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<channel>
	<title>Vox Charta &#187; Solar and Stellar</title>
	<atom:link href="http://voxcharta.org/category/astro-ph/solar-stellar-astro-ph/feed/" rel="self" type="application/rss+xml" />
	<link>http://voxcharta.org</link>
	<description></description>
	<lastBuildDate>Tue, 22 May 2012 18:03:08 +0000</lastBuildDate>
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			<item>
		<title>A Public Set of Synthetic Spectra from Expanding Atmospheres for X-Ray Novae. I. Solar Abundances</title>
		<link>http://voxcharta.org/2012/05/21/a-public-set-of-synthetic-spectra-from-expanding-atmospheres-for-x-ray-novae-i-solar-abundances/</link>
		<comments>http://voxcharta.org/2012/05/21/a-public-set-of-synthetic-spectra-from-expanding-atmospheres-for-x-ray-novae-i-solar-abundances/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:53:03 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorption line]]></category>
		<category><![CDATA[abundance]]></category>
		<category><![CDATA[atmosphere]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[eff]]></category>
		<category><![CDATA[example application]]></category>
		<category><![CDATA[grating]]></category>
		<category><![CDATA[line profile]]></category>
		<category><![CDATA[mass loss]]></category>
		<category><![CDATA[model parameter]]></category>
		<category><![CDATA[SGR]]></category>
		<category><![CDATA[solar set]]></category>
		<category><![CDATA[static model]]></category>
		<category><![CDATA[stellar atmosphere]]></category>
		<category><![CDATA[synthetic spectra]]></category>
		<category><![CDATA[van rossum]]></category>
		<category><![CDATA[white dwarf]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/a-public-set-of-synthetic-spectra-from-expanding-atmospheres-for-x-ray-novae-i-solar-abundances/</guid>
		<description><![CDATA[X-ray grating observations have revealed great detail in the spectra of Novae in the Super Soft Source (SSS) phase. Notable features in the SSS spectra are blue-shifted absorption lines, P-Cygni line profiles, and the absence of strong ionization edges, all of which are indicators of an expanding atmosphere.   We present, and make publicly [...]]]></description>
			<content:encoded><![CDATA[<p>X-ray grating observations have revealed great detail in the spectra of Novae in the Super Soft Source (SSS) phase. Notable features in the SSS spectra are blue-shifted absorption lines, P-Cygni line profiles, and the absence of strong ionization edges, all of which are indicators of an expanding atmosphere.   We present, and make publicly available, a set of 672 wind-type (WT) synthetic spectra, obtained from the expanding NLTE SSS models introduced in Van Rossum 2010 with the PHOENIX stellar atmosphere code. The set presented in this paper is limited to solar abundances with the aim to focus on the basic model parameters and their effect on the spectra, providing the basis upon which abundance effects can be studied using a much bigger non-solar set in the next paper in this series.   We fit the WT spectra to the five grating spectra taken in the SSS phase of nova V4743 Sgr 2003 as an example application of the WT models. Within the limits of solar abundances we demonstrate that the following parameters are constrained by the data (in order of decreasing accuracy): column density N_H, bolometric luminosity L_bol, effective temperature T_eff, white dwarf radius R, wind asymptotic velocity v_inf, and the mass-loss rate M_dot. The models are also sensitive to the assumed white dwarf mass M_wd but the effect on the spectra can largely be compensated by the other model parameters. The WT spectra with solar abundances fit the data better than abundance optimized hydro-static models.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/a-public-set-of-synthetic-spectra-from-expanding-atmospheres-for-x-ray-novae-i-solar-abundances/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Infrared observations of the recurrent nova T Pyxidis: ancient dust basks in the warm glow of the 2011 outburst</title>
		<link>http://voxcharta.org/2012/05/21/infrared-observations-of-the-recurrent-nova-t-pyxidis-ancient-dust-basks-in-the-warm-glow-of-the-2011-outburst/</link>
		<comments>http://voxcharta.org/2012/05/21/infrared-observations-of-the-recurrent-nova-t-pyxidis-ancient-dust-basks-in-the-warm-glow-of-the-2011-outburst/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:47:20 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accumulation]]></category>
		<category><![CDATA[herschel]]></category>
		<category><![CDATA[infrared observation]]></category>
		<category><![CDATA[infrared photometry]]></category>
		<category><![CDATA[interstellar dust]]></category>
		<category><![CDATA[nebulosity]]></category>
		<category><![CDATA[outburst]]></category>
		<category><![CDATA[pyx]]></category>
		<category><![CDATA[recurrent nova]]></category>
		<category><![CDATA[space observatory]]></category>
		<category><![CDATA[space telescope]]></category>
		<category><![CDATA[warm glow]]></category>

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

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/nitrogen-line-spectroscopy-in-o-stars-iii-the-earliest-o-stars/</guid>
		<description><![CDATA[This is the third paper in a series aiming at the analysis of nitrogen abundances in O-type stars, to enable further constraints on the early evolution of massive stars. We provide first theoretical predictions for the NIV4058/NIII4640 emission line ratio in dependence of various parameters, and confront them with results from the analysis of a [...]]]></description>
			<content:encoded><![CDATA[<p>This is the third paper in a series aiming at the analysis of nitrogen abundances in O-type stars, to enable further constraints on the early evolution of massive stars. We provide first theoretical predictions for the NIV4058/NIII4640 emission line ratio in dependence of various parameters, and confront them with results from the analysis of a sample of early LMC/SMC O-stars. Stellar and wind parameters are determined by line profile fitting of H/He/N lines, exploiting the helium and nitrogen ionization balance. Corresponding synthetic spectra are calculated using the NLTE atmospheric code FASTWIND. Though there is a monotonic relationship between the emission line ratio and Teff, all other parameters being equal, theoretical predictions indicate additional dependencies, most notably, on the nitrogen abundance. These basic predictions are confirmed by results from atmospheric code CMFGEN. The effective temperatures for the earliest O-stars, inferred from the nitrogen ionization balance, are partly considerably hotter than indicated by previous studies. Consistent with earlier results, effective temperatures increase from supergiants to dwarfs for all spectral types in the LMC. The relation between observed NIV4058/NIII4640 emission line ratio and Teff, for a given luminosity class, turned out to be quite monotonic for our sample stars, and fairly consistent with our model predictions. The scatter within a spectral sub-type is mainly produced by abundance effects. Our findings suggest that the Walborn et al. (2002) classification scheme is able to provide a meaningful relation between spectral type and Teff, provided that it is possible to discriminate for the luminosity class. This might be difficult to achieve in low-Z environments such as the SMC, owing to rather low wind-strengths. According to our predictions, the major bias of the classification scheme is due to nitrogen content.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/nitrogen-line-spectroscopy-in-o-stars-iii-the-earliest-o-stars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Sunspot rotation, filament, and flare: The event on 2000 February 10</title>
		<link>http://voxcharta.org/2012/05/21/sunspot-rotation-filament-and-flare-the-event-on-2000-february-10/</link>
		<comments>http://voxcharta.org/2012/05/21/sunspot-rotation-filament-and-flare-the-event-on-2000-february-10/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:44:28 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[c class]]></category>
		<category><![CDATA[chromosphere]]></category>
		<category><![CDATA[class flare]]></category>
		<category><![CDATA[corona]]></category>
		<category><![CDATA[filament channel]]></category>
		<category><![CDATA[filament eruption]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[magnetic flux]]></category>
		<category><![CDATA[mass ejection]]></category>
		<category><![CDATA[photosphere]]></category>
		<category><![CDATA[polarity]]></category>
		<category><![CDATA[rapid increase]]></category>
		<category><![CDATA[region ar]]></category>
		<category><![CDATA[rotation rate]]></category>
		<category><![CDATA[sunspot]]></category>
		<category><![CDATA[twenty four hours]]></category>
		<category><![CDATA[umbrae]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/sunspot-rotation-filament-and-flare-the-event-on-2000-february-10/</guid>
		<description><![CDATA[We find that a sunspot with positive polarity had an obvious counter-clockwise rotation and resulted in the formation and eruption of an inverse S-shaped filament in NOAA active region (AR) 08858 from 2000 February 9 to 10. The sunspot had two umbrae which rotated around each other by 195 degrees within about twenty-four hours. The [...]]]></description>
			<content:encoded><![CDATA[<p>We find that a sunspot with positive polarity had an obvious counter-clockwise rotation and resulted in the formation and eruption of an inverse S-shaped filament in NOAA active region (AR) 08858 from 2000 February 9 to 10. The sunspot had two umbrae which rotated around each other by 195 degrees within about twenty-four hours. The average rotation rate was nearly 8 degrees per hour. The fastest rotation in the photosphere took place during 14:00UT to 22:01UT on February 9, with the rotation rate of nearly 16 degrees per hour. The fastest rotation in the chromosphere and the corona took place during 15:28UT to 19:00UT on February 9, with the rotation rate of nearly 20 degrees per hour. Interestingly, the rapid increase of the positive magnetic flux just occurred during the fastest rotation of the rotating sunspot, the bright loop-shaped structure and the filament. During the sunspot rotation, the inverse S-shaped filament gradually formed in the EUV filament channel. The filament experienced two eruptions. In the first eruption, the filament rose quickly and then the filament loops carrying the cool and the hot material were seen to spiral into the sunspot counterclockwise. About ten minutes later, the filament became active and finally erupted. The filament eruption was accompanied with a C-class flare and a halo coronal mass ejection (CME). These results provide evidence that sunspot rotation plays an important role in the formation and eruption of the sigmoidal active-region filament.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/sunspot-rotation-filament-and-flare-the-event-on-2000-february-10/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The role of radiative losses in the late evolution of pulse-heated coronal loops/strands</title>
		<link>http://voxcharta.org/2012/05/21/the-role-of-radiative-losses-in-the-late-evolution-of-pulse-heated-coronal-loopsstrands/</link>
		<comments>http://voxcharta.org/2012/05/21/the-role-of-radiative-losses-in-the-late-evolution-of-pulse-heated-coronal-loopsstrands/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:43:43 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[curve]]></category>
		<category><![CDATA[curves]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[hydrodynamic simulation]]></category>
		<category><![CDATA[plasma]]></category>
		<category><![CDATA[plasma density]]></category>
		<category><![CDATA[radiative loss]]></category>
		<category><![CDATA[rate increase]]></category>
		<category><![CDATA[slope]]></category>
		<category><![CDATA[solar corona]]></category>
		<category><![CDATA[spectral line]]></category>
		<category><![CDATA[spectral model]]></category>
		<category><![CDATA[strand]]></category>
		<category><![CDATA[temperature]]></category>
		<category><![CDATA[temperature dependence]]></category>
		<category><![CDATA[threshold value]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/the-role-of-radiative-losses-in-the-late-evolution-of-pulse-heated-coronal-loopsstrands/</guid>
		<description><![CDATA[Radiative losses from optically thin plasma are an important ingredient for modeling plasma confined in the solar corona. Spectral models are continuously updated to include the emission from more spectral lines, with significant effects on radiative losses, especially around 1 MK. We investigate the effect of changing the radiative losses temperature dependence due to upgrading [...]]]></description>
