an-underwater-mediterranean-neutrino-telescope-taking-into-account-the-estimated-directional-resolution-and-energy-of-the-reconstructed-tracks/#comments</comments>
		<pubDate>Fri, 27 Jan 2012 01:41:40 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[capability]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[estimation]]></category>
		<category><![CDATA[neutrino telescope]]></category>
		<category><![CDATA[search method]]></category>
		<category><![CDATA[significant improvement]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/26/evaluation-of-the-discovery-potential-of-an-underwater-mediterranean-neutrino-telescope-taking-into-account-the-estimated-directional-resolution-and-energy-of-the-reconstructed-tracks/</guid>
		<description><![CDATA[We report on the development of search methods for point like and extended neutrino sources, utilizing the tracking and energy estimation capabilities of an underwater, Very Large Volume Neutrino Telescope (VLVnT). We demonstrate that the developed techniques offer a significant improvement on the telescope&#8217;s discovery potential. We also present results on the potential of the [...]]]></description>
			<content:encoded><![CDATA[<p>We report on the development of search methods for point like and extended neutrino sources, utilizing the tracking and energy estimation capabilities of an underwater, Very Large Volume Neutrino Telescope (VLVnT). We demonstrate that the developed techniques offer a significant improvement on the telescope&#8217;s discovery potential. We also present results on the potential of the Mediterranean KM3NeT to discover galactic, neutrino sources.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/26/evaluation-of-the-discovery-potential-of-an-underwater-mediterranean-neutrino-telescope-taking-into-account-the-estimated-directional-resolution-and-energy-of-the-reconstructed-tracks/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Analytical time-like geodesics [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/01/26/analytical-time-like-geodesics-cross-listing/</link>
		<comments>http://voxcharta.org/2012/01/26/analytical-time-like-geodesics-cross-listing/#comments</comments>
		<pubDate>Fri, 27 Jan 2012 01:40:45 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[analytical solution]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[elliptic functions and elliptic integrals]]></category>
		<category><![CDATA[Lambda]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[proper time]]></category>
		<category><![CDATA[space time]]></category>
		<category><![CDATA[tau]]></category>
		<category><![CDATA[temporal evolution]]></category>
		<category><![CDATA[transient phenomena]]></category>
		<category><![CDATA[true anomaly]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/26/analytical-time-like-geodesics-cross-listing/</guid>
		<description><![CDATA[Time-like orbits in Schwarzschild space-time are presented and classified in a very transparent and straightforward way into four types. The analytical solutions to orbit, time, and proper time equations are given for all orbit types in the form r=r(\lambda), t=t(\chi), and \tau=\tau(\chi), where \lambda\ is the true anomaly and \chi\ is a parameter along the [...]]]></description>
			<content:encoded><![CDATA[<p>Time-like orbits in Schwarzschild space-time are presented and classified in a very transparent and straightforward way into four types. The analytical solutions to orbit, time, and proper time equations are given for all orbit types in the form r=r(\lambda), t=t(\chi), and \tau=\tau(\chi), where \lambda\ is the true anomaly and \chi\ is a parameter along the orbit. A very simple relation between \lambda\ and \chi\ is also shown. These solutions are very useful for modeling temporal evolution of transient phenomena near black holes since they are expressed with Jacobi elliptic functions and elliptic integrals, which can be calculated very efficiently and accurately.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/26/analytical-time-like-geodesics-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Demonstration of On-Sky Calibration of Astronomical Spectra using a 25 GHz near-IR Laser Frequency Comb [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/01/25/demonstration-of-on-sky-calibration-of-astronomical-spectra-using-a-25-ghz-near-ir-laser-frequency-comb-cross-listing/</link>
		<comments>http://voxcharta.org/2012/01/25/demonstration-of-on-sky-calibration-of-astronomical-spectra-using-a-25-ghz-near-ir-laser-frequency-comb-cross-listing/#comments</comments>
		<pubDate>Thu, 26 Jan 2012 01:48:00 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[array]]></category>
		<category><![CDATA[astronomical spectra]]></category>
		<category><![CDATA[atomic clock]]></category>
		<category><![CDATA[calibration source]]></category>
		<category><![CDATA[cavity]]></category>
		<category><![CDATA[comb]]></category>
		<category><![CDATA[demonstration]]></category>
		<category><![CDATA[echelle orders]]></category>
		<category><![CDATA[global positioning system]]></category>
		<category><![CDATA[hobby eberly telescope]]></category>
		<category><![CDATA[laser frequency]]></category>
		<category><![CDATA[mcdonald observatory]]></category>
		<category><![CDATA[optical frequency]]></category>
		<category><![CDATA[radial velocity]]></category>
		<category><![CDATA[sky]]></category>
		<category><![CDATA[target]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/25/demonstration-of-on-sky-calibration-of-astronomical-spectra-using-a-25-ghz-near-ir-laser-frequency-comb-cross-listing/</guid>
		<description><![CDATA[We describe and characterize a 25 GHz laser frequency comb based on a cavity-filtered erbium fiber mode-locked laser. The comb provides a uniform array of optical frequencies spanning 1450 nm to 1700 nm, and is stabilized by use of a global positioning system referenced atomic clock. This comb was deployed at the 9.2 m Hobby-Eberly [...]]]></description>
			<content:encoded><![CDATA[<p>We describe and characterize a 25 GHz laser frequency comb based on a cavity-filtered erbium fiber mode-locked laser. The comb provides a uniform array of optical frequencies spanning 1450 nm to 1700 nm, and is stabilized by use of a global positioning system referenced atomic clock. This comb was deployed at the 9.2 m Hobby-Eberly telescope at the McDonald Observatory where it was used as a radial velocity calibration source for the fiber-fed Pathfinder near-infrared spectrograph. Stellar targets were observed in three echelle orders over four nights, and radial velocity precision of ~10 m/s (~6 MHz) was achieved from the comb-calibrated spectra.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/25/demonstration-of-on-sky-calibration-of-astronomical-spectra-using-a-25-ghz-near-ir-laser-frequency-comb-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The impact of Gaia and LSST on binary stars and exo-planets</title>
		<link>http://voxcharta.org/2012/01/25/the-impact-of-gaia-and-lsst-on-binary-stars-and-exo-planets/</link>
		<comments>http://voxcharta.org/2012/01/25/the-impact-of-gaia-and-lsst-on-binary-stars-and-exo-planets/#comments</comments>
		<pubDate>Thu, 26 Jan 2012 01:47:04 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astrometry]]></category>
		<category><![CDATA[astronomy]]></category>
		<category><![CDATA[binaries]]></category>
		<category><![CDATA[binary star]]></category>
		<category><![CDATA[binary system]]></category>
		<category><![CDATA[exo planets]]></category>
		<category><![CDATA[exoplanet]]></category>
		<category><![CDATA[gaia]]></category>
		<category><![CDATA[large scale]]></category>
		<category><![CDATA[lsst]]></category>
		<category><![CDATA[missions]]></category>
		<category><![CDATA[new era]]></category>
		<category><![CDATA[radial velocity]]></category>
		<category><![CDATA[tens]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/25/the-impact-of-gaia-and-lsst-on-binary-stars-and-exo-planets/</guid>
		<description><![CDATA[Two upcoming large scale surveys, the ESA Gaia and LSST projects, will bring a new era in astronomy. The number of binary systems that will be observed and detected by these projects is enormous, estimations range from millions for Gaia to several tens of millions for LSST. We review some tools that should be developed [...]]]></description>
			<content:encoded><![CDATA[<p>Two upcoming large scale surveys, the ESA Gaia and LSST projects, will bring a new era in astronomy. The number of binary systems that will be observed and detected by these projects is enormous, estimations range from millions for Gaia to several tens of millions for LSST. We review some tools that should be developed and also what can be gained from these missions on the subject of binaries and exoplanets from the astrometry, photometry, radial velocity and their alert systems.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/25/the-impact-of-gaia-and-lsst-on-binary-stars-and-exo-planets/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>High Resolution Rapid Response observations of compact radio sources with the Ceduna Hobart Interferometer (CHI)</title>
		<link>http://voxcharta.org/2012/01/25/high-resolution-rapid-response-observations-of-compact-radio-sources-with-the-ceduna-hobart-interferometer-chi/</link>
		<comments>http://voxcharta.org/2012/01/25/high-resolution-rapid-response-observations-of-compact-radio-sources-with-the-ceduna-hobart-interferometer-chi/#comments</comments>
		<pubDate>Thu, 26 Jan 2012 01:45:54 +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[active galactic nuclei]]></category>
		<category><![CDATA[astrophysical phenomena]]></category>
		<category><![CDATA[baseline interferometer]]></category>
		<category><![CDATA[brightness temperature]]></category>
		<category><![CDATA[calibration technique]]></category>
		<category><![CDATA[ceduna south australia]]></category>
		<category><![CDATA[compact radio source]]></category>
		<category><![CDATA[electromagnetic spectrum]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[hobart tasmania]]></category>
		<category><![CDATA[observational procedures]]></category>
		<category><![CDATA[radio coverage]]></category>
		<category><![CDATA[radio interferometer]]></category>
		<category><![CDATA[radio observation]]></category>
		<category><![CDATA[radio telescope]]></category>
		<category><![CDATA[ray space]]></category>
		<category><![CDATA[simultaneous observations]]></category>
		<category><![CDATA[software correlator]]></category>
		<category><![CDATA[space telescope]]></category>
		<category><![CDATA[university of tasmania]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/25/high-resolution-rapid-response-observations-of-compact-radio-sources-with-the-ceduna-hobart-interferometer-chi/</guid>
		<description><![CDATA[Context. Frequent, simultaneous observations across the electromagnetic spectrum are essential to the study of a range of astrophysical phenomena including Active Galactic Nuclei. A key tool of such studies is the ability to observe an object when it flares i.e. exhibits a rapid and significant increase in its flux density.   Aims. We describe [...]]]></description>