			<content:encoded><![CDATA[<p>Radiative losses from optically thin plasma are an important ingredient for modeling plasma confined in the solar corona. Spectral models are continuously updated to include the emission from more spectral lines, with significant effects on radiative losses, especially around 1 MK. We investigate the effect of changing the radiative losses temperature dependence due to upgrading of spectral codes on predictions obtained from modeling plasma confined in the solar corona. The hydrodynamic simulation of a pulse-heated loop strand is revisited comparing results using an old and a recent radiative losses function. We find significant changes in the plasma evolution during the late phases of plasma cooling: when the recent radiative loss curve is used, the plasma cooling rate increases significantly when temperatures reach 1-2 MK. Such more rapid cooling occurs when the plasma density is larger than a threshold value, and therefore in impulsive heating models that cause the loop plasma to become overdense. The fast cooling has the effect of steepening the slope of the emission measure distribution of coronal plasmas with temperature at temperatures lower than ~2 MK. The effects of changes in the radiative losses curves can be important for modeling the late phases of the evolution of pulse-heated coronal loops, and, more in general, of thermally unstable optically thin plasmas.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/the-role-of-radiative-losses-in-the-late-evolution-of-pulse-heated-coronal-loopsstrands/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Proton, Electron, and Ion Heating in the Fast Solar Wind from Nonlinear Coupling Between Alfvenic and Fast-Mode Turbulence</title>
		<link>http://voxcharta.org/2012/05/21/proton-electron-and-ion-heating-in-the-fast-solar-wind-from-nonlinear-coupling-between-alfvenic-and-fast-mode-turbulence/</link>
		<comments>http://voxcharta.org/2012/05/21/proton-electron-and-ion-heating-in-the-fast-solar-wind-from-nonlinear-coupling-between-alfvenic-and-fast-mode-turbulence/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:42:32 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[advection]]></category>
		<category><![CDATA[coulomb]]></category>
		<category><![CDATA[diffusion equation]]></category>
		<category><![CDATA[energy input]]></category>
		<category><![CDATA[energy transfer]]></category>
		<category><![CDATA[frequency waves]]></category>
		<category><![CDATA[heavy ion]]></category>
		<category><![CDATA[interplanetary space]]></category>
		<category><![CDATA[ion cyclotron resonance]]></category>
		<category><![CDATA[ion populations]]></category>
		<category><![CDATA[mhd turbulence]]></category>
		<category><![CDATA[particle species]]></category>
		<category><![CDATA[proton electron]]></category>
		<category><![CDATA[situ measurement]]></category>
		<category><![CDATA[slow mode]]></category>
		<category><![CDATA[solar corona]]></category>
		<category><![CDATA[solar wind]]></category>
		<category><![CDATA[thermal equilibrium]]></category>
		<category><![CDATA[velocity distribution]]></category>
		<category><![CDATA[wave power]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/proton-electron-and-ion-heating-in-the-fast-solar-wind-from-nonlinear-coupling-between-alfvenic-and-fast-mode-turbulence/</guid>
		<description><![CDATA[In the parts of the solar corona and solar wind that experience the fewest Coulomb collisions, the component proton, electron, and heavy ion populations are not in thermal equilibrium with one another. Observed differences in temperatures, outflow speeds, and velocity distribution anisotropies are useful constraints on proposed explanations for how the plasma is heated and [...]]]></description>
			<content:encoded><![CDATA[<p>In the parts of the solar corona and solar wind that experience the fewest Coulomb collisions, the component proton, electron, and heavy ion populations are not in thermal equilibrium with one another. Observed differences in temperatures, outflow speeds, and velocity distribution anisotropies are useful constraints on proposed explanations for how the plasma is heated and accelerated. This paper presents new predictions of the rates of collisionless heating for each particle species, in which the energy input is assumed to come from magnetohydrodynamic (MHD) turbulence. We first created an empirical description of the radial evolution of Alfven, fast-mode, and slow-mode MHD waves. This model provides the total wave power in each mode as a function of distance along an expanding flux tube in the high-speed solar wind. Next we solved a set of cascade advection-diffusion equations that give the time-steady wavenumber spectra at each distance. An approximate term for nonlinear coupling between the Alfven and fast-mode fluctuations is included. For reasonable choices of the parameters, our model contains enough energy transfer from the fast mode to the Alfven mode to excite the high-frequency ion cyclotron resonance. This resonance is efficient at heating protons and other ions in the direction perpendicular to the background magnetic field, and our model predicts heating rates for these species that agree well with both spectroscopic and in situ measurements. Nonetheless, the high-frequency waves comprise only a small part of the total Alfvenic fluctuation spectrum, which remains highly two-dimensional as is observed in interplanetary space.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/proton-electron-and-ion-heating-in-the-fast-solar-wind-from-nonlinear-coupling-between-alfvenic-and-fast-mode-turbulence/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Constraining mean-field models of the nuclear matter equation of state at low densities [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/constraining-mean-field-models-of-the-nuclear-matter-equation-of-state-at-low-densities-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/constraining-mean-field-models-of-the-nuclear-matter-equation-of-state-at-low-densities-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:37:05 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astrophysical applications]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[coupling]]></category>
		<category><![CDATA[degrees of freedom]]></category>
		<category><![CDATA[dense nuclear matter]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[dependent properties]]></category>
		<category><![CDATA[equation of state]]></category>
		<category><![CDATA[expansion]]></category>
		<category><![CDATA[field model]]></category>
		<category><![CDATA[light nuclei]]></category>
		<category><![CDATA[low density]]></category>
		<category><![CDATA[meson]]></category>
		<category><![CDATA[neutron]]></category>
		<category><![CDATA[nucleon]]></category>
		<category><![CDATA[phase shift]]></category>
		<category><![CDATA[relativistic effects]]></category>
		<category><![CDATA[saturation]]></category>
		<category><![CDATA[veos]]></category>
		<category><![CDATA[virial equation of state]]></category>

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

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/neutrinos-and-the-stars-replacement/</guid>
		<description><![CDATA[The role of neutrinos in stars is introduced for students with little prior astrophysical exposure. We begin with neutrinos as an energy-loss channel in ordinary stars and conversely, how stars provide information on neutrinos and possible other low-mass particles. Next we turn to the Sun as a measurable source of neutrinos and other particles. Finally [...]]]></description>
			<content:encoded><![CDATA[<p>The role of neutrinos in stars is introduced for students with little prior astrophysical exposure. We begin with neutrinos as an energy-loss channel in ordinary stars and conversely, how stars provide information on neutrinos and possible other low-mass particles. Next we turn to the Sun as a measurable source of neutrinos and other particles. Finally we discuss supernova (SN) neutrinos, the SN 1987A measurements, and the quest for a high-statistics neutrino measurement from the next nearby SN. We also touch on the subject of neutrino oscillations in the high-density SN context.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/neutrinos-and-the-stars-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>SN 2006oz: rise of a super-luminous supernova observed by the SDSS-II SN Survey [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/sn-2006oz-rise-of-a-super-luminous-supernova-observed-by-the-sdss-ii-sn-survey-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/sn-2006oz-rise-of-a-super-luminous-supernova-observed-by-the-sdss-ii-sn-survey-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:35:50 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absolute magnitude]]></category>
		<category><![CDATA[absolute peak]]></category>
		<category><![CDATA[body functions]]></category>
		<category><![CDATA[common property]]></category>
		<category><![CDATA[deep imaging]]></category>
		<category><![CDATA[explosion models]]></category>
		<category><![CDATA[host galaxy]]></category>
		<category><![CDATA[light curve]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[magnetar]]></category>
		<category><![CDATA[maximum light]]></category>
		<category><![CDATA[optical spectrum]]></category>
		<category><![CDATA[peak luminosity]]></category>
		<category><![CDATA[photosphere]]></category>
		<category><![CDATA[radioactive decay]]></category>
		<category><![CDATA[rest frame]]></category>
		<category><![CDATA[rise time]]></category>
		<category><![CDATA[sdss]]></category>
		<category><![CDATA[starburst galaxy]]></category>
		<category><![CDATA[u band]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/sn-2006oz-rise-of-a-super-luminous-supernova-observed-by-the-sdss-ii-sn-survey-replacement/</guid>
		<description><![CDATA[We study SN 2006oz, a newly-recognized member of the class of H-poor, super-luminous supernovae. We present multi-color light curves from the SDSS-II SN Survey, that cover the rise time, as well as an optical spectrum that shows that the explosion occurred at z~0.376. We fitted black body functions to estimate the temperature and radius evolution [...]]]></description>
			<content:encoded><![CDATA[<p>We study SN 2006oz, a newly-recognized member of the class of H-poor, super-luminous supernovae. We present multi-color light curves from the SDSS-II SN Survey, that cover the rise time, as well as an optical spectrum that shows that the explosion occurred at z~0.376. We fitted black body functions to estimate the temperature and radius evolution of the photosphere and used the parametrized code SYNOW to model the spectrum. We constructed a bolometric light curve and compared it with explosion models. The very early light curves show a dip in the g- and r-bands and a possible initial cooling phase in the u-band before rising to maximum light. The bolometric light curve shows a precursor plateau with a duration of 6-10 days in the rest-frame. A lower limit of M_u &lt; -21.5 can be placed on the absolute peak luminosity of the SN, while the rise time is constrained to be at least 29 days. During our observations, the emitting sphere doubled its radius to 2&#215;10^15 cm, while the temperature remained hot at 15000 K. As for other similar SNe, the spectrum is best modeled with elements including O II and Mg II, while we tentatively suggest that Fe III might be present. We suggest that the precursor plateau might be related to a recombination wave in a circumstellar medium (CSM) and discuss whether this is a common property of all similar explosions. The subsequent rise can be equally well described by input from a magnetar or by ejecta-CSM interaction, but the models are not well constrained owing to the lack of post-maximum observations, and CSM interaction has difficulties accounting for the precursor plateau self-consistently. Radioactive decay is less likely to be the mechanism that powers the luminosity. The host galaxy, detected in deep imaging with the 10 m GTC, is a moderately young and star-forming, but not a starburst, galaxy. It has an absolute magnitude of M_g = -16.9.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/sn-2006oz-rise-of-a-super-luminous-supernova-observed-by-the-sdss-ii-sn-survey-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The survival of nuclei in jets associated with core-collapse supernovae [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/the-survival-of-nuclei-in-jets-associated-with-core-collapse-supernovae-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/the-survival-of-nuclei-in-jets-associated-with-core-collapse-supernovae-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:33:30 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cocoon]]></category>