			<content:encoded><![CDATA[<p>Context. Frequent, simultaneous observations across the electromagnetic spectrum are essential to the study of a range of astrophysical phenomena including Active Galactic Nuclei. A key tool of such studies is the ability to observe an object when it flares i.e. exhibits a rapid and significant increase in its flux density.   Aims. We describe the specific observational procedures and the calibration techniques that have been developed and tested to create a single baseline radio interferometer that can rapidly observe a flaring object. This is the only facility that is dedicated to rapid high resolution radio observations of an object south of -30 degrees declination. An immediate application is to provide rapid contemporaneous radio coverage of AGN flaring at {\gamma}-ray frequencies detected by the Fermi Gamma-ray Space Telescope.   Methods. A single baseline interferometer was formed with radio telescopes in Hobart, Tasmania and Ceduna, South Australia. A software correlator was set up at the University of Tasmania to correlate these data.   Results. Measurements of the flux densities of flaring objects can be made using our observing strategy within half an hour of a triggering event. These observations can be calibrated with amplitude errors better than 15%. Lower limits to the brightness temperatures of the sources can also be calculated using CHI.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/25/high-resolution-rapid-response-observations-of-compact-radio-sources-with-the-ceduna-hobart-interferometer-chi/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Magnetically-levitating disks around supermassive black holes [Replacement]</title>
		<link>http://voxcharta.org/2012/01/25/magnetically-levitating-disks-around-supermassive-black-holes-replacement/</link>
		<comments>http://voxcharta.org/2012/01/25/magnetically-levitating-disks-around-supermassive-black-holes-replacement/#comments</comments>
		<pubDate>Thu, 26 Jan 2012 01:31:34 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion disk]]></category>
		<category><![CDATA[disk fragmentation]]></category>
		<category><![CDATA[duration]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gravitational force]]></category>
		<category><![CDATA[interstellar gas clouds]]></category>
		<category><![CDATA[lifetime]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetic pressure]]></category>
		<category><![CDATA[molecular cloud]]></category>
		<category><![CDATA[numerical experiment]]></category>
		<category><![CDATA[possible solution]]></category>
		<category><![CDATA[puzzle]]></category>
		<category><![CDATA[scale geometry]]></category>
		<category><![CDATA[supermassive black hole]]></category>
		<category><![CDATA[tidal disruption]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/25/magnetically-levitating-disks-around-supermassive-black-holes-replacement/</guid>
		<description><![CDATA[In this paper we report on the formation of magnetically-levitating accretion disks around supermassive black holes. The structure of these disks is calculated by numerically modelling tidal disruption of magnetized interstellar gas clouds. We find that the resulting disks are entirely supported by the pressure of the magnetic fields against the component of gravitational force [...]]]></description>
			<content:encoded><![CDATA[<p>In this paper we report on the formation of magnetically-levitating accretion disks around supermassive black holes. The structure of these disks is calculated by numerically modelling tidal disruption of magnetized interstellar gas clouds. We find that the resulting disks are entirely supported by the pressure of the magnetic fields against the component of gravitational force directed perpendicular to the disks. The magnetic field shows ordered large-scale geometry that remains stable for the duration of our numerical experiments extending over 10% of the disk lifetime. Strong magnetic pressure allows high accretion rate and inhibits disk fragmentation. This in combination with the repeated feeding of manetized molecular clouds to a supermassive black hole yields a possible solution to the long-standing puzzle of black hole growth in the centres of galaxies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/25/magnetically-levitating-disks-around-supermassive-black-holes-replacement/feed/</wfw:commentRss>
		<slash:comments>1</slash:comments>
		</item>
		<item>
		<title>The surface detector array of the Telescope Array experiment [Replacement]</title>
		<link>http://voxcharta.org/2012/01/25/the-surface-detector-array-of-the-telescope-array-experiment-replacement/</link>
		<comments>http://voxcharta.org/2012/01/25/the-surface-detector-array-of-the-telescope-array-experiment-replacement/#comments</comments>
		<pubDate>Thu, 26 Jan 2012 01:31:21 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[detector array]]></category>
		<category><![CDATA[extensive air showers]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[observation]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[photon]]></category>
		<category><![CDATA[simultaneous detection]]></category>
		<category><![CDATA[surface detector]]></category>
		<category><![CDATA[technical features]]></category>
		<category><![CDATA[telescope array]]></category>
		<category><![CDATA[utah usa]]></category>
		<category><![CDATA[western desert]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/25/the-surface-detector-array-of-the-telescope-array-experiment-replacement/</guid>
		<description><![CDATA[The Telescope Array (TA) experiment, located in the western desert of Utah,USA, is designed for observation of extensive air showers from extremely high energy cosmic rays. The experiment has a surface detector array surrounded by three fluorescence detectors to enable simultaneous detection of shower particles at ground level and fluorescence photons along the shower track. [...]]]></description>
			<content:encoded><![CDATA[<p>The Telescope Array (TA) experiment, located in the western desert of Utah,USA, is designed for observation of extensive air showers from extremely high energy cosmic rays. The experiment has a surface detector array surrounded by three fluorescence detectors to enable simultaneous detection of shower particles at ground level and fluorescence photons along the shower track. The TA surface detectors and fluorescence detectors started full hybrid observation in March, 2008. In this article we describe the design and technical features of the TA surface detector.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/25/the-surface-detector-array-of-the-telescope-array-experiment-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Optimizing Automated Classification of Periodic Variable Stars in New Synoptic Surveys</title>
		<link>http://voxcharta.org/2012/01/24/optimizing-automated-classification-of-periodic-variable-stars-in-new-synoptic-surveys/</link>
		<comments>http://voxcharta.org/2012/01/24/optimizing-automated-classification-of-periodic-variable-stars-in-new-synoptic-surveys/#comments</comments>
		<pubDate>Wed, 25 Jan 2012 01:55:28 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[challenges]]></category>
		<category><![CDATA[classifier]]></category>
		<category><![CDATA[classifier performance]]></category>
		<category><![CDATA[databases]]></category>
		<category><![CDATA[distributions]]></category>
		<category><![CDATA[error rate]]></category>
		<category><![CDATA[feature space]]></category>
		<category><![CDATA[gaia]]></category>
		<category><![CDATA[hipparcos]]></category>
		<category><![CDATA[intention]]></category>
		<category><![CDATA[light curve]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[lsst]]></category>
		<category><![CDATA[metrics]]></category>
		<category><![CDATA[mismatch]]></category>
		<category><![CDATA[ogle]]></category>
		<category><![CDATA[promises]]></category>
		<category><![CDATA[real world]]></category>
		<category><![CDATA[synoptic survey]]></category>
		<category><![CDATA[variable star]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/24/optimizing-automated-classification-of-periodic-variable-stars-in-new-synoptic-surveys/</guid>
		<description><![CDATA[Efficient and automated classification of periodic variable stars is becoming increasingly important as the scale of astronomical surveys grows. Several recent papers have used methods from machine learning and statistics to construct classifiers on databases of labeled, multi&#8211;epoch sources with the intention of using these classifiers to automatically infer the classes of unlabeled sources from [...]]]></description>
			<content:encoded><![CDATA[<p>Efficient and automated classification of periodic variable stars is becoming increasingly important as the scale of astronomical surveys grows. Several recent papers have used methods from machine learning and statistics to construct classifiers on databases of labeled, multi&#8211;epoch sources with the intention of using these classifiers to automatically infer the classes of unlabeled sources from new surveys. However, the same source observed with two different synoptic surveys will generally yield different derived metrics (features) from the light curve. Since such features are used in classifiers, this survey-dependent mismatch in feature space will typically lead to degraded classifier performance. In this paper we show how and why feature distributions change using OGLE and \textit{Hipparcos} light curves. To overcome survey systematics, we apply a method, \textit{noisification}, which attempts to empirically match distributions of features between the labeled sources used to construct the classifier and the unlabeled sources we wish to classify. Results from simulated and real&#8211;world light curves show that noisification can significantly improve classifier performance. In a three&#8211;class problem using light curves from \textit{Hipparcos} and OGLE, noisification reduces the classifier error rate from 27.0% to 7.0%. We recommend that noisification be used for upcoming surveys such as Gaia and LSST and describe some of the promises and challenges of applying noisification to these surveys.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/24/optimizing-automated-classification-of-periodic-variable-stars-in-new-synoptic-surveys/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Magnetically-levitating disks around supermassive black holes</title>
		<link>http://voxcharta.org/2012/01/24/magnetically-levitating-disks-around-supermassive-black-holes/</link>
		<comments>http://voxcharta.org/2012/01/24/magnetically-levitating-disks-around-supermassive-black-holes/#comments</comments>
		<pubDate>Wed, 25 Jan 2012 01:54:23 +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[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion disk]]></category>
		<category><![CDATA[disk fragmentation]]></category>
		<category><![CDATA[duration]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gravitational force]]></category>
		<category><![CDATA[interstellar gas clouds]]></category>
		<category><![CDATA[lifetime]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetic pressure]]></category>
		<category><![CDATA[molecular cloud]]></category>
		<category><![CDATA[numerical experiment]]></category>
		<category><![CDATA[possible solution]]></category>