		<category><![CDATA[core collapse supernovae]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[jet parameters]]></category>
		<category><![CDATA[jets]]></category>
		<category><![CDATA[launch]]></category>
		<category><![CDATA[lorentz]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[multi messenger]]></category>
		<category><![CDATA[nickel]]></category>
		<category><![CDATA[nuclei]]></category>
		<category><![CDATA[propagation]]></category>
		<category><![CDATA[signal]]></category>
		<category><![CDATA[spallation]]></category>
		<category><![CDATA[stellar material]]></category>
		<category><![CDATA[survival]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/the-survival-of-nuclei-in-jets-associated-with-core-collapse-supernovae-replacement/</guid>
		<description><![CDATA[Heavy nuclei such as nickel-56 are synthesized in a wide range of core-collapse supernovae (CCSN), including energetic supernovae associated with gamma-ray bursts (GRBs). Recent studies suggest that jet-like outflows are a common feature of CCSN. These outflows may entrain synthesized nuclei at launch or during propagation, and provide interesting multi-messenger signals including heavy ultra-high energy [...]]]></description>
			<content:encoded><![CDATA[<p>Heavy nuclei such as nickel-56 are synthesized in a wide range of core-collapse supernovae (CCSN), including energetic supernovae associated with gamma-ray bursts (GRBs). Recent studies suggest that jet-like outflows are a common feature of CCSN. These outflows may entrain synthesized nuclei at launch or during propagation, and provide interesting multi-messenger signals including heavy ultra-high energy cosmic rays. Here, we investigate the destruction processes of nuclei during crossing from the stellar material into the jet material via a cocoon, and during propagation after being successfully loaded into the jet. We find that nuclei can survive for a range of jet parameters because collisional cooling is faster than spallation. While canonical high-luminosity GRB jets may contain nuclei, magnetic dominated models or low-luminosity jets with small bulk Lorentz factors are more favorable for having a more significant heavy nuclei component.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/the-survival-of-nuclei-in-jets-associated-with-core-collapse-supernovae-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Asteroseismology of the open clusters NGC 6791, NGC 6811, and NGC 6819 from nineteen months of Kepler photometry</title>
		<link>http://voxcharta.org/2012/05/20/asteroseismology-of-the-open-clusters-ngc-6791-ngc-6811-and-ngc-6819-from-nineteen-months-of-kepler-photometry/</link>
		<comments>http://voxcharta.org/2012/05/20/asteroseismology-of-the-open-clusters-ngc-6791-ngc-6811-and-ngc-6819-from-nineteen-months-of-kepler-photometry/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:45:06 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[19 months]]></category>
		<category><![CDATA[binaries]]></category>
		<category><![CDATA[blue straggler]]></category>
		<category><![CDATA[clump stars]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[dnu]]></category>
		<category><![CDATA[eff]]></category>
		<category><![CDATA[epsilon]]></category>
		<category><![CDATA[giant branch stars]]></category>
		<category><![CDATA[kepler]]></category>
		<category><![CDATA[linewidth]]></category>
		<category><![CDATA[nasa]]></category>
		<category><![CDATA[open cluster]]></category>
		<category><![CDATA[photometric data]]></category>
		<category><![CDATA[photometry]]></category>
		<category><![CDATA[red giant]]></category>
		<category><![CDATA[separations]]></category>
		<category><![CDATA[space telescope]]></category>
		<category><![CDATA[stellar classification]]></category>
		<category><![CDATA[stellar population]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/asteroseismology-of-the-open-clusters-ngc-6791-ngc-6811-and-ngc-6819-from-nineteen-months-of-kepler-photometry/</guid>
		<description><![CDATA[We studied 115 red giants in the three open clusters NGC 6791, NGC 6811, and NGC 6819, based on photometric data covering more than 19 months with NASA&#8217;s Kepler space telescope. We present the asteroseismic diagrams of the asymptotic parameters \Delta\nu, \delta\nu_01, \delta\nu_02 and \epsilon. When the stellar populations from the clusters are compared, we [...]]]></description>
			<content:encoded><![CDATA[<p>We studied 115 red giants in the three open clusters NGC 6791, NGC 6811, and NGC 6819, based on photometric data covering more than 19 months with NASA&#8217;s Kepler space telescope. We present the asteroseismic diagrams of the asymptotic parameters \Delta\nu, \delta\nu_01, \delta\nu_02 and \epsilon. When the stellar populations from the clusters are compared, we see evidence for a difference in mass of the red giant branch stars, and possibly a difference in structure of the red clump stars, from the small separations \delta\nu_01 and \delta\nu_02. Ensemble \&#8217;echelle diagrams and lower limits to the linewidth of l = 0 modes as a function of Dnu of the clusters NGC 6791 and NGC 6819 are also shown, together with a correlation between the l = 0 ridge width and T_eff. Lastly, we distinguish between red giant branch and red clump stars through the measurement of the period spacing of mixed modes in 53 stars among all the three clusters to verify the stellar classification from the color-magnitude diagram. These seismic results also allow us to identify a number of potentially interesting stars including evolved blue stragglers and binaries, as well as stars in late He-core burning phases.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/asteroseismology-of-the-open-clusters-ngc-6791-ngc-6811-and-ngc-6819-from-nineteen-months-of-kepler-photometry/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Does the Sun work as a nuclear fusion amplifier of planetary tidal forcing? A proposal for a physical mechanism based on the mass-luminosity relation</title>
		<link>http://voxcharta.org/2012/05/20/does-the-sun-work-as-a-nuclear-fusion-amplifier-of-planetary-tidal-forcing-a-proposal-for-a-physical-mechanism-based-on-the-mass-luminosity-relation/</link>
		<comments>http://voxcharta.org/2012/05/20/does-the-sun-work-as-a-nuclear-fusion-amplifier-of-planetary-tidal-forcing-a-proposal-for-a-physical-mechanism-based-on-the-mass-luminosity-relation/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:40:16 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[amplification factor]]></category>
		<category><![CDATA[classical physics]]></category>
		<category><![CDATA[conversion factor]]></category>
		<category><![CDATA[dynamo processes]]></category>
		<category><![CDATA[fusion rate]]></category>
		<category><![CDATA[gravitational potential energy]]></category>
		<category><![CDATA[magnification factor]]></category>
		<category><![CDATA[mercury and venus]]></category>
		<category><![CDATA[nuclear fusion]]></category>
		<category><![CDATA[orbital period]]></category>
		<category><![CDATA[physical mechanism]]></category>
		<category><![CDATA[solar activity]]></category>
		<category><![CDATA[solar core]]></category>
		<category><![CDATA[solar cycle]]></category>
		<category><![CDATA[solar dynamo]]></category>
		<category><![CDATA[solar luminosity]]></category>
		<category><![CDATA[sun work]]></category>
		<category><![CDATA[sunspot number]]></category>
		<category><![CDATA[tidal energy]]></category>
		<category><![CDATA[venus earth]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/does-the-sun-work-as-a-nuclear-fusion-amplifier-of-planetary-tidal-forcing-a-proposal-for-a-physical-mechanism-based-on-the-mass-luminosity-relation/</guid>
		<description><![CDATA[Empirical evidences show that planetary tides may influence solar activity: 1) the 11-yr Schwabe sunspot number cycle is constrained between the spring tidal period of Jupiter and Saturn, 9.93 yr, and the tidal orbital period of Jupiter, 11.86 yr, and a model based on these cycles reconstructs solar dynamics at multiple time ; 2) a [...]]]></description>
			<content:encoded><![CDATA[<p>Empirical evidences show that planetary tides may influence solar activity: 1) the 11-yr Schwabe sunspot number cycle is constrained between the spring tidal period of Jupiter and Saturn, 9.93 yr, and the tidal orbital period of Jupiter, 11.86 yr, and a model based on these cycles reconstructs solar dynamics at multiple time ; 2) a measure of the alignment of Venus, Earth and Jupiter reveals quasi 11.07-yr cycles well correlated to the 11-year Schwabe solar cycles; 3) there exists a 11.08 yr cyclical recurrence in the solar jerk-shock vector, which is induced mostly by Mercury and Venus. However, Newtonian classical physics fails to explain the phenomenon. Only by means of a significant nuclear fusion amplification of the tidal gravitational potential energy released in the Sun, may planetary tides produce irradiance output oscillations with a sufficient magnitude to influence solar dynamo processes. Here we use an adaptation of the well-known mass-luminosity relation to calculate a conversion factor between the solar luminosity and the potential gravitational power associated to the mass lost by nuclear fusion: the average estimated amplification factor is A=4,250,000. We use this magnification factor to evaluate the theoretical luminosity oscillations that planetary tides may potentially stimulate inside the solar core by making its nuclear fusion rate oscillate. By converting the power related to this energy into solar irradiance units at 1 AU we find that the tidal oscillations may be able to theoretically induce an oscillating luminosity increase from 0.05-0.65 $W/m^{2}$ to 0.25-1.63 $W/m^{2}$, which is a range compatible with the ACRIM satellite observed total solar irradiance fluctuations. In conclusion, the Sun, by means of its nuclear active core, may be working as a great amplifier of the small planetary tidal energy dissipated in it.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/does-the-sun-work-as-a-nuclear-fusion-amplifier-of-planetary-tidal-forcing-a-proposal-for-a-physical-mechanism-based-on-the-mass-luminosity-relation/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Age and helium content of the open cluster NGC 6791 from multiple eclipsing binary members. II. age dependencies and new insights</title>
		<link>http://voxcharta.org/2012/05/20/age-and-helium-content-of-the-open-cluster-ngc-6791-from-multiple-eclipsing-binary-members-ii-age-dependencies-and-new-insights/</link>
		<comments>http://voxcharta.org/2012/05/20/age-and-helium-content-of-the-open-cluster-ngc-6791-from-multiple-eclipsing-binary-members-ii-age-dependencies-and-new-insights/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:39:36 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accuracy and precision]]></category>
		<category><![CDATA[binary star]]></category>
		<category><![CDATA[cluster ngc]]></category>
		<category><![CDATA[cluster stars]]></category>
		<category><![CDATA[consistency check]]></category>
		<category><![CDATA[eclipsing binary]]></category>
		<category><![CDATA[gyr]]></category>
		<category><![CDATA[helium content]]></category>
		<category><![CDATA[helium mass]]></category>
		<category><![CDATA[mass fraction]]></category>
		<category><![CDATA[mass loss]]></category>
		<category><![CDATA[model comparison]]></category>
		<category><![CDATA[new insights]]></category>
		<category><![CDATA[observational constraints]]></category>
		<category><![CDATA[open cluster]]></category>
		<category><![CDATA[stellar model]]></category>
		<category><![CDATA[stellar structure]]></category>
		<category><![CDATA[stellar system]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/age-and-helium-content-of-the-open-cluster-ngc-6791-from-multiple-eclipsing-binary-members-ii-age-dependencies-and-new-insights/</guid>
		<description><![CDATA[Models of stellar structure and evolution can be constrained by measuring accurate parameters of detached eclipsing binaries in open clusters. Multiple binary stars provide the means to determine helium abundances in these old stellar systems, and in turn, to improve estimates of their age. In the first paper of this series, we demonstrated how measurements [...]]]></description>