		<category><![CDATA[puzzle]]></category>
		<category><![CDATA[scale geometry]]></category>
		<category><![CDATA[supermassive black hole]]></category>
		<category><![CDATA[tidal disruption]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/24/magnetically-levitating-disks-around-supermassive-black-holes/</guid>
		<description><![CDATA[In this paper we report on the formation of magnetically-levitating accretion disks around supermassive black holes. The structure of these disks is calculated by numerically modelling tidal disruption of magnetized interstellar gas clouds. We find that the resulting disks are entirely supported by the pressure of the magnetic fields against the component of gravitational force [...]]]></description>
			<content:encoded><![CDATA[<p>In this paper we report on the formation of magnetically-levitating accretion disks around supermassive black holes. The structure of these disks is calculated by numerically modelling tidal disruption of magnetized interstellar gas clouds. We find that the resulting disks are entirely supported by the pressure of the magnetic fields against the component of gravitational force directed perpendicular to the disks. The magnetic field shows ordered large-scale geometry that remains stable for the duration of our numerical experiments extending over 10% of the disk lifetime. Strong magnetic pressure allows high accretion and inhibits disk fragmentation. This in combination with the repeated feeding of manetized molecular clouds to a supermassive black hole yields a possible solution to the long-standing puzzle of black hole growth in the centres of galaxies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/24/magnetically-levitating-disks-around-supermassive-black-holes/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The surface detector array of the Telescope Array experiment to explore the highest energy cosmic rays</title>
		<link>http://voxcharta.org/2012/01/24/the-surface-detector-array-of-the-telescope-array-experiment-to-explore-the-highest-energy-cosmic-rays/</link>
		<comments>http://voxcharta.org/2012/01/24/the-surface-detector-array-of-the-telescope-array-experiment-to-explore-the-highest-energy-cosmic-rays/#comments</comments>
		<pubDate>Wed, 25 Jan 2012 01:50:22 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[detector array]]></category>
		<category><![CDATA[extensive air showers]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[highest energy]]></category>
		<category><![CDATA[observation]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[photon]]></category>
		<category><![CDATA[simultaneous detection]]></category>
		<category><![CDATA[surface detector]]></category>
		<category><![CDATA[technical features]]></category>
		<category><![CDATA[telescope array]]></category>
		<category><![CDATA[utah usa]]></category>
		<category><![CDATA[western desert]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/24/the-surface-detector-array-of-the-telescope-array-experiment-to-explore-the-highest-energy-cosmic-rays/</guid>
		<description><![CDATA[The Telescope Array (TA) experiment, located in the western desert of Utah,USA, is designed for observation of extensive air showers from extremely high energy cosmic rays. The experiment has a surface detector array surrounded by three fluorescence detectors to enable simultaneous detection of shower particles at ground level and fluorescence photons along the shower track. [...]]]></description>
			<content:encoded><![CDATA[<p>The Telescope Array (TA) experiment, located in the western desert of Utah,USA, is designed for observation of extensive air showers from extremely high energy cosmic rays. The experiment has a surface detector array surrounded by three fluorescence detectors to enable simultaneous detection of shower particles at ground level and fluorescence photons along the shower track. The TA surface detectors and fluorescence detectors started full hybrid observation in March, 2008. In this article we describe the design and technical features of the TA surface detector.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/24/the-surface-detector-array-of-the-telescope-array-experiment-to-explore-the-highest-energy-cosmic-rays/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>PyCOOL &#8211; a Cosmological Object-Oriented Lattice code written in Python</title>
		<link>http://voxcharta.org/2012/01/24/pycool-a-cosmological-object-oriented-lattice-code-written-in-python/</link>
		<comments>http://voxcharta.org/2012/01/24/pycool-a-cosmological-object-oriented-lattice-code-written-in-python/#comments</comments>
		<pubDate>Wed, 25 Jan 2012 01:44:59 +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[chaotic inflation]]></category>
		<category><![CDATA[consumer graphics]]></category>
		<category><![CDATA[cosmological model]]></category>
		<category><![CDATA[curvature]]></category>
		<category><![CDATA[early universe]]></category>
		<category><![CDATA[field model]]></category>
		<category><![CDATA[gnu general public license]]></category>
		<category><![CDATA[graphics card]]></category>
		<category><![CDATA[graphics processing unit]]></category>
		<category><![CDATA[lattice simulations]]></category>
		<category><![CDATA[perturbation]]></category>
		<category><![CDATA[post processing]]></category>
		<category><![CDATA[python language]]></category>
		<category><![CDATA[python program]]></category>
		<category><![CDATA[scalar field]]></category>
		<category><![CDATA[speed accuracy]]></category>
		<category><![CDATA[sweet spot]]></category>
		<category><![CDATA[symplectic integrator]]></category>
		<category><![CDATA[www physics]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/24/pycool-a-cosmological-object-oriented-lattice-code-written-in-python/</guid>
		<description><![CDATA[There are a number of different phenomena in the early universe that have to be studied numerically with lattice simulations. This paper presents a graphics processing unit (GPU) accelerated Python program called PyCOOL that solves the evolution of scalar fields in a lattice with very precise symplectic integrators. The program has been written with the [...]]]></description>
			<content:encoded><![CDATA[<p>There are a number of different phenomena in the early universe that have to be studied numerically with lattice simulations. This paper presents a graphics processing unit (GPU) accelerated Python program called PyCOOL that solves the evolution of scalar fields in a lattice with very precise symplectic integrators. The program has been written with the intention to hit a sweet spot of speed, accuracy and user friendliness. This has been achieved by using the Python language with the PyCUDA interface to make a program that is easy to adapt to different scalar field models. In this paper we derive the symplectic dynamics that govern the evolution of the system and then present the implementation of the program in Python and PyCUDA. The functionality of the program is tested in a chaotic inflation preheating model, a single field oscillon case and in a supersymmetric curvaton model which leads to Q-ball production. We have also compared the performance of a consumer graphics card to a professional Tesla compute card in these simulations. We find that the program is not only accurate but also very fast. To further increase the usefulness of the program we have equipped it with numerous post-processing functions that provide useful information about the cosmological model. These include various spectra and statistics of the fields. The program can be additionally used to calculate the generated curvature perturbation. The program is publicly available under GNU General Public License at <a href="https://github.com/jtksai/PyCOOL">https://github.com/jtksai/PyCOOL</a> . Some additional information can be found from <a href="http://www.physics.utu.fi/tiedostot/theory/particlecosmology/pycool/">http://www.physics.utu.fi/tiedostot/theory/particlecosmology/pycool/</a> .</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/24/pycool-a-cosmological-object-oriented-lattice-code-written-in-python/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Radioscience simulations in General Relativity and in alternative theories of gravity [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/01/24/radioscience-simulations-in-general-relativity-and-in-alternative-theories-of-gravity-cross-listing/</link>
		<comments>http://voxcharta.org/2012/01/24/radioscience-simulations-in-general-relativity-and-in-alternative-theories-of-gravity-cross-listing/#comments</comments>
		<pubDate>Wed, 25 Jan 2012 01:43:44 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[aim]]></category>
		<category><![CDATA[arc]]></category>
		<category><![CDATA[cassini mission]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[doppler]]></category>
		<category><![CDATA[flexible approach]]></category>
		<category><![CDATA[general relativity]]></category>
		<category><![CDATA[gravity]]></category>
		<category><![CDATA[initial condition]]></category>
		<category><![CDATA[least square]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[metric theory]]></category>
		<category><![CDATA[new software]]></category>
		<category><![CDATA[orders of magnitude]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[signal]]></category>
		<category><![CDATA[signature]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[solar system]]></category>
		<category><![CDATA[space time]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/24/radioscience-simulations-in-general-relativity-and-in-alternative-theories-of-gravity-cross-listing/</guid>
		<description><![CDATA[In this paper, we focus on the possibility to test General Relativity in the Solar System with radioscience measurements. To this aim, we present a new software that simulates Range and Doppler signals directly from the space-time metric. This flexible approach allows one to perform simulations in General Relativity and in alternative metric theories of [...]]]></description>
			<content:encoded><![CDATA[<p>In this paper, we focus on the possibility to test General Relativity in the Solar System with radioscience measurements. To this aim, we present a new software that simulates Range and Doppler signals directly from the space-time metric. This flexible approach allows one to perform simulations in General Relativity and in alternative metric theories of gravity. In a second step, a least-squares fit of the different initial conditions involved in the situation is performed in order to compare anomalous signals produced by a given alternative theory with the ones obtained in General Relativity. This software provides orders of magnitude and signatures stemming from hypothetical alternative theories of gravity on radioscience signals. As an application, we present some simulations done for the Cassini mission in Post-Einsteinian Gravity and in the context of MOND External Field Effect. We deduce constraints on the Post-Einsteinian parameters but find that the considered arc of the Cassini mission is not useful to constrain the MOND External Field Effect.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/24/radioscience-simulations-in-general-relativity-and-in-alternative-theories-of-gravity-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A reconstruction method for neutrino induced muon tracks taking into account the apriori knowledge of the neutrino source</title>
		<link>http://voxcharta.org/2012/01/24/a-reconstruction-method-for-neutrino-induced-muon-tracks-taking-into-account-the-apriori-knowledge-of-the-neutrino-source/</link>
		<comments>http://voxcharta.org/2012/01/24/a-reconstruction-method-for-neutrino-induced-muon-tracks-taking-into-account-the-apriori-knowledge-of-the-neutrino-source/#comments</comments>
		<pubDate>Wed, 25 Jan 2012 01:43:15 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accelerator]]></category>
		<category><![CDATA[apriori knowledge]]></category>
		<category><![CDATA[astrophysical objects]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[efficiency]]></category>
		<category><![CDATA[gamma ray sources]]></category>
		<category><![CDATA[muon]]></category>
		<category><![CDATA[neutrino]]></category>
		<category><![CDATA[neutrino source]]></category>
		<category><![CDATA[origin of cosmic rays]]></category>
		<category><![CDATA[reconstruction method]]></category>
		<category><![CDATA[satellite experiment]]></category>
		<category><![CDATA[Telescope]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/24/a-reconstruction-method-for-neutrino-induced-muon-tracks-taking-into-account-the-apriori-knowledge-of-the-neutrino-source/</guid>
		<description><![CDATA[Gamma ray earthbound and satellite experiments have discovered, over the last years, many Galactic and extragalactic gamma ray sources. The detection of astrophysical neutrinos emitted by the same sources would imply that these astrophysical objects are charged cosmic ray accelerators and help to resolve the enigma of the origin of cosmic rays. A very large [...]]]></description>
			<content:encoded><![CDATA[<p>Gamma ray earthbound and satellite experiments have discovered, over the last years, many Galactic and extragalactic gamma ray sources. The detection of astrophysical neutrinos emitted by the same sources would imply that these astrophysical objects are charged cosmic ray accelerators and help to resolve the enigma of the origin of cosmic rays. A very large volume neutrino telescope will be able to detect these potential neutrino emitters. The apriori known direction of the neutrino source can be used to effectively suppress the $^{40}K$ optical background and increase significantly the tracking efficiency through causality filters. We report on advancing filtering and prefit techniques using the known neutrino source direction and first results are presented.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/24/a-reconstruction-method-for-neutrino-induced-muon-tracks-taking-into-account-the-apriori-knowledge-of-the-neutrino-source/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Reconstruction efficiency and discovery potential of a Mediterranean neutrino telescope: A simulation study using the Hellenic Open University Simulation &amp; Reconstruction (HOURS) package</title>
		<link>http://voxcharta.org/2012/01/24/reconstruction-efficiency-and-discovery-potential-of-a-mediterranean-neutrino-telescope-a-simulation-study-using-the-hellenic-open-university-simulation-reconstruction-hours-package/</link>
		<comments>http://voxcharta.org/2012/01/24/reconstruction-efficiency-and-discovery-potential-of-a-mediterranean-neutrino-telescope-a-simulation-study-using-the-hellenic-open-university-simulation-reconstruction-hours-package/#comments</comments>
		<pubDate>Wed, 25 Jan 2012 01:41:14 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[angular resolution]]></category>
		<category><![CDATA[atmospheric neutrino]]></category>
		<category><![CDATA[capability]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[energy neutrino]]></category>
		<category><![CDATA[experimental time]]></category>
		<category><![CDATA[gamma ray emission]]></category>
		<category><![CDATA[hadronic interactions]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[muon]]></category>
		<category><![CDATA[neutrino flux]]></category>
		<category><![CDATA[neutrino telescope]]></category>
		<category><![CDATA[open university]]></category>
		<category><![CDATA[point source]]></category>
		<category><![CDATA[reconstruction efficiency]]></category>
		<category><![CDATA[simulation study]]></category>
		<category><![CDATA[software package]]></category>
		<category><![CDATA[university simulation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/24/reconstruction-efficiency-and-discovery-potential-of-a-mediterranean-neutrino-telescope-a-simulation-study-using-the-hellenic-open-university-simulation-reconstruction-hours-package/</guid>
		<description><![CDATA[We report on the evaluation of the performance of a Mediterranean very large volume neutrino telescope. We present results of our studies concerning the capability of the telescope in detecting/discovering galactic (steady point sources) and extragalactic, transient (Gamma Ray Bursts) high energy neutrino sources as well as measuring ultra high energy diffuse neutrino fluxes. The [...]]]></description>
			<content:encoded><![CDATA[<p>We report on the evaluation of the performance of a Mediterranean very large volume neutrino telescope. We present results of our studies concerning the capability of the telescope in detecting/discovering galactic (steady point sources) and extragalactic, transient (Gamma Ray Bursts) high energy neutrino sources as well as measuring ultra high energy diffuse neutrino fluxes. The neutrino effective area and angular resolution are presented as a function of the neutrino energy, and the background event rate (atmospheric neutrinos and muons) is estimated. The discovery potential of the neutrino telescope is evaluated and the experimental time required for a significant discovery of potential neutrino emitters (known from their gamma ray emission, assumedly produced by hadronic interactions) is estimated. For the simulation we use the HOU Reconstruction &amp; Simulation (HOURS) software package.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/24/reconstruction-efficiency-and-discovery-potential-of-a-mediterranean-neutrino-telescope-a-simulation-study-using-the-hellenic-open-university-simulation-reconstruction-hours-package/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Identifying Patterns on Cosmic Ray Maps with Wavelets on the Sphere [Replacement]</title>
		<link>http://voxcharta.org/2012/01/24/identifying-patterns-on-cosmic-ray-maps-with-wavelets-on-the-sphere-replacement/</link>
		<comments>http://voxcharta.org/2012/01/24/identifying-patterns-on-cosmic-ray-maps-with-wavelets-on-the-sphere-replacement/#comments</comments>
		<pubDate>Wed, 25 Jan 2012 01:32:50 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cosmic magnetic fields]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[deflection]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[map]]></category>
		<category><![CDATA[shape]]></category>
		<category><![CDATA[spectrum]]></category>
		<category><![CDATA[sphere]]></category>
		<category><![CDATA[wavelet]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/24/identifying-patterns-on-cosmic-ray-maps-with-wavelets-on-the-sphere-replacement/</guid>
		<description><![CDATA[The deflection of ultra-high energy cosmic rays depends on the shape of the injection spectrum of the source and the pervasive cosmic magnetic fields. In this work it is applied the wavelet transform on the sphere to search for energy ordered filamentary structures arisen from magnetic bending. These structures, the so-called multiplets, can bring relevant [...]]]></description>
			<content:encoded><![CDATA[<p>The deflection of ultra-high energy cosmic rays depends on the shape of the injection spectrum of the source and the pervasive cosmic magnetic fields. In this work it is applied the wavelet transform on the sphere to search for energy ordered filamentary structures arisen from magnetic bending. These structures, the so-called multiplets, can bring relevant information concerning the intervening magnetic fields.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/24/identifying-patterns-on-cosmic-ray-maps-with-wavelets-on-the-sphere-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Recoiling Ion-Channeling in Direct Dark Matter Detectors</title>
		<link>http://voxcharta.org/2012/01/23/recoiling-ion-channeling-in-direct-dark-matter-detectors/</link>
		<comments>http://voxcharta.org/2012/01/23/recoiling-ion-channeling-in-direct-dark-matter-detectors/#comments</comments>
		<pubDate>Tue, 24 Jan 2012 01:54:13 +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[analytic model]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[estimates]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[modulation]]></category>
		<category><![CDATA[nucleus]]></category>
		<category><![CDATA[scintillation]]></category>
		<category><![CDATA[wimp]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/23/recoiling-ion-channeling-in-direct-dark-matter-detectors/</guid>
		<description><![CDATA[The channeling of the recoiling nucleus in crystalline detectors after a WIMP collision would produce a larger scintillation or ionization signal in direct detection experiments than otherwise expected. I present estimates of channeling fractions obtained using analytic models developed from the 1960&#8217;s onwards to describe channeling and blocking effects. We find the fractions to be [...]]]></description>
			<content:encoded><![CDATA[<p>The channeling of the recoiling nucleus in crystalline detectors after a WIMP collision would produce a larger scintillation or ionization signal in direct detection experiments than otherwise expected. I present estimates of channeling fractions obtained using analytic models developed from the 1960&#8217;s onwards to describe channeling and blocking effects. We find the fractions to be too small to affect the fits to potential WIMP candidates. I also examine the possibility of detecting a daily modulation of the dark matter signal due to channeling.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/23/recoiling-ion-channeling-in-direct-dark-matter-detectors/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Technical aspects in dark matter investigations</title>
		<link>http://voxcharta.org/2012/01/23/technical-aspects-in-dark-matter-investigations/</link>
		<comments>http://voxcharta.org/2012/01/23/technical-aspects-in-dark-matter-investigations/#comments</comments>
		<pubDate>Tue, 24 Jan 2012 01:53:04 +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[dark matter]]></category>
		<category><![CDATA[experimental aspects]]></category>
		<category><![CDATA[experimental result]]></category>
		<category><![CDATA[matter investigations]]></category>
		<category><![CDATA[relevant role]]></category>
		<category><![CDATA[technical aspects]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/23/technical-aspects-in-dark-matter-investigations/</guid>
		<description><![CDATA[Some theoretical and experimental aspects regarding the direct dark matter field are mentioned. In particular some arguments, which play a relevant role in the evaluation of model dependent interpretations of experimental results and in comparisons, are shortly addressed.