			<content:encoded><![CDATA[<p>Models of stellar structure and evolution can be constrained by measuring accurate parameters of detached eclipsing binaries in open clusters. Multiple binary stars provide the means to determine helium abundances in these old stellar systems, and in turn, to improve estimates of their age. In the first paper of this series, we demonstrated how measurements of multiple eclipsing binaries in the old open cluster NGC6791 sets tighter constraints on the properties of stellar models than has previously been possible, thereby potentially improving both the accuracy and precision of the cluster age. Here we add additional constraints and perform an extensive model comparison to determine the best estimates of the cluster age and helium content, employing as many observational constraints as possible. We improve our photometry and correct empirically for differential reddening effects. We then perform an extensive comparison of the CMDs and eclipsing binary measurements to Victoria and DSEP isochrones to estimate cluster parameters. We also reanalyse a spectrum of the star 2-17 to improve [Fe/H] constraints. We find a best estimate of the age of ~8.3 Gyr while demonstrating that remaining age uncertainty is dominated by uncertainties in the CNO abundances. The helium mass fraction is well constrained at Y = 0.30 \pm 0.01 resulting in dY/dZ ~ 1.4 assuming that such a relation exists. During the analysis we firmly identify blue straggler stars, including the star 2-17, and find indications for the presence of their evolved counterparts. Our analysis supports the RGB mass-loss found from asteroseismology and we determine precisely the absolute mass of stars on the lower RGB, 1.15\pm0.02Msun. This will be an important consistency check for the detailed asteroseismology of cluster stars.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/age-and-helium-content-of-the-open-cluster-ngc-6791-from-multiple-eclipsing-binary-members-ii-age-dependencies-and-new-insights/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Protostellar Accretion Flows Destabilized by Magnetic Flux Redistribution</title>
		<link>http://voxcharta.org/2012/05/20/protostellar-accretion-flows-destabilized-by-magnetic-flux-redistribution/</link>
		<comments>http://voxcharta.org/2012/05/20/protostellar-accretion-flows-destabilized-by-magnetic-flux-redistribution/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:38:57 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[advection]]></category>
		<category><![CDATA[central star]]></category>
		<category><![CDATA[collapse]]></category>
		<category><![CDATA[dense core]]></category>
		<category><![CDATA[density region]]></category>
		<category><![CDATA[field strength]]></category>
		<category><![CDATA[heart of the problem]]></category>
		<category><![CDATA[inflow]]></category>
		<category><![CDATA[interchange instability]]></category>
		<category><![CDATA[latter phase]]></category>
		<category><![CDATA[low density]]></category>
		<category><![CDATA[magnetic flux]]></category>
		<category><![CDATA[molecular cloud]]></category>
		<category><![CDATA[orders of magnitude]]></category>
		<category><![CDATA[radii]]></category>
		<category><![CDATA[realistic level]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[stellar field]]></category>
		<category><![CDATA[three dimensions]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/protostellar-accretion-flows-destabilized-by-magnetic-flux-redistribution/</guid>
		<description><![CDATA[Magnetic flux redistribution lies at the heart of the problem of star formation in dense cores of molecular clouds that are magnetized to a realistic level. If all of the magnetic flux of a typical core were to be dragged into the central star, the stellar field strength would be orders of magnitude higher than [...]]]></description>
			<content:encoded><![CDATA[<p>Magnetic flux redistribution lies at the heart of the problem of star formation in dense cores of molecular clouds that are magnetized to a realistic level. If all of the magnetic flux of a typical core were to be dragged into the central star, the stellar field strength would be orders of magnitude higher than the observed values. This well-known &#8220;magnetic flux problem&#8221; can in principle be resolved through non-ideal MHD effects. Two dimensional (axisymmetric) calculations have shown that ambipolar diffusion, in particular, can transport magnetic flux outward relative to matter, allowing material to enter the central object without dragging the field lines along. We show through simulations that such axisymmetric protostellar accretion flows are unstable in three dimensions to magnetic interchange instability in the azimuthal direction. The instability is driven by the magnetic flux redistributed from the matter that enters the central object. It typically starts to develop during the transition from the prestellar phase of star formation to the protostellar mass accretion phase. In the latter phase, the magnetic flux is transported outward mainly through advection, by strongly magnetized low-density regions that expand against the collapsing inflow. The tussle between the gravity-driven infall and magnetically driven expansion leads to a filamentary inner accretion flow, more disordered than previously pictured. The efficient outward transport of magnetic flux by advection lowers the field strength at small radii, making the magnetic braking less efficient and the formation of rotationally supported disks easier in principle. However, we find no evidence for such disks in any of our rotating collapse simulations. We conclude that the inner protostellar accretion flow is shaped to a large extent by this magnetic interchange instability. How disks form in such an environment is unclear.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/protostellar-accretion-flows-destabilized-by-magnetic-flux-redistribution/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Three-Dimensional Explosion Geometry of Stripped-Envelope Core-Collapse Supernovae. I. Spectropolarimetric Observations</title>
		<link>http://voxcharta.org/2012/05/20/three-dimensional-explosion-geometry-of-stripped-envelope-core-collapse-supernovae-i-spectropolarimetric-observations/</link>
		<comments>http://voxcharta.org/2012/05/20/three-dimensional-explosion-geometry-of-stripped-envelope-core-collapse-supernovae-i-spectropolarimetric-observations/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:38:33 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[core collapse supernovae]]></category>
		<category><![CDATA[dispersion]]></category>
		<category><![CDATA[distributions]]></category>
		<category><![CDATA[ejecta]]></category>
		<category><![CDATA[explosion]]></category>
		<category><![CDATA[polarization]]></category>
		<category><![CDATA[SNe]]></category>
		<category><![CDATA[three dimensional geometry]]></category>
		<category><![CDATA[type ic]]></category>
		<category><![CDATA[wavelength]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/three-dimensional-explosion-geometry-of-stripped-envelope-core-collapse-supernovae-i-spectropolarimetric-observations/</guid>
		<description><![CDATA[We study the multi-dimensional geometry of supernova (SN) explosions by means of spectropolarimetric observations of stripped-envelope SNe, i.e., SNe without a H-rich layer. We perform spectropolarimetric observations of 2 stripped-envelope SNe, the Type Ib SN 2009jf and the Type Ic SN 2009mi. Both objects show non-zero polarization at the wavelength of the strong lines. They [...]]]></description>
			<content:encoded><![CDATA[<p>We study the multi-dimensional geometry of supernova (SN) explosions by means of spectropolarimetric observations of stripped-envelope SNe, i.e., SNe without a H-rich layer. We perform spectropolarimetric observations of 2 stripped-envelope SNe, the Type Ib SN 2009jf and the Type Ic SN 2009mi. Both objects show non-zero polarization at the wavelength of the strong lines. They also show a loop in the Stokes Q-U diagram, which indicates a non-axisymmetric, three-dimensional ion distribution in the ejecta. We show that five out of six stripped-envelope SNe which have been observed spectropolarimetrically so far show such a loop. This implies that a three-dimensional geometry is common in stripped-envelope SNe. We find that stronger lines tend to show higher polarization. This effect is not related to the geometry, and must be corrected to compare the polarization of different lines or different objects. Even after the correction, however, there remains a dispersion of polarization degree among different objects. Such a dispersion might be caused by three-dimensional clumpy ion distributions viewed from different directions.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/three-dimensional-explosion-geometry-of-stripped-envelope-core-collapse-supernovae-i-spectropolarimetric-observations/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Two distinct halo populations in the solar neighborhood. IV. Lithium abundances</title>
		<link>http://voxcharta.org/2012/05/20/two-distinct-halo-populations-in-the-solar-neighborhood-iv-lithium-abundances/</link>
		<comments>http://voxcharta.org/2012/05/20/two-distinct-halo-populations-in-the-solar-neighborhood-iv-lithium-abundances/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:38:22 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abundance]]></category>
		<category><![CDATA[bang nucleosynthesis]]></category>
		<category><![CDATA[big bang]]></category>
		<category><![CDATA[constants]]></category>
		<category><![CDATA[environmental effect]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[interpolating]]></category>
		<category><![CDATA[lii]]></category>
		<category><![CDATA[linear dependence]]></category>
		<category><![CDATA[Lithium]]></category>
		<category><![CDATA[main sequence]]></category>
		<category><![CDATA[model atmosphere]]></category>
		<category><![CDATA[resolution spectra]]></category>
		<category><![CDATA[solar neighborhood]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[wmap]]></category>
		<category><![CDATA[yonsei]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/two-distinct-halo-populations-in-the-solar-neighborhood-iv-lithium-abundances/</guid>
		<description><![CDATA[We investigate if there is a difference in the lithium abundances of stars belonging to two halo populations of F and G main-sequence stars previously found to differ in [alpha/Fe] for the metallicity range -1.4 &#60; [Fe/H] &#60; -0.7. Li abundances are derived from the LiI 6707.8 A line measured in high-resolution spectra using MARCS [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate if there is a difference in the lithium abundances of stars belonging to two halo populations of F and G main-sequence stars previously found to differ in [alpha/Fe] for the metallicity range -1.4 &lt; [Fe/H] &lt; -0.7. Li abundances are derived from the LiI 6707.8 A line measured in high-resolution spectra using MARCS model atmospheres. Furthermore, masses of the stars are determined from the logTeff &#8211; logg diagram by interpolating between Yonsei-Yale evolutionary tracks. There is no significant systematic difference in the lithium abundances of high- and low-alpha halo stars. For the large majority of stars with masses 0.7 &lt; M/M_sun &lt; 0.9 and heavy-element mass fractions 0.001 &lt; Z &lt; 0.006, the Li abundance is well fitted by a relation A(Li) = a0 + a1 M + a2 Z + a3 M Z, where a0, a1, a2, and a3 are constants. Extrapolating this relation to Z = 0 leads to a Li abundance close to the primordial value predicted from standard Big Bang nucleosynthesis calculations and the WMAP baryon density. The relation, however, does not apply to stars with [Fe/H] &lt; -1.5. We suggest that metal-rich halo stars were formed with a Li abundance close to the primordial value, and that lithium in their atmospheres has been depleted in time with an approximately linear dependence on stellar mass and Z. The lack of a systematic difference in the Li abundances of high- and low-alpha stars indicates that an environmental effect is not important for the destruction of lithium.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/two-distinct-halo-populations-in-the-solar-neighborhood-iv-lithium-abundances/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>The role of OH in the chemical evolution of protoplanetary disks. I. The comet-forming region [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/the-role-of-oh-in-the-chemical-evolution-of-protoplanetary-disks-i-the-comet-forming-region-replacement/</link>
		<comments>http://voxcharta.org/2012/05/20/the-role-of-oh-in-the-chemical-evolution-of-protoplanetary-disks-i-the-comet-forming-region-replacement/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:34:42 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accurate treatment]]></category>
		<category><![CDATA[chemical composition]]></category>
		<category><![CDATA[chemical evolution]]></category>
		<category><![CDATA[chemical model]]></category>