]]></description>
			<content:encoded><![CDATA[<p>Some theoretical and experimental aspects regarding the direct dark matter field are mentioned. In particular some arguments, which play a relevant role in the evaluation of model dependent interpretations of experimental results and in comparisons, are shortly addressed.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/23/technical-aspects-in-dark-matter-investigations/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Developing arrayed waveguide grating spectrographs for multi-object astronomical spectroscopy</title>
		<link>http://voxcharta.org/2012/01/23/developing-arrayed-waveguide-grating-spectrographs-for-multi-object-astronomical-spectroscopy/</link>
		<comments>http://voxcharta.org/2012/01/23/developing-arrayed-waveguide-grating-spectrographs-for-multi-object-astronomical-spectroscopy/#comments</comments>
		<pubDate>Tue, 24 Jan 2012 01:50:31 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[aim]]></category>
		<category><![CDATA[astronomical spectroscopy]]></category>
		<category><![CDATA[astronomy]]></category>
		<category><![CDATA[axis]]></category>
		<category><![CDATA[coupler]]></category>
		<category><![CDATA[efficiency]]></category>
		<category><![CDATA[fibers]]></category>
		<category><![CDATA[free spectral range]]></category>
		<category><![CDATA[grade chips]]></category>
		<category><![CDATA[grating]]></category>
		<category><![CDATA[interference]]></category>
		<category><![CDATA[optical fiber]]></category>
		<category><![CDATA[resolving power]]></category>
		<category><![CDATA[several ways]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectral resolution]]></category>
		<category><![CDATA[spectrograph]]></category>
		<category><![CDATA[telecommunication]]></category>
		<category><![CDATA[throughput]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/23/developing-arrayed-waveguide-grating-spectrographs-for-multi-object-astronomical-spectroscopy/</guid>
		<description><![CDATA[With the aim of utilizing arrayed waveguide gratings for multi-object spectroscopy in the field of astronomy, we outline several ways in which standard telecommunications grade chips should be modified. In particular, by removing the parabolic-horn taper or multimode interference coupler, and injecting with an optical fiber directly, the resolving power was increased threefold from 2400 [...]]]></description>
			<content:encoded><![CDATA[<p>With the aim of utilizing arrayed waveguide gratings for multi-object spectroscopy in the field of astronomy, we outline several ways in which standard telecommunications grade chips should be modified. In particular, by removing the parabolic-horn taper or multimode interference coupler, and injecting with an optical fiber directly, the resolving power was increased threefold from 2400 \pm 200 (spectral resolution of 0.63 \pm 0.2 nm) to 7000 \pm 700 (0.22 \pm 0.02 nm) while attaining a throughput of 77 \pm 5%. More importantly, the removal of the taper enabled simultaneous off-axis injection from multiple fibers, significantly increasing the number of spectra that can be obtained at once (i.e. the observing efficiency). Here we report that ~ 12 fibers can be injected simultaneously within the free spectral range of our device, with a 20% reduction in resolving power for fibers placed at 0.8 mm off centre.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/23/developing-arrayed-waveguide-grating-spectrographs-for-multi-object-astronomical-spectroscopy/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Tokyo Axion Helioscope</title>
		<link>http://voxcharta.org/2012/01/23/the-tokyo-axion-helioscope/</link>
		<comments>http://voxcharta.org/2012/01/23/the-tokyo-axion-helioscope/#comments</comments>
		<pubDate>Tue, 24 Jan 2012 01:49:48 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[axion]]></category>
		<category><![CDATA[coherence]]></category>
		<category><![CDATA[conversion]]></category>
		<category><![CDATA[gas container]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[photon]]></category>
		<category><![CDATA[pin photodiode]]></category>
		<category><![CDATA[ray detector]]></category>
		<category><![CDATA[solar core]]></category>
		<category><![CDATA[Sun]]></category>
		<category><![CDATA[technical detail]]></category>
		<category><![CDATA[tokyo]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/23/the-tokyo-axion-helioscope/</guid>
		<description><![CDATA[The Tokyo Axion Helioscope experiment aims to detect axions which are produced in the solar core. The helioscope uses a strong magnetic field in order to convert axions into X-ray photons and has a mounting to follow the sun very accurately. The photons are detected by an X-ray detector which is made of 16 PIN-photodiodes. [...]]]></description>
			<content:encoded><![CDATA[<p>The Tokyo Axion Helioscope experiment aims to detect axions which are produced in the solar core. The helioscope uses a strong magnetic field in order to convert axions into X-ray photons and has a mounting to follow the sun very accurately. The photons are detected by an X-ray detector which is made of 16 PIN-photodiodes. In addition, a gas container and a gas regulation system is adopted for recovering the coherence between axions and photons in the conversion region giving sensitivity to axions with masses up to 2 eV. In this paper, we report on the technical detail of the Tokyo Axion Helioscope.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/23/the-tokyo-axion-helioscope/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A new third-order cosmic shear statistics: Separating E/B-mode correlations on a finite interval</title>
		<link>http://voxcharta.org/2012/01/23/a-new-third-order-cosmic-shear-statistics-separating-eb-mode-correlations-on-a-finite-interval/</link>
		<comments>http://voxcharta.org/2012/01/23/a-new-third-order-cosmic-shear-statistics-separating-eb-mode-correlations-on-a-finite-interval/#comments</comments>
		<pubDate>Tue, 24 Jan 2012 01:41:41 +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[absence]]></category>
		<category><![CDATA[cmb polarization]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[correlation function]]></category>
		<category><![CDATA[cosmic shear]]></category>
		<category><![CDATA[decomposition]]></category>
		<category><![CDATA[e mode]]></category>
		<category><![CDATA[finite interval]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gravitational lensing]]></category>
		<category><![CDATA[minimum separation]]></category>
		<category><![CDATA[modes]]></category>
		<category><![CDATA[numerical simulation]]></category>
		<category><![CDATA[ring statistics]]></category>
		<category><![CDATA[scales]]></category>
		<category><![CDATA[separation problems]]></category>
		<category><![CDATA[statistic]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/23/a-new-third-order-cosmic-shear-statistics-separating-eb-mode-correlations-on-a-finite-interval/</guid>
		<description><![CDATA[Decomposing the shear signal into E and B-modes properly, i.e. without leakage of B-modes into the E-mode signal and vice versa, has been a long-standing problem in weak gravitational lensing. At the two-point level this problem was resolved by developing the so-called ring statistics, and later the COSEBIs; however, extending these concepts to the three-point [...]]]></description>
			<content:encoded><![CDATA[<p>Decomposing the shear signal into E and B-modes properly, i.e. without leakage of B-modes into the E-mode signal and vice versa, has been a long-standing problem in weak gravitational lensing. At the two-point level this problem was resolved by developing the so-called ring statistics, and later the COSEBIs; however, extending these concepts to the three-point level is far from trivial. Currently used methods to decompose three-point shear correlation functions (3PCFs) into E- and B-modes require knowledge of the 3PCF down to arbitrary small scales. This implies that the 3PCF needs to be modeled on scales smaller than the minimum separation of 2 galaxies and subsequently will be biased towards the model, or, in the absence of a model, the statistics is affected by E/B-mode leakage (or mixing). In this paper we derive a new third-order E/B-mode statistic that performs the decomposition using the 3PCF only on a finite interval, and thereby is free of any E/B-mode leakage while at the same time relying solely on information from the data. In addition, we relate this third-order ring statistics to the convergence field, thereby enabling a fast and convenient calculation of this statistic from numerical simulations. We note that our new statistics should be applicable to corresponding E/B-mode separation problems in the CMB polarization field.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/23/a-new-third-order-cosmic-shear-statistics-separating-eb-mode-correlations-on-a-finite-interval/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Benchmarking CRBLASTER on the 350-MHz 49-core Maestro Development Board</title>
		<link>http://voxcharta.org/2012/01/23/benchmarking-crblaster-on-the-350-mhz-49-core-maestro-development-board/</link>
		<comments>http://voxcharta.org/2012/01/23/benchmarking-crblaster-on-the-350-mhz-49-core-maestro-development-board/#comments</comments>
		<pubDate>Tue, 24 Jan 2012 01:40:52 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[computational framework]]></category>
		<category><![CDATA[core processor]]></category>
		<category><![CDATA[cosmic ray rejection]]></category>
		<category><![CDATA[floating point]]></category>
		<category><![CDATA[fpu]]></category>
		<category><![CDATA[generation computer]]></category>
		<category><![CDATA[image analysis programs]]></category>
		<category><![CDATA[interface mpi]]></category>
		<category><![CDATA[interim test]]></category>
		<category><![CDATA[message passing interface]]></category>
		<category><![CDATA[mpi library]]></category>