		<category><![CDATA[chemical species]]></category>
		<category><![CDATA[cm 3]]></category>
		<category><![CDATA[comet formation]]></category>
		<category><![CDATA[complex organic molecules]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[desorption]]></category>
		<category><![CDATA[ects]]></category>
		<category><![CDATA[grain size distribution]]></category>
		<category><![CDATA[model yields]]></category>
		<category><![CDATA[photo processes]]></category>
		<category><![CDATA[photon flux]]></category>
		<category><![CDATA[protoplanetary disk]]></category>
		<category><![CDATA[rate equations]]></category>
		<category><![CDATA[timescale]]></category>
		<category><![CDATA[water ice]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/the-role-of-oh-in-the-chemical-evolution-of-protoplanetary-disks-i-the-comet-forming-region-replacement/</guid>
		<description><![CDATA[Context. Time dependent gas-grain chemistry can help us understand the layered structure of species deposited onto the surface of grains during the lifetime of a protoplanetary disk. The history of trapping important quantities of carbon- and oxygen-bearing molecules onto the grains is of special significance for the formation of more complex (organic) molecules on the [...]]]></description>
			<content:encoded><![CDATA[<p>Context. Time dependent gas-grain chemistry can help us understand the layered structure of species deposited onto the surface of grains during the lifetime of a protoplanetary disk. The history of trapping important quantities of carbon- and oxygen-bearing molecules onto the grains is of special significance for the formation of more complex (organic) molecules on the surface of grains. Aims. Among other processes, cosmic ray-induced UV photo-processes can lead to the efficient formation of OH. Using a more accurate treatment of cosmic ray-gas interactions for disks, we obtain an increased cosmic ray-induced UV photon flux of 3.8&#215;10^5 photons cm^-2s^-1 for a cosmic-ray ionization rate of H2 value of 5&#215;10^-17 s^-1 (compared to previous estimates of 10^4 photons cm^-2s^-1 based on ISM dust properties). We explore the role of the enhanced OH abundance on the gas-grain chemistry in the midplane of the disk at 10 AU, which is a plausible location for comet formation. We focus on studying the formation/destruction pathways and timescales of the dominant chemical species. Methods. We solve the chemical rate equations based on a gas-grain chemical network and correcting for the enhanced cosmic rayinduced UV field. This field is estimated from an appropriate treatment of dust properties in a protoplanetary disk, as opposed to previous estimates that assume an ISM-like grain size distribution. We also explore the chemical eff?ects of photo-desorption of water ice into OH+H. Results. Near the end of the disk&#8217;s lifetime our chemical model yields H2O, CO, CO2 and CH4 ice abundances at 10 AU (consistent with a midplane density of 10^10 cm^-3 and a temperature of 20 K) that are compatible with measurements of the chemical composition of cometary bodies for a [C/O] ratio of 0.16. Such comparison provides constraints on the physical conditions in which comets were formed.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/the-role-of-oh-in-the-chemical-evolution-of-protoplanetary-disks-i-the-comet-forming-region-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Was The Sun Born In A Massive Cluster? [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/was-the-sun-born-in-a-massive-cluster-replacement/</link>
		<comments>http://voxcharta.org/2012/05/20/was-the-sun-born-in-a-massive-cluster-replacement/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:34:18 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cluster]]></category>
		<category><![CDATA[cluster mass]]></category>
		<category><![CDATA[cluster properties]]></category>
		<category><![CDATA[contamination]]></category>
		<category><![CDATA[contrary]]></category>
		<category><![CDATA[cross section]]></category>
		<category><![CDATA[disruption]]></category>
		<category><![CDATA[eccentric orbit]]></category>
		<category><![CDATA[lifetime]]></category>
		<category><![CDATA[massive cluster]]></category>
		<category><![CDATA[myr]]></category>
		<category><![CDATA[nearby supernova]]></category>
		<category><![CDATA[outer planet]]></category>
		<category><![CDATA[outer solar system]]></category>
		<category><![CDATA[probability]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[star cluster]]></category>
		<category><![CDATA[stellar encounters]]></category>
		<category><![CDATA[surface density]]></category>
		<category><![CDATA[velocity distribution]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/was-the-sun-born-in-a-massive-cluster-replacement/</guid>
		<description><![CDATA[A number of authors have argued that the Sun must have been born in a cluster of no more than about 1000 stars, on the basis that, in a larger cluster, close encounters between the Sun and other stars would have truncated the outer Solar System or excited the outer planets into eccentric orbits. However, [...]]]></description>
			<content:encoded><![CDATA[<p>A number of authors have argued that the Sun must have been born in a cluster of no more than about 1000 stars, on the basis that, in a larger cluster, close encounters between the Sun and other stars would have truncated the outer Solar System or excited the outer planets into eccentric orbits. However, this dynamical limit is in tension with meteoritic evidence that the Solar System was exposed to a nearby supernova during or shortly after its formation; a 1000-star cluster is much too small for supernova contamination to be likely. In this paper we revisit the dynamical limit in the light of improved observations of the properties of young clusters. We use a series of scattering simulations to measure the velocity-dependent cross-section for disruption of the outer Solar System by stellar encounters, and use this cross-section to compute the probability of a disruptive encounter as a function of birth cluster properties. We find that, contrary to prior work, the probability of disruption is small regardless of the cluster mass, and that it actually decreases rather than increases with cluster mass. Our results differ from prior work for three main reasons: (1) unlike in most previous work, we compute a velocity-dependent cross section and properly integrate over the cluster mass-dependent velocity distribution of incoming stars; (2) we adopt realistically-short cluster lifetimes of a few crossing times, rather than assuming lifetimes of 10 to 100 Myr; and (3) following recent observations, we adopt a mass-independent surface density for embedded clusters, rather than a mass-independent radius as assumed many earlier papers. Our results remove the tension between the dynamical limit and the meteoritic evidence, and suggest that the Sun was born in a massive cluster.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/was-the-sun-born-in-a-massive-cluster-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>High-resolution X-ray spectroscopy reveals the special nature of Wolf-Rayet star winds [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/high-resolution-x-ray-spectroscopy-reveals-the-special-nature-of-wolf-rayet-star-winds-replacement/</link>
		<comments>http://voxcharta.org/2012/05/20/high-resolution-x-ray-spectroscopy-reveals-the-special-nature-of-wolf-rayet-star-winds-replacement/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:33:52 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration]]></category>
		<category><![CDATA[clump]]></category>
		<category><![CDATA[fe line]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[hot x]]></category>
		<category><![CDATA[newton telescope]]></category>
		<category><![CDATA[o star]]></category>
		<category><![CDATA[photosphere]]></category>
		<category><![CDATA[porous structure]]></category>
		<category><![CDATA[rams]]></category>
		<category><![CDATA[shock]]></category>
		<category><![CDATA[spectral analysis]]></category>
		<category><![CDATA[spectral signature]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[star winds]]></category>
		<category><![CDATA[stellar radii]]></category>
		<category><![CDATA[stellar wind]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xmm newton]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/high-resolution-x-ray-spectroscopy-reveals-the-special-nature-of-wolf-rayet-star-winds-replacement/</guid>
		<description><![CDATA[We present the first high-resolution X-ray spectrum of a putatively single Wolf-Rayet star. 400 ks observations of WR 6 by the XMM-Newton-telescope resulted in a superb quality high-resolution X-ray spectrum. Spectral analysis reveals that the X-rays originate far out in the stellar wind, more than 30 stellar radii from the photosphere, and thus outside the [...]]]></description>
			<content:encoded><![CDATA[<p>We present the first high-resolution X-ray spectrum of a putatively single Wolf-Rayet star. 400 ks observations of WR 6 by the XMM-Newton-telescope resulted in a superb quality high-resolution X-ray spectrum. Spectral analysis reveals that the X-rays originate far out in the stellar wind, more than 30 stellar radii from the photosphere, and thus outside the wind acceleration zone where the line-driving instability could create shocks. The X-ray emitting plasma reaches temperatures up to 50\,MK, and is embedded within the un-shocked, &#8220;cool&#8221; stellar wind as revealed by characteristic spectral signatures. We detect a fluorescent Fe line at approx 6.4 keV. The presence of fluorescence is consistent with a two-component medium, where the cool wind is permeated with the hot X-ray emitting plasma. The wind must have a very porous structure to allow the observed amount of X-rays to escape. We find that neither the line-driving instability nor any alternative binary scenario can explain the data. We suggest a scenario where X-rays are produced when the fast wind rams into slow &#8220;sticky clumps&#8221; that resist acceleration. Our new data show that the X-rays in single WR-star are generated by some special mechanism different from the one operating in the O-star winds.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/high-resolution-x-ray-spectroscopy-reveals-the-special-nature-of-wolf-rayet-star-winds-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Particle-in-cell simulations of particle energization from low Mach number fast mode shocks [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/particle-in-cell-simulations-of-particle-energization-from-low-mach-number-fast-mode-shocks-replacement-2/</link>
		<comments>http://voxcharta.org/2012/05/20/particle-in-cell-simulations-of-particle-energization-from-low-mach-number-fast-mode-shocks-replacement-2/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:33:26 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[boundary method]]></category>
		<category><![CDATA[cell pic]]></category>
		<category><![CDATA[cell simulation]]></category>
		<category><![CDATA[dimensional particle]]></category>
		<category><![CDATA[electron distribution]]></category>
		<category><![CDATA[electron mass]]></category>
		<category><![CDATA[initial generation]]></category>
		<category><![CDATA[mach number]]></category>
		<category><![CDATA[magnetic pressure]]></category>
		<category><![CDATA[microphysics]]></category>
		<category><![CDATA[moving wall]]></category>
		<category><![CDATA[pic simulations]]></category>
		<category><![CDATA[plasma turbulence]]></category>
		<category><![CDATA[shock formation]]></category>
		<category><![CDATA[shock speed]]></category>
		<category><![CDATA[shock transition]]></category>
		<category><![CDATA[simulation result]]></category>
		<category><![CDATA[simulation time]]></category>
		<category><![CDATA[solar flare]]></category>
		<category><![CDATA[transition region]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/particle-in-cell-simulations-of-particle-energization-from-low-mach-number-fast-mode-shocks-replacement-2/</guid>
		<description><![CDATA[Astrophysical shocks are often studied in the high Mach number limit but weakly compressive fast shocks can occur in magnetic reconnection outflows and are considered to be a site of particle energization in solar flares. Here we study the microphysics of such perpendicular, low Mach number collisionless shocks using two-dimensional particle-in-cell (PIC) simulations with a [...]]]></description>