		<category><![CDATA[node beowulf cluster]]></category>
		<category><![CDATA[noise generator]]></category>
		<category><![CDATA[parallel algorithm]]></category>
		<category><![CDATA[performance comparison]]></category>
		<category><![CDATA[point operations]]></category>
		<category><![CDATA[poisson noise]]></category>
		<category><![CDATA[radiation environment]]></category>
		<category><![CDATA[research scientists]]></category>
		<category><![CDATA[test chip]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/23/benchmarking-crblaster-on-the-350-mhz-49-core-maestro-development-board/</guid>
		<description><![CDATA[I describe the performance of the CRBLASTER computational framework on a 350-MHz 49-core Maestro Development Board (MDB). The 49-core Interim Test Chip (ITC) was developed by the U.S. Government and is based on the intellectual property of the 64-core TILE64 processor of the Tilera Corporation. The Maestro processor is intended for use in the high [...]]]></description>
			<content:encoded><![CDATA[<p>I describe the performance of the CRBLASTER computational framework on a 350-MHz 49-core Maestro Development Board (MDB). The 49-core Interim Test Chip (ITC) was developed by the U.S. Government and is based on the intellectual property of the 64-core TILE64 processor of the Tilera Corporation. The Maestro processor is intended for use in the high radiation environments found in space; the ITC was fabricated using IBM 90-nm CMOS 9SF technology and Radiation-Hardening-by-Design (RHDB) rules. CRBLASTER is a parallel-processing cosmic-ray rejection application based on a simple computational framework that uses the high-performance computing industry standard Message Passing Interface (MPI) library. CRBLASTER was designed to be used by research scientists to easily port image-analysis programs based on embarrassingly-parallel algorithms to a parallel-processing environment such as a multi-node Beowulf cluster or multi-core processors using MPI. I describe my experience of porting CRBLASTER to the 64-core TILE64 processor, the Maestro simulator, and finally the 49-core Maestro processor itself. Performance comparisons using the ITC are presented between emulating all floating-point operations in software and doing all floating point operations with hardware assist from an IEEE-754 compliant Aurora FPU (floating point unit) that is attached to each of the 49 cores. Benchmarking of the CRBLASTER computational framework using the memory-intensive L.A.COSMIC cosmic ray rejection algorithm and a computational-intensive Poisson noise generator reveal subtleties of the Maestro hardware design. Lastly, I describe the importance of using real scientific applications during the testing phase of next-generation computer hardware; complex real-world scientific applications can stress hardware in novel ways that may not necessarily be revealed while executing simple applications or unit tests.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/23/benchmarking-crblaster-on-the-350-mhz-49-core-maestro-development-board/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The reliability of the AIC method in Cosmological Model Selection [Replacement]</title>
		<link>http://voxcharta.org/2012/01/23/the-reliability-of-the-aic-method-in-cosmological-model-selection-replacement/</link>
		<comments>http://voxcharta.org/2012/01/23/the-reliability-of-the-aic-method-in-cosmological-model-selection-replacement/#comments</comments>
		<pubDate>Tue, 24 Jan 2012 01:36:28 +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[aic]]></category>
		<category><![CDATA[akaike information criterion]]></category>
		<category><![CDATA[appropriateness]]></category>
		<category><![CDATA[bootstrap technique]]></category>
		<category><![CDATA[candidate models]]></category>
		<category><![CDATA[choices]]></category>
		<category><![CDATA[cosmological model]]></category>
		<category><![CDATA[dark energy]]></category>
		<category><![CDATA[discrepancy]]></category>
		<category><![CDATA[distributions]]></category>
		<category><![CDATA[divergence]]></category>
		<category><![CDATA[energy model]]></category>
		<category><![CDATA[model comparison]]></category>
		<category><![CDATA[model selection]]></category>
		<category><![CDATA[realization]]></category>
		<category><![CDATA[reliability]]></category>
		<category><![CDATA[statistical error]]></category>
		<category><![CDATA[suitable conditions]]></category>
		<category><![CDATA[threshold parameter]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/23/the-reliability-of-the-aic-method-in-cosmological-model-selection-replacement/</guid>
		<description><![CDATA[The Akaike information criterion (AIC) has been used as a statistical criterion to compare the appropriateness of different dark energy candidate models underlying a particular data set. Under suitable conditions, the AIC is an indirect estimate of the Kullback-Leibler divergence D(T//A) of a candidate model A with respect to the truth T. Thus, a dark [...]]]></description>
			<content:encoded><![CDATA[<p>The Akaike information criterion (AIC) has been used as a statistical criterion to compare the appropriateness of different dark energy candidate models underlying a particular data set. Under suitable conditions, the AIC is an indirect estimate of the Kullback-Leibler divergence D(T//A) of a candidate model A with respect to the truth T. Thus, a dark energy model with a smaller AIC is ranked as a better model, since it has a smaller Kullback-Leibler discrepancy with T. In this paper, we explore the impact of statistical errors in estimating the AIC during model comparison. Using a parametric bootstrap technique, we study the distribution of AIC differences between a set of candidate models due to different realizations of noise in the data and show that the shape and spread of this distribution can be quite varied. We also study the rate of success of the AIC procedure for different values of a threshold parameter popularly used in the literature. For plausible choices of true dark energy models, our studies suggest that investigating such distributions of AIC differences in addition to the threshold is useful in correctly interpreting comparisons of dark energy models using the AIC technique.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/23/the-reliability-of-the-aic-method-in-cosmological-model-selection-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Radiation hardness studies of InGaAs and Si photodiodes at 30, 52, &amp; 98 MeV and fluences to 5&#215;10^11 protons/cm^2 [Replacement]</title>
		<link>http://voxcharta.org/2012/01/23/radiation-hardness-studies-of-ingaas-and-si-photodiodes-at-30-52-98-mev-and-fluences-to-5x1011-protonscm2-replacement/</link>
		<comments>http://voxcharta.org/2012/01/23/radiation-hardness-studies-of-ingaas-and-si-photodiodes-at-30-52-98-mev-and-fluences-to-5x1011-protonscm2-replacement/#comments</comments>
		<pubDate>Tue, 24 Jan 2012 01:36:18 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cm 2]]></category>
		<category><![CDATA[degradation]]></category>
		<category><![CDATA[effects of ionizing radiation]]></category>
		<category><![CDATA[indiana university cyclotron facility]]></category>
		<category><![CDATA[ingaas photodiodes]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[mev protons]]></category>
		<category><![CDATA[radiation hardness]]></category>
		<category><![CDATA[responsivity]]></category>
		<category><![CDATA[university cyclotron facility]]></category>
		<category><![CDATA[wavelength]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/23/radiation-hardness-studies-of-ingaas-and-si-photodiodes-at-30-52-98-mev-and-fluences-to-5x1011-protonscm2-replacement/</guid>
		<description><![CDATA[Here we report the results of an investigation into the effects of ionizing radiation on commercial-off-the-shelf InGaAs and Si photodiodes. The photodiodes were exposed to 30, 52, and 98 MeV protons with fluences ranging from 10^8 &#8211; 5&#215;10^11 protons/cm^2 at the Indiana University Cyclotron Facility. We tested the photodiodes for changes to their dark current [...]]]></description>
			<content:encoded><![CDATA[<p>Here we report the results of an investigation into the effects of ionizing radiation on commercial-off-the-shelf InGaAs and Si photodiodes. The photodiodes were exposed to 30, 52, and 98 MeV protons with fluences ranging from 10^8 &#8211; 5&#215;10^11 protons/cm^2 at the Indiana University Cyclotron Facility. We tested the photodiodes for changes to their dark current and their relative responsivity as a function of wavelength. The Si photodiodes showed increasing damage to their responsivity with increasing fluence; the InGaAs photodiodes showed significantly increased dark current as the fluence increased. In addition, we monitored the absolute responsivity of the InGaAs photodiodes over their entire bandpass. Our measurements showed no evidence for broadband degradation or graying of the response at the fluences tested. All measurements in this investigation were made relative to detectors traceable to NIST standards.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/23/radiation-hardness-studies-of-ingaas-and-si-photodiodes-at-30-52-98-mev-and-fluences-to-5x1011-protonscm2-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Radio-optical outlier quasars &#8211; a case study with ICRF2 and SDSS</title>
		<link>http://voxcharta.org/2012/01/22/radio-optical-outlier-quasars-a-case-study-with-icrf2-and-sdss/</link>
		<comments>http://voxcharta.org/2012/01/22/radio-optical-outlier-quasars-a-case-study-with-icrf2-and-sdss/#comments</comments>
		<pubDate>Mon, 23 Jan 2012 01:49:21 +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[active galactic nuclei]]></category>
		<category><![CDATA[astrometric data]]></category>
		<category><![CDATA[baseline interferometry]]></category>
		<category><![CDATA[common objects]]></category>
		<category><![CDATA[digital sky survey]]></category>