			<content:encoded><![CDATA[<p>Astrophysical shocks are often studied in the high Mach number limit but weakly compressive fast shocks can occur in magnetic reconnection outflows and are considered to be a site of particle energization in solar flares. Here we study the microphysics of such perpendicular, low Mach number collisionless shocks using two-dimensional particle-in-cell (PIC) simulations with a reduced ion/electron mass ratio and employ a moving wall boundary method for initial generation of the shock. This moving wall method allows for more control of the shock speed, smaller simulation box sizes, and longer simulation times than the commonly used fixed wall, reflection method of shock formation. Our results, which are independent of the shock formation method, reveal the prevalence shock drift acceleration (SDA) of both electron and ions in a purely perpendicular shock with Alfv\&#8217;en Mach number $M_A=6.8$ and ratio of thermal to magnetic pressure $\beta=8$. We determine the respective minimum energies required for electrons and ions to incur SDA. We derive a theoretical electron distribution via SDA that compares to the simulation results. We also show that a modified two-stream instability due to the incoming and reflecting ions in the shock transition region acts as the mechanism to generate collisionless plasma turbulence that sustains the shock.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/particle-in-cell-simulations-of-particle-energization-from-low-mach-number-fast-mode-shocks-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Supernova 1998S at 14 years Postmortem: Continuing CSM Interaction and Dust Formation [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/supernova-1998s-at-14-years-postmortem-continuing-csm-interaction-and-dust-formation-replacement/</link>
		<comments>http://voxcharta.org/2012/05/20/supernova-1998s-at-14-years-postmortem-continuing-csm-interaction-and-dust-formation-replacement/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:32:58 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[centroid]]></category>
		<category><![CDATA[circumstellar material]]></category>
		<category><![CDATA[clump]]></category>
		<category><![CDATA[dust extinction]]></category>
		<category><![CDATA[dust formation]]></category>
		<category><![CDATA[emission features]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[large binocular telescope]]></category>
		<category><![CDATA[last decade]]></category>
		<category><![CDATA[optical spectrum]]></category>
		<category><![CDATA[oxygen profiles]]></category>
		<category><![CDATA[radial distribution]]></category>
		<category><![CDATA[red supergiant]]></category>
		<category><![CDATA[red wing]]></category>
		<category><![CDATA[SNe]]></category>
		<category><![CDATA[strong wind]]></category>
		<category><![CDATA[type iin]]></category>
		<category><![CDATA[wavelength dependence]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/supernova-1998s-at-14-years-postmortem-continuing-csm-interaction-and-dust-formation-replacement/</guid>
		<description><![CDATA[We report late-time spectroscopic observations of the Type IIn SN 1998S, taken 14 years after explosion using the Large Binocular Telescope. The optical spectrum exhibits broad emission features of [O I], [O II], [O III], H-alpha, H-beta, and [Fe II]. The last decade of evolution has exhibited a strengthening of the oxygen transitions, evidence that [...]]]></description>
			<content:encoded><![CDATA[<p>We report late-time spectroscopic observations of the Type IIn SN 1998S, taken 14 years after explosion using the Large Binocular Telescope. The optical spectrum exhibits broad emission features of [O I], [O II], [O III], H-alpha, H-beta, and [Fe II]. The last decade of evolution has exhibited a strengthening of the oxygen transitions, evidence that the late-time emission is powered by increasingly metal-rich SN ejecta crossing the reverse shock. The H-alpha luminosity requires that SN 1998S is still interacting with dense circumstellar material (CSM), probably produced by the strong wind of a red supergiant progenitor at least ~1000 years before explosion. The emission lines exhibit asymmetric blueshifted profiles, which implies that the receding hemisphere of the SN is obscured by dust. The [O III] line, in particular, exhibits a complete suppression of its red wing. This could be the result of the expected wavelength dependence for dust extinction or a smaller radial distribution for [O III]. In the latter case, the red wing of [O III] could be absorbed by core dust, while both the blue and red wings are absorbed by dust within the cool dense shell between the forward and reverse shocks; this interpretation could explain why late-time [O III] emission from SNe is often weaker than models predict. The [O I] line exhibits double-peaked structure on top of the broader underlying profile, possibly due to emission from individual clumps of ejecta or ring-like structures of metal-rich debris. The centroids of the peaks are blueshifted and lack a red counterpart. However, an archival spectrum obtained on day 1093 exhibits a third, redshifted peak, which we suspect has become extinguished by dust that formed over the last decade. This implies that the &#8220;missing&#8221; red components of multi-peaked oxygen profiles observed in other SNe might be obscured by varying degrees of dust extinction.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/supernova-1998s-at-14-years-postmortem-continuing-csm-interaction-and-dust-formation-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Constraining the Circumbinary Envelope of Z CMa via imaging polarimetry</title>
		<link>http://voxcharta.org/2012/05/17/constraining-the-circumbinary-envelope-of-z-cma-via-imaging-polarimetry/</link>
		<comments>http://voxcharta.org/2012/05/17/constraining-the-circumbinary-envelope-of-z-cma-via-imaging-polarimetry/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:55:53 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[beam of light]]></category>
		<category><![CDATA[binary system]]></category>
		<category><![CDATA[cma]]></category>
		<category><![CDATA[cocoon]]></category>
		<category><![CDATA[dual beam]]></category>
		<category><![CDATA[herbig]]></category>
		<category><![CDATA[jets]]></category>
		<category><![CDATA[low density]]></category>
		<category><![CDATA[micro jet]]></category>
		<category><![CDATA[optical wavelength]]></category>
		<category><![CDATA[ori]]></category>
		<category><![CDATA[outburst]]></category>
		<category><![CDATA[pencil]]></category>
		<category><![CDATA[polarimeter]]></category>
		<category><![CDATA[polarimetry]]></category>
		<category><![CDATA[polarization angle]]></category>
		<category><![CDATA[preferred orientation]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[variability]]></category>
		<category><![CDATA[variable geometry]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/constraining-the-circumbinary-envelope-of-z-cma-via-imaging-polarimetry/</guid>
		<description><![CDATA[Z CMa is a complex binary system, composed of a Herbig Be and an FU Ori star. The Herbig star is surrounded by a dust cocoon of variable geometry, and the whole system is surrounded by an infalling envelope. Previous spectropolarimetric observations have reported a preferred orientation of the polarization angle, perpendicular to the direction [...]]]></description>
			<content:encoded><![CDATA[<p>Z CMa is a complex binary system, composed of a Herbig Be and an FU Ori star. The Herbig star is surrounded by a dust cocoon of variable geometry, and the whole system is surrounded by an infalling envelope. Previous spectropolarimetric observations have reported a preferred orientation of the polarization angle, perpendicular to the direction of a large, parsec-sized jet associated with the Herbig star. The variability in the amount of polarized light has been associated to changes in the geometry of the dust cocoon that surrounds the Herbig star. We aim to constrain the properties of Z CMa by means of imaging polarimetry at optical wavelengths. Using ExPo, a dual-beam imaging polarimeter which operates at optical wavelengths, we have obtained imaging (linear) polarimetric data of Z CMa. Our observations were secured during the return to quiescence after the 2008 outburst. We detect three polarized features over Z CMa. Two of these features are related to the two jets reported in this system: the large jet associated to the Herbig star, and the micro-jet associated to the FU Ori star. Our results suggest that the micro-jet extends to a distance ten times larger than reported in previous studies. The third feature suggests the presence of a hole in the dust cocoon that surrounds the Herbig star of this system. According to our simulations, this hole can produce a pencil beam of light that we see scattered off the low-density envelope surrounding the system.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/constraining-the-circumbinary-envelope-of-z-cma-via-imaging-polarimetry/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Acceleration of Energetic Particles through Reconnection of Weakly Stochastic Magnetic Field</title>
		<link>http://voxcharta.org/2012/05/17/acceleration-of-energetic-particles-through-reconnection-of-weakly-stochastic-magnetic-field/</link>
		<comments>http://voxcharta.org/2012/05/17/acceleration-of-energetic-particles-through-reconnection-of-weakly-stochastic-magnetic-field/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:53:16 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[driven turbulence]]></category>
		<category><![CDATA[energetic particle]]></category>
		<category><![CDATA[intensity]]></category>
		<category><![CDATA[large scale]]></category>
		<category><![CDATA[latter case]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetic reconnection]]></category>
		<category><![CDATA[motion]]></category>
		<category><![CDATA[new evidence]]></category>
		<category><![CDATA[particle acceleration]]></category>
		<category><![CDATA[pino]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[successful testing]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/acceleration-of-energetic-particles-through-reconnection-of-weakly-stochastic-magnetic-field/</guid>
		<description><![CDATA[Astrophysical media are turbulent and therefore reconnection should be treated in the presence of pre-existing turbulence. We consider the model of fast magnetic reconnection in Lazarian &#38; Vishniac (1999) which predicts that the rate of reconnection is controlled by the intensity and the injection scale of turbulent motions. We provide new evidence of successful testing [...]]]></description>
			<content:encoded><![CDATA[<p>Astrophysical media are turbulent and therefore reconnection should be treated in the presence of pre-existing turbulence. We consider the model of fast magnetic reconnection in Lazarian &amp; Vishniac (1999) which predicts that the rate of reconnection is controlled by the intensity and the injection scale of turbulent motions. We provide new evidence of successful testing of the model and argue that the model presents a generic set up for astrophysical reconnection events. We study particle acceleration that takes place in volumes of driven turbulence as well turbulent volumes in the presence of large scale reconnection. We show that in the latter case the acceleration is of the first order Fermi type thus supporting the model of acceleration proposed in Gouveia dal Pino &amp; Lazarian (2005).</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/acceleration-of-energetic-particles-through-reconnection-of-weakly-stochastic-magnetic-field/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Constraints on model atmospheres from complex asteroseismology of the \beta Cephei stars</title>
		<link>http://voxcharta.org/2012/05/17/constraints-on-model-atmospheres-from-complex-asteroseismology-of-the-beta-cephei-stars/</link>
		<comments>http://voxcharta.org/2012/05/17/constraints-on-model-atmospheres-from-complex-asteroseismology-of-the-beta-cephei-stars/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:52:56 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[beta]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[gamma]]></category>
		<category><![CDATA[kurucz]]></category>
		<category><![CDATA[model atmosphere]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[peg]]></category>

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

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/studying-the-hybrid-pulsator-12-lacertae-mode-identification-and-complex-seismic-modelling/</guid>
		<description><![CDATA[We present identification of the mode degree, l, for all observed frequencies of 12 Lac and results of seismic modelling which consists in fitting simultaneously the centroid mode frequencies and the corresponding values of the complex nonadiabatic f-parameter. Effects of chemical composition, opacities, core overshooting and non-LTE atmospheres were taken into account.