		<category><![CDATA[faint magnitude limit]]></category>
		<category><![CDATA[independent check]]></category>
		<category><![CDATA[optical link]]></category>
		<category><![CDATA[orders of magnitude]]></category>
		<category><![CDATA[positional accuracy]]></category>
		<category><![CDATA[radio brightness]]></category>
		<category><![CDATA[radio positions]]></category>
		<category><![CDATA[radio source]]></category>
		<category><![CDATA[reference frame]]></category>
		<category><![CDATA[sdss]]></category>
		<category><![CDATA[sigma level]]></category>
		<category><![CDATA[sky coverage]]></category>
		<category><![CDATA[sky survey data]]></category>
		<category><![CDATA[sloan digital]]></category>
		<category><![CDATA[vlbi observations]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/22/radio-optical-outlier-quasars-a-case-study-with-icrf2-and-sdss/</guid>
		<description><![CDATA[With Gaia, it will become possible to directly link the radio and optical reference frames using a large number of common objects. For the most accurate radio-optical link, it is important to know the level of spatial coincidence between the quasars&#8217; optical positions, and the radio positions determined by Very Long Baseline Interferometry (VLBI) observations. [...]]]></description>
			<content:encoded><![CDATA[<p>With Gaia, it will become possible to directly link the radio and optical reference frames using a large number of common objects. For the most accurate radio-optical link, it is important to know the level of spatial coincidence between the quasars&#8217; optical positions, and the radio positions determined by Very Long Baseline Interferometry (VLBI) observations. The &#8220;outlier&#8221; objects, for which the positions are significantly offset at the two different electromagnetic wavebands, may be of astrophysical interest as well. Here we present a case study to compare the radio positions of ~800 quasars common in the second realization of the International Celestial Reference Frame (ICRF2) and in the Sloan Digital Sky Survey Data Release 7 (SDSS DR7) catalogue. Compared to the radio ICRF2, the SDSS provides two orders of magnitude less accurate astrometric data in the optical. However, its extensive sky coverage and faint magnitude limit allow us to directly relate the positions of a large sample of radio sources. This way we provide an independent check of the overall accuracy of the SDSS positions and confirm that the astrometric calibration of the latest Data Release 8 (DR8) is poorer than that of the DR7. We find over 20 sources for which the optical and radio brightness peaks are apparently not coincident at least at the 3-sigma level of SDSS DR7 positional accuracy, and briefly discuss the possible causes, including dual active galactic nuclei.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/22/radio-optical-outlier-quasars-a-case-study-with-icrf2-and-sdss/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Spherical 3D Isotropic Wavelets [Replacement]</title>
		<link>http://voxcharta.org/2012/01/22/spherical-3d-isotropic-wavelets-replacement/</link>
		<comments>http://voxcharta.org/2012/01/22/spherical-3d-isotropic-wavelets-replacement/#comments</comments>
		<pubDate>Mon, 23 Jan 2012 01:32:54 +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[algorithm]]></category>
		<category><![CDATA[cosmological data]]></category>
		<category><![CDATA[cosmological simulations]]></category>
		<category><![CDATA[denoising]]></category>
		<category><![CDATA[formalism]]></category>
		<category><![CDATA[fourier]]></category>
		<category><![CDATA[large scale]]></category>
		<category><![CDATA[scale structure]]></category>
		<category><![CDATA[sky coverage]]></category>
		<category><![CDATA[spherical coordinates]]></category>
		<category><![CDATA[structure maps]]></category>
		<category><![CDATA[survey]]></category>
		<category><![CDATA[toy model]]></category>
		<category><![CDATA[wavelet decomposition]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/22/spherical-3d-isotropic-wavelets-replacement/</guid>
		<description><![CDATA[Future cosmological surveys will provide 3D large scale structure maps with large sky coverage, for which a 3D Spherical Fourier-Bessel (SFB) analysis in spherical coordinates is natural. Wavelets are particularly well-suited to the analysis and denoising of cosmological data, but a spherical 3D isotropic wavelet transform does not currently exist to analyse spherical 3D data. [...]]]></description>
			<content:encoded><![CDATA[<p>Future cosmological surveys will provide 3D large scale structure maps with large sky coverage, for which a 3D Spherical Fourier-Bessel (SFB) analysis in spherical coordinates is natural. Wavelets are particularly well-suited to the analysis and denoising of cosmological data, but a spherical 3D isotropic wavelet transform does not currently exist to analyse spherical 3D data. The aim of this paper is to present a new formalism for a spherical 3D isotropic wavelet, i.e. one based on the SFB decomposition of a 3D field and accompany the formalism with a public code to perform wavelet transforms. We describe a new 3D isotropic spherical wavelet decomposition based on the undecimated wavelet transform (UWT) described in Starck et al. 2006. We also present a new fast Discrete Spherical Fourier-Bessel Transform (DSFBT) based on both a discrete Bessel Transform and the HEALPIX angular pixelisation scheme. We test the 3D wavelet transform and as a toy-application, apply a denoising algorithm in wavelet space to the Virgo large box cosmological simulations and find we can successfully remove noise without much loss to the large scale structure. We have described a new spherical 3D isotropic wavelet transform, ideally suited to analyse and denoise future 3D spherical cosmological surveys, which uses a novel Discrete Spherical Fourier-Bessel Transform. We illustrate its potential use for denoising using a toy model. All the algorithms presented in this paper are available for download as a public code called MRS3D at <a href="http://jstarck.free.fr/mrs3d.html">http://jstarck.free.fr/mrs3d.html</a></p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/22/spherical-3d-isotropic-wavelets-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Multi-Chroic Feed-Horn Coupled TES Polarimeters [Replacement]</title>
		<link>http://voxcharta.org/2012/01/22/multi-chroic-feed-horn-coupled-tes-polarimeters-replacement/</link>
		<comments>http://voxcharta.org/2012/01/22/multi-chroic-feed-horn-coupled-tes-polarimeters-replacement/#comments</comments>
		<pubDate>Mon, 23 Jan 2012 01:31:04 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[array]]></category>
		<category><![CDATA[ballon]]></category>
		<category><![CDATA[balloon]]></category>
		<category><![CDATA[bandwidth]]></category>
		<category><![CDATA[cmb polarization]]></category>
		<category><![CDATA[collaboration]]></category>
		<category><![CDATA[cosmic microwave background]]></category>
		<category><![CDATA[excellent control]]></category>
		<category><![CDATA[feed horn]]></category>
		<category><![CDATA[foreground]]></category>
		<category><![CDATA[ghz band]]></category>
		<category><![CDATA[polarimeter]]></category>
		<category><![CDATA[proposal]]></category>
		<category><![CDATA[sensitive detector]]></category>
		<category><![CDATA[sky]]></category>
		<category><![CDATA[space mission]]></category>
		<category><![CDATA[spectral coverage]]></category>
		<category><![CDATA[systematics]]></category>
		<category><![CDATA[technology ideal]]></category>
		<category><![CDATA[truce]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/22/multi-chroic-feed-horn-coupled-tes-polarimeters-replacement/</guid>
		<description><![CDATA[Multi-chroic polarization sensitive detectors offer an avenue to increase both the spectral coverage and sensitivity of instruments optimized for observations of the cosmic-microwave background (CMB) or sub-mm sky. We report on an effort to adapt the Truce Collaboration horn coupled bolometric polarimeters for operation over octave bandwidth. Development is focused on detectors operating in both [...]]]></description>
			<content:encoded><![CDATA[<p>Multi-chroic polarization sensitive detectors offer an avenue to increase both the spectral coverage and sensitivity of instruments optimized for observations of the cosmic-microwave background (CMB) or sub-mm sky. We report on an effort to adapt the Truce Collaboration horn coupled bolometric polarimeters for operation over octave bandwidth. Development is focused on detectors operating in both the 90 and 150 GHz bands which offer the highest CMB polarization to foreground ratio. We plan to deploy an array of 256 multi-chroic 90/150 GHz polarimeters with 1024 TES detectors on ACTPol in 2013, and there are proposals to use this technology for balloon-borne instruments. The combination of excellent control of beam systematics and sensitivity make this technology ideal for future ground, ballon, and space missions.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/22/multi-chroic-feed-horn-coupled-tes-polarimeters-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Comparison of potential ASKAP HI survey source finders</title>
		<link>http://voxcharta.org/2012/01/19/comparison-of-potential-askap-hi-survey-source-finders/</link>
		<comments>http://voxcharta.org/2012/01/19/comparison-of-potential-askap-hi-survey-source-finders/#comments</comments>
		<pubDate>Fri, 20 Jan 2012 01:54:31 +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[algorithm]]></category>
		<category><![CDATA[clipping]]></category>
		<category><![CDATA[completeness]]></category>
		<category><![CDATA[cubes]]></category>
		<category><![CDATA[dimensional data]]></category>
		<category><![CDATA[dingo]]></category>
		<category><![CDATA[hi survey]]></category>
		<category><![CDATA[inclination]]></category>
		<category><![CDATA[number of galaxies]]></category>
		<category><![CDATA[paramount importance]]></category>