]]></description>
			<content:encoded><![CDATA[<p>We present identification of the mode degree, l, for all observed frequencies of 12 Lac and results of seismic modelling which consists in fitting simultaneously the centroid mode frequencies and the corresponding values of the complex nonadiabatic f-parameter. Effects of chemical composition, opacities, core overshooting and non-LTE atmospheres were taken into account.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/studying-the-hybrid-pulsator-12-lacertae-mode-identification-and-complex-seismic-modelling/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A solar tornado observed by AIA/SDO: Rotational flow and evolution of magnetic helicity in a prominence and cavity</title>
		<link>http://voxcharta.org/2012/05/17/a-solar-tornado-observed-by-aiasdo-rotational-flow-and-evolution-of-magnetic-helicity-in-a-prominence-and-cavity/</link>
		<comments>http://voxcharta.org/2012/05/17/a-solar-tornado-observed-by-aiasdo-rotational-flow-and-evolution-of-magnetic-helicity-in-a-prominence-and-cavity/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:51:13 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[aia]]></category>
		<category><![CDATA[blob]]></category>
		<category><![CDATA[cavity]]></category>
		<category><![CDATA[coherent rotation]]></category>
		<category><![CDATA[complexity]]></category>
		<category><![CDATA[cyclone]]></category>
		<category><![CDATA[fades]]></category>
		<category><![CDATA[helical structure]]></category>
		<category><![CDATA[helium lines]]></category>
		<category><![CDATA[helix axis]]></category>
		<category><![CDATA[hydrogen]]></category>
		<category><![CDATA[line of sight]]></category>
		<category><![CDATA[magnetic helicity]]></category>
		<category><![CDATA[narrow loop]]></category>
		<category><![CDATA[observatory]]></category>
		<category><![CDATA[prominence]]></category>
		<category><![CDATA[sdo]]></category>
		<category><![CDATA[streaks]]></category>
		<category><![CDATA[telescopes]]></category>
		<category><![CDATA[tornado]]></category>

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

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/recent-observations-of-plasma-and-alfvenic-wave-energy-injection-at-the-base-of-the-fast-solar-wind/</guid>
		<description><![CDATA[We take stock of recent observations that identify the episodic plasma heating and injection of Alfvenic energy at the base of fast solar wind (in coronal holes). The plasma heating is associated with the occurrence of chromospheric spicules that leave the lower solar atmosphere at speeds of order 100km/s, the hotter coronal counterpart of the [...]]]></description>
			<content:encoded><![CDATA[<p>We take stock of recent observations that identify the episodic plasma heating and injection of Alfvenic energy at the base of fast solar wind (in coronal holes). The plasma heating is associated with the occurrence of chromospheric spicules that leave the lower solar atmosphere at speeds of order 100km/s, the hotter coronal counterpart of the spicule emits radiation characteristic of root heating that rapidly reaches temperatures of the order of 1MK. Furthermore, the same spicules and their coronal counterparts (&#8220;Propagating Coronal Disturbances&#8221;; PCD) exhibit large amplitude, high speed, Alfvenic (transverse) motion of sufficient energy content to accelerate the material to high speeds. We propose that these (disjointed) heating and accelerating components form a one-two punch to supply, and then accelerate, the fast solar wind. We consider some compositional constraints on this concept, extend the premise to the slow solar wind, and identify future avenues of exploration.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/recent-observations-of-plasma-and-alfvenic-wave-energy-injection-at-the-base-of-the-fast-solar-wind/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The nature of dust in compact Galactic planetary nebulae from Spitzer spectra</title>
		<link>http://voxcharta.org/2012/05/17/the-nature-of-dust-in-compact-galactic-planetary-nebulae-from-spitzer-spectra/</link>
		<comments>http://voxcharta.org/2012/05/17/the-nature-of-dust-in-compact-galactic-planetary-nebulae-from-spitzer-spectra/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:49:48 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[continuum]]></category>
		<category><![CDATA[dust grains]]></category>
		<category><![CDATA[enhancement]]></category>
		<category><![CDATA[equilibrium]]></category>
		<category><![CDATA[evolutionary sequence]]></category>
		<category><![CDATA[galactic center]]></category>
		<category><![CDATA[galactic disk]]></category>
		<category><![CDATA[galactic planetary nebulae]]></category>
		<category><![CDATA[group properties]]></category>
		<category><![CDATA[interstellar environments]]></category>
		<category><![CDATA[irs]]></category>
		<category><![CDATA[magellanic cloud]]></category>
		<category><![CDATA[mcd]]></category>
		<category><![CDATA[pne]]></category>
		<category><![CDATA[point symmetry]]></category>
		<category><![CDATA[radiation field]]></category>
		<category><![CDATA[solid state]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[state feature]]></category>
		<category><![CDATA[symmetric point]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/the-nature-of-dust-in-compact-galactic-planetary-nebulae-from-spitzer-spectra/</guid>
		<description><![CDATA[We present the Spitzer/IRS spectra of 157 compact Galactic PNe. These young PNe provide insight on the effects of dust in early post-AGB evolution, before much of the dust is altered or destroyed by the hardening stellar radiation field. Most of the selected targets have PN-type IRS spectra, while a few turned out to be [...]]]></description>
			<content:encoded><![CDATA[<p>We present the Spitzer/IRS spectra of 157 compact Galactic PNe. These young PNe provide insight on the effects of dust in early post-AGB evolution, before much of the dust is altered or destroyed by the hardening stellar radiation field. Most of the selected targets have PN-type IRS spectra, while a few turned out to be misclassified stars. We inspected the group properties of the PN spectra and classified them based on the different dust classes (featureless, carbon-rich dust; oxygen-rich dust; mixed-chemistry dust) and subclasses (aromatic and aliphatic; crystalline and amorphous). All PNe are characterized by dust continuum and more than 80% of the sample shows solid state features above the continuum, in contrast with the Magellanic Cloud sample where only ~40% of the entire sample displays solid state features; this is an indication of the strong link between dust properties and metallicity. The Galactic PNe that show solid state features are almost equally divided among the CRD, ORD, and MCD. We analyzed dust properties together with other PN properties and found that (i) there is an enhancement of MCD PNe toward the Galactic center; (ii) CRD PNe could be seen as defining an evolutionary sequence, contrary to the ORD and MCD PNe; (iii) C- and O-rich grains retain different equilibrium temperatures, as expected from models; (iv) ORD PNe are highly asymmetric and CRD PNe highly symmetric; point-symmetry is statistically more common in MCD. We find that the Galactic Disk sample does not include MCD PNe, and the other dust classes are differently populated from high to low metallicity environments. The MCPNe seem to attain higher dust temperatures at similar evolutionary stages, in agreement with the observational findings of smaller dust grains in low metallicity interstellar environments.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/the-nature-of-dust-in-compact-galactic-planetary-nebulae-from-spitzer-spectra/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The evolution of the X-ray emission of HH 2 &#8211; Investigating heating and cooling processes</title>
		<link>http://voxcharta.org/2012/05/17/the-evolution-of-the-x-ray-emission-of-hh-2-investigating-heating-and-cooling-processes/</link>
		<comments>http://voxcharta.org/2012/05/17/the-evolution-of-the-x-ray-emission-of-hh-2-investigating-heating-and-cooling-processes/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:45:57 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[alignment]]></category>
		<category><![CDATA[bipolar]]></category>
		<category><![CDATA[bipolar outflows]]></category>
		<category><![CDATA[chandra observation]]></category>
		<category><![CDATA[constancy]]></category>
		<category><![CDATA[heating and cooling]]></category>
		<category><![CDATA[herbig haro]]></category>
		<category><![CDATA[optical emission]]></category>
		<category><![CDATA[proper motion]]></category>
		<category><![CDATA[radiative loss]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[stellar object]]></category>
		<category><![CDATA[temperature gas]]></category>
		<category><![CDATA[thermal conduction]]></category>
		<category><![CDATA[time scale]]></category>
		<category><![CDATA[wavelength]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/the-evolution-of-the-x-ray-emission-of-hh-2-investigating-heating-and-cooling-processes/</guid>
		<description><![CDATA[Young stellar objects often drive powerful bipolar outflows which evolve on time scales of a few years. An increasing number of these outflows has been detected in X-rays implying the existence of million degree plasma almost co-spatial with the lower temperature gas observed in the optical and near-IR. The details of the heating and cooling [...]]]></description>
			<content:encoded><![CDATA[<p>Young stellar objects often drive powerful bipolar outflows which evolve on time scales of a few years. An increasing number of these outflows has been detected in X-rays implying the existence of million degree plasma almost co-spatial with the lower temperature gas observed in the optical and near-IR. The details of the heating and cooling processes of the X-ray emitting part of these so-called Herbig-Haro objects are still ambiguous, e.g., whether the cooling is dominated by expansion, radiation or thermal conduction.   We present a second epoch Chandra observation of the first X-ray detected Herbig-Haro object (HH 2) and derive the proper-motion of the X-ray emitting plasma and its cooling history. We argue that the most likely explanation for the constancy of the X-ray luminosity, the alignment with the optical emission and the proper-motion is that the cooling is dominated by radiative losses leading to cooling times exceeding a decade. We explain that a strong shock caused by fast material ramming into slower gas in front of it about ten years ago can explain the X-ray emission while being compatible with the available multi-wavelength data of HH 2.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/the-evolution-of-the-x-ray-emission-of-hh-2-investigating-heating-and-cooling-processes/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A new Skyrme interaction with improved spin-isospin properties [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/17/a-new-skyrme-interaction-with-improved-spin-isospin-properties-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/17/a-new-skyrme-interaction-with-improved-spin-isospin-properties-cross-listing/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:43:50 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accurate description]]></category>
		<category><![CDATA[charge exchange]]></category>
		<category><![CDATA[core collapse]]></category>
		<category><![CDATA[decay]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[earth]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[finite nuclei]]></category>
		<category><![CDATA[improvements]]></category>
		<category><![CDATA[interaction]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[physical processes]]></category>
		<category><![CDATA[resonance]]></category>
		<category><![CDATA[saturation]]></category>
		<category><![CDATA[spin isospin]]></category>
		<category><![CDATA[stars in the universe]]></category>
		<category><![CDATA[stellar nucleosynthesis]]></category>
		<category><![CDATA[stringent test]]></category>
		<category><![CDATA[supernova explosion]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/a-new-skyrme-interaction-with-improved-spin-isospin-properties-cross-listing/</guid>
		<description><![CDATA[A correct determination of the spin-isospin properties of the nuclear effective interaction should lead, among other improvements, to an accurate description of the Gamow-Teller Resonances (GTR). These nuclear excitations impact on a variety of physical processes: from the response in charge-exchange reactions of nuclei naturally present in the Earth, to the description of the stellar [...]]]></description>
			<content:encoded><![CDATA[<p>A correct determination of the spin-isospin properties of the nuclear effective interaction should lead, among other improvements, to an accurate description of the Gamow-Teller Resonances (GTR). These nuclear excitations impact on a variety of physical processes: from the response in charge-exchange reactions of nuclei naturally present in the Earth, to the description of the stellar nucleosynthesis, and of the pre-supernova explosion core-collapse evolution of massive stars in the Universe. A reliable description of the GTR provides also stringent tests for neutrinoless double-$\beta$ decay calculations. We present a new Skyrme interaction as accurate as previous forces in the description of finite nuclei and of uniform matter properties around saturation density, and that accurately accounts for the GTR in ${}^{48}$Ca, ${}^{90}$Zr and ${}^{208}$Pb.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/a-new-skyrme-interaction-with-improved-spin-isospin-properties-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
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		<title>Angular Momentum Transport and Variability in Boundary Layers of Accretion Disks Driven by Global Acoustic Modes</title>
		<link>http://voxcharta.org/2012/05/17/angular-momentum-transport-and-variability-in-boundary-layers-of-accretion-disks-driven-by-global-acoustic-modes/</link>