		<category><![CDATA[performance difference]]></category>
		<category><![CDATA[point source]]></category>
		<category><![CDATA[reconstruction]]></category>
		<category><![CDATA[reliability]]></category>
		<category><![CDATA[sigma]]></category>
		<category><![CDATA[survey goals]]></category>
		<category><![CDATA[survey source]]></category>
		<category><![CDATA[velocity profile]]></category>
		<category><![CDATA[wallaby]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/19/comparison-of-potential-askap-hi-survey-source-finders/</guid>
		<description><![CDATA[The large size of the ASKAP HI surveys DINGO and WALLABY necessitates automated 3D source finding. A performance difference of a few percent corresponds to a significant number of galaxies being detected or undetected. As such, the performance of the automated source finding is of paramount importance to both of these surveys. We have analysed [...]]]></description>
			<content:encoded><![CDATA[<p>The large size of the ASKAP HI surveys DINGO and WALLABY necessitates automated 3D source finding. A performance difference of a few percent corresponds to a significant number of galaxies being detected or undetected. As such, the performance of the automated source finding is of paramount importance to both of these surveys. We have analysed the performance of various source finders to determine which will allow us to meet our survey goals during the DINGO and WALLABY design studies. Here we present a comparison of the performance of five different methods of automated source finding. These source finders are Duchamp, the Gamma-finder, CNHI, a 2D-1D Wavelet Reconstruction and S+C finder, a sigma clipping method. Each source finder was applied on the same three-dimensional data cubes containing (a) point sources with a Gaussian velocity profile and (b) spatially extended model-galaxies with inclinations and rotation profiles. We focus on the completeness and reliability of each algorithm when comparing the performance of the different source finders.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Solar diameter with 2012 Venus transit</title>
		<link>http://voxcharta.org/2012/01/19/solar-diameter-with-2012-venus-transit/</link>
		<comments>http://voxcharta.org/2012/01/19/solar-diameter-with-2012-venus-transit/#comments</comments>
		<pubDate>Fri, 20 Jan 2012 01:52:26 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absolute calibration]]></category>
		<category><![CDATA[arcsec]]></category>
		<category><![CDATA[atmospheric refraction]]></category>
		<category><![CDATA[circles]]></category>
		<category><![CDATA[diameter of the sun]]></category>
		<category><![CDATA[egress]]></category>
		<category><![CDATA[ephemerides]]></category>
		<category><![CDATA[ingress]]></category>
		<category><![CDATA[mercury transit]]></category>
		<category><![CDATA[optimal condition]]></category>
		<category><![CDATA[phenomenon]]></category>
		<category><![CDATA[planetary disk]]></category>
		<category><![CDATA[radius]]></category>
		<category><![CDATA[solar diameter]]></category>
		<category><![CDATA[solar limb]]></category>
		<category><![CDATA[solar luminosity]]></category>
		<category><![CDATA[solar observatory]]></category>
		<category><![CDATA[transit of venus]]></category>
		<category><![CDATA[unprecedented accuracy]]></category>
		<category><![CDATA[venus transit]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/19/solar-diameter-with-2012-venus-transit/</guid>
		<description><![CDATA[The role of Venus and Mercury transits is crucial to know the past history of the solar diameter. Through the W parameter, the logarithmic derivative of the radius with respect to the luminosity, the past values of the solar luminosity can be recovered. The black drop phenomenon affects the evaluation of the instants of internal [...]]]></description>
			<content:encoded><![CDATA[<p>The role of Venus and Mercury transits is crucial to know the past history of the solar diameter. Through the W parameter, the logarithmic derivative of the radius with respect to the luminosity, the past values of the solar luminosity can be recovered. The black drop phenomenon affects the evaluation of the instants of internal and external contacts between the planetary disk and the solar limb. With these observed instants compared with the ephemerides the value of the solar diameter is recovered. The black drop and seeing effects are overcome with two fitting circles, to Venus and to the Sun, drawn in the undistorted part of the image. The corrections of ephemerides due to the atmospheric refraction will also be taken into account. The forthcoming transit of Venus will allow an accuracy on the diameter of the Sun better than 0.01 arcsec, with good images of the ingress and of the egress taken each second. Chinese solar observatories are in the optimal conditions to obtain valuable data for the measurement of the solar diameter with the Venus transit of 5/6 June 2012 with an unprecedented accuracy, and with absolute calibration given by the ephemerides.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Solar astrometry: the status of art in 2011</title>
		<link>http://voxcharta.org/2012/01/19/solar-astrometry-the-status-of-art-in-2011/</link>
		<comments>http://voxcharta.org/2012/01/19/solar-astrometry-the-status-of-art-in-2011/#comments</comments>
		<pubDate>Fri, 20 Jan 2012 01:52:08 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astrometry]]></category>
		<category><![CDATA[balloon]]></category>
		<category><![CDATA[climate studies]]></category>
		<category><![CDATA[decade]]></category>
		<category><![CDATA[drift scan]]></category>
		<category><![CDATA[evolutionary stage]]></category>
		<category><![CDATA[Measurement]]></category>
		<category><![CDATA[meridian]]></category>
		<category><![CDATA[paramount importance]]></category>
		<category><![CDATA[radius]]></category>
		<category><![CDATA[relationship]]></category>
		<category><![CDATA[satellite]]></category>
		<category><![CDATA[scan mode]]></category>
		<category><![CDATA[shape]]></category>
		<category><![CDATA[solar diameter]]></category>
		<category><![CDATA[space measurement]]></category>
		<category><![CDATA[telescopes]]></category>
		<category><![CDATA[total solar irradiance]]></category>
		<category><![CDATA[transits]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/19/solar-astrometry-the-status-of-art-in-2011/</guid>
		<description><![CDATA[Solar astrometry deals with the accurate measumerent of the solar diameter, and in general with the measurement of the shape of the Sun. During the last decades several techniques have been developed to monitor the radius and the irradiance of the Sun: meridian transits, telescopes in drift-scan mode, solar astrolabes, balloons, and satellites dedicated to [...]]]></description>
			<content:encoded><![CDATA[<p>Solar astrometry deals with the accurate measumerent of the solar diameter, and in general with the measurement of the shape of the Sun. During the last decades several techniques have been developed to monitor the radius and the irradiance of the Sun: meridian transits, telescopes in drift-scan mode, solar astrolabes, balloons, and satellites dedicated to the measurements of the solar diameter, and space measurements of the total solar irradiance are now performed to know the relationship radius-luminosity for the Sun in this evolutionary stage of its life. The feedback of solar astrometry in climate studies is of paramount importance. The status of art in the various fields of research here adressed is outlined.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Sines, steps and droplets: Semiparametric Bayesian modeling of arrival time series</title>
		<link>http://voxcharta.org/2012/01/19/sines-steps-and-droplets-semiparametric-bayesian-modeling-of-arrival-time-series/</link>
		<comments>http://voxcharta.org/2012/01/19/sines-steps-and-droplets-semiparametric-bayesian-modeling-of-arrival-time-series/#comments</comments>
		<pubDate>Fri, 20 Jan 2012 01:46:07 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[arrival time]]></category>
		<category><![CDATA[astronomy]]></category>
		<category><![CDATA[bayesian method]]></category>
		<category><![CDATA[binning]]></category>
		<category><![CDATA[droplet]]></category>
		<category><![CDATA[frequentist methods]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[Measurement]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[pulsars]]></category>
		<category><![CDATA[pulses]]></category>
		<category><![CDATA[time domain]]></category>
		<category><![CDATA[time series data]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/01/19/sines-steps-and-droplets-semiparametric-bayesian-modeling-of-arrival-time-series/</guid>
		<description><![CDATA[I describe ongoing work developing Bayesian methods for flexible modeling of arrival time series data without binning, aiming to improve detection and measurement of X-ray and gamma-ray pulsars, and of pulses in gamma-ray bursts. The methods use parametric and semiparametric Poisson point process models for the event rate, and by design have close connections to [...]]]></description>
			<content:encoded><![CDATA[<p>I describe ongoing work developing Bayesian methods for flexible modeling of arrival time series data without binning, aiming to improve detection and measurement of X-ray and gamma-ray pulsars, and of pulses in gamma-ray bursts. The methods use parametric and semiparametric Poisson point process models for the event rate, and by design have close connections to conventional frequentist methods currently used in time-domain astronomy.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/01/19/sines-steps-and-droplets-semiparametric-bayesian-modeling-of-arrival-time-series/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Multi-Chroic Feed-Horn Coupled TES Polarimeters</title>
		<link>http://voxcharta.org/2012/01/19/multi-chroic-feed-horn-coupled-tes-pola