		<comments>http://voxcharta.org/2012/05/17/angular-momentum-transport-and-variability-in-boundary-layers-of-accretion-disks-driven-by-global-acoustic-modes/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:40:34 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion disk]]></category>
		<category><![CDATA[acoustic mode]]></category>
		<category><![CDATA[amplifier]]></category>
		<category><![CDATA[angular momentum transport]]></category>
		<category><![CDATA[boundary layer]]></category>
		<category><![CDATA[compact object]]></category>
		<category><![CDATA[dissipation]]></category>
		<category><![CDATA[equatorial plane]]></category>
		<category><![CDATA[global mode]]></category>
		<category><![CDATA[inner edge]]></category>
		<category><![CDATA[mass transport]]></category>
		<category><![CDATA[orbital period]]></category>
		<category><![CDATA[orbital velocity]]></category>
		<category><![CDATA[pattern speed]]></category>
		<category><![CDATA[resonance]]></category>
		<category><![CDATA[rotational velocity]]></category>
		<category><![CDATA[shock]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[variability]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/angular-momentum-transport-and-variability-in-boundary-layers-of-accretion-disks-driven-by-global-acoustic-modes/</guid>
		<description><![CDATA[Disk accretion onto a weakly magnetized central object, e.g. a star, is inevitably accompanied by the formation of a boundary layer near the surface, in which matter slows down from the highly supersonic orbital velocity of the disk to the rotational velocity of the star. We perform high resolution 2D hydrodynamical simulations in the equatorial [...]]]></description>
			<content:encoded><![CDATA[<p>Disk accretion onto a weakly magnetized central object, e.g. a star, is inevitably accompanied by the formation of a boundary layer near the surface, in which matter slows down from the highly supersonic orbital velocity of the disk to the rotational velocity of the star. We perform high resolution 2D hydrodynamical simulations in the equatorial plane of an astrophysical boundary layer with the goal of exploring the dynamics of non-axisymmetric structures that form there. We generically find that the supersonic shear in the boundary layer excites non-axisymmetric quasi-stationary acoustic modes that are trapped between the surface of the star and a Lindblad resonance in the disk. These modes rotate in a prograde fashion, are stable for hundreds of orbital periods, and have a pattern speed that is less than and of order the rotational velocity at the inner edge of the disk. The origin of these intrinsically global modes is intimately related to the operation of a corotation amplifier in the system. Dissipation of acoustic modes in weak shocks provides a universal mechanism for angular momentum and mass transport even in purely hydrodynamic (i.e. non-magnetized) boundary layers. We discuss the possible implications of these trapped modes for explaining the variability seen in accreting compact objects.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/angular-momentum-transport-and-variability-in-boundary-layers-of-accretion-disks-driven-by-global-acoustic-modes/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
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		<title>Direct MD simulation of liquid-solid phase equilibria for two-component plasmas [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/direct-md-simulation-of-liquid-solid-phase-equilibria-for-two-component-plasmas-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/direct-md-simulation-of-liquid-solid-phase-equilibria-for-two-component-plasmas-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:35:55 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bond angle]]></category>
		<category><![CDATA[carbon ions]]></category>
		<category><![CDATA[component model]]></category>
		<category><![CDATA[constants]]></category>
		<category><![CDATA[cumming]]></category>
		<category><![CDATA[electron screening]]></category>
		<category><![CDATA[equilibrium]]></category>
		<category><![CDATA[finite size effects]]></category>
		<category><![CDATA[liquid phase]]></category>
		<category><![CDATA[md simulation]]></category>
		<category><![CDATA[medin]]></category>
		<category><![CDATA[melting temperature]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[oxygen ions]]></category>
		<category><![CDATA[oxygen system]]></category>
		<category><![CDATA[phase diagram]]></category>
		<category><![CDATA[phase equilibrium]]></category>
		<category><![CDATA[rapid proton]]></category>
		<category><![CDATA[screening effects]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/direct-md-simulation-of-liquid-solid-phase-equilibria-for-two-component-plasmas-replacement/</guid>
		<description><![CDATA[We determine the liquid-solid phase diagram for carbon-oxygen and oxygen-selenium plasma mixtures using two-phase MD simulations. We identified liquid, solid, and interface regions using a bond angle metric. To study finite size effects, we perform 27648 and 55296 ion simulations. To help monitor non-equilibrium effects, we calculate diffusion constants $D_i$. For the carbon-oxygen system we [...]]]></description>
			<content:encoded><![CDATA[<p>We determine the liquid-solid phase diagram for carbon-oxygen and oxygen-selenium plasma mixtures using two-phase MD simulations. We identified liquid, solid, and interface regions using a bond angle metric. To study finite size effects, we perform 27648 and 55296 ion simulations. To help monitor non-equilibrium effects, we calculate diffusion constants $D_i$. For the carbon-oxygen system we find that $D_O$ for oxygen ions in the solid is much smaller than $D_C$ for carbon ions and that both diffusion constants are 80 or more times smaller than diffusion constants in the liquid phase. There is excellent agreement between our carbon-oxygen phase diagram and that predicted by Medin and Cumming. This suggests that errors from finite size and non-equilibrium effects are small and that the carbon-oxygen phase diagram is now accurately known. The oxygen-selenium system is a simple two-component model for more complex rapid proton capture nucleosynthesis ash compositions for an accreting neutron star. Diffusion of oxygen, in a predominately selenium crystal, is remarkably fast, comparable to diffusion in the liquid phase. We find a somewhat lower melting temperature for the oxygen-selenium system than that predicted by Medin and Cumming. This is probably because of electron screening effects.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/direct-md-simulation-of-liquid-solid-phase-equilibria-for-two-component-plasmas-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The inner wind of IRC+10216 revisited: New exotic chemistry and diagnostic for dust condensation in carbon stars [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/the-inner-wind-of-irc10216-revisited-new-exotic-chemistry-and-diagnostic-for-dust-condensation-in-carbon-stars-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/the-inner-wind-of-irc10216-revisited-new-exotic-chemistry-and-diagnostic-for-dust-condensation-in-carbon-stars-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:35:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abundant species]]></category>
		<category><![CDATA[aromatics]]></category>
		<category><![CDATA[carbon dust]]></category>
		<category><![CDATA[carbon star]]></category>
		<category><![CDATA[chemical families]]></category>
		<category><![CDATA[dust formation]]></category>
		<category><![CDATA[formation region]]></category>
		<category><![CDATA[gas layers]]></category>
		<category><![CDATA[halogen]]></category>
		<category><![CDATA[herschel]]></category>
		<category><![CDATA[hydride]]></category>
		<category><![CDATA[inner wind]]></category>
		<category><![CDATA[mass ratio]]></category>
		<category><![CDATA[observational data]]></category>
		<category><![CDATA[polycyclic aromatic hydrocarbon]]></category>
		<category><![CDATA[pulsation period]]></category>
		<category><![CDATA[silicon carbide]]></category>
		<category><![CDATA[stellar pulsation]]></category>
		<category><![CDATA[supergiant star]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/the-inner-wind-of-irc10216-revisited-new-exotic-chemistry-and-diagnostic-for-dust-condensation-in-carbon-stars-replacement/</guid>
		<description><![CDATA[Aims. We model the chemistry of the inner wind of the carbon star IRC+10216 and consider the effect of periodic shocks induced by the stellar pulsation on the gas to follow the non-equilibrium chemistry in the shocked gas layers. We consider a very complete set of chemical families, including hydrocarbons and aromatics, hydrides, halogens and [...]]]></description>
			<content:encoded><![CDATA[<p>Aims. We model the chemistry of the inner wind of the carbon star IRC+10216 and consider the effect of periodic shocks induced by the stellar pulsation on the gas to follow the non-equilibrium chemistry in the shocked gas layers. We consider a very complete set of chemical families, including hydrocarbons and aromatics, hydrides, halogens and phosphorous-bearing species. Derived abundances are compared to the latest observational data from large surveys and Herschel. Results. The shocks induce a non-equilibrium chemistry in the dust formation zone of IRC+10216 where the collision destruction of CO in the post-shock gas triggers the formation of O-bearing species (H2O, SiO). Most of the modelled abundances agree very well with the latest values derived from Herschel data on IRC+10216. Hydrides form a family of abundant species that are expelled into the intermediate envelope. In particular, HF traps all the atomic fluorine in the dust formation zone. Halogens are also abundant and their chemistry is independent of the C/O ratio of the star. Therefore, HCl and other Cl-bearing species should also be present in the inner wind of O-rich AGB or supergiant stars. We identify a specific region ranging from 2.5 R* to 4 R*, where polycyclic aromatic hydrocarbons form and grow. The estimated carbon dust-to-gas mass ratio derived from the mass of aromatics ranges from 1.2 x 10^(-3) to 5.8 x 10^{-3} and agrees well with existing observational values. The aromatic formation region is located outside hot layers where SiC2 is produced as a bi-product of silicon carbide dust synthesis. Finally, we predict that some molecular lines will show flux variation with pulsation phase and time (e.g., H2O) while other species will not (e.g., CO). These variations merely reflect the non-equilibrium chemistry that destroys and reforms molecules over a pulsation period in the shocked gas of the dust formation zone.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/the-inner-wind-of-irc10216-revisited-new-exotic-chemistry-and-diagnostic-for-dust-condensation-in-carbon-stars-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Particle-in-cell simulations of particle energization from low Mach number fast mode shocks [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/particle-in-cell-simulations-of-particle-energization-from-low-mach-number-fast-mode-shocks-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/particle-in-cell-simulations-of-particle-energization-from-low-mach-number-fast-mode-shocks-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:33:19 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[boundary method]]></category>
		<category><![CDATA[cell pic]]></category>
		<category><![CDATA[cell simulation]]></category>
		<category><![CDATA[dimensional particle]]></category>
		<category><![CDATA[electron distribution]]></category>
		<category><![CDATA[electron mass]]></category>
		<category><![CDATA[initial generation]]></category>
		<category><![CDATA[mach number]]></category>
		<category><![CDATA[magnetic pressure]]></category>
		<category><![CDATA[microphysics]]></category>
		<category><![CDATA[moving wall]]></category>
		<category><![CDATA[pic simulations]]></category>
		<category><![CDATA[plasma turbulence]]></category>
		<category><![CDATA[shock formation]]></category>
		<category><![CDATA[shock speed]]></category>
		<category><![CDATA[shock transition]]></category>
		<category><![CDATA[simulation result]]></category>
		<category><![CDATA[simulation time]]></category>
		<category><![CDATA[solar flare]]></category>
		<category><![CDATA[transition region]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/particle-in-cell-simulations-of-particle-energization-from-low-mach-number-fast-mode-shocks-replacement/</guid>
		<description><![CDATA[Astrophysical shocks are often studied in the high Mach number limit but weakly compressive fast shocks can occur in magnetic reconnection outflows and are considered to be a site of particle energization in solar flares. Here we study the microphysics of such perpendicular, low Mach number collisionless shocks using two-dimensional particle-in-cell (PIC) simulations with a [...]]]></description>
			<content:encoded><![CDATA[<p>Astrophysical shocks are often studied in the high Mach number limit but weakly compressive fast shocks can occur in magnetic reconnection outflows and are considered to be a site of particle energization in solar flares. Here we study the microphysics of such perpendicular, low Mach number collisionless shocks using two-dimensional particle-in-cell (PIC) simulations with a reduced ion/electron mass ratio and employ a moving wall boundary method for initial generation of the shock. This moving wall method allows for more control of the shock speed, smaller simulation box sizes, and longer simulation times than the commonly used fixed wall, reflection method of shock formation. Our results, which are independent of the shock formation method, reveal the prevalence shock drift acceleration (SDA) of both electron and ions in a purely perpendicular shock with Alfv\&#8217;en Mach number $M_A=6.8$ and ratio of thermal to magnetic pressure $\beta=8$. We determine the respective minimum energies required for electrons and ions to incur SDA. We derive a theoretical electron distribution via SDA that compares to the simulation results. We also show that a modified two-stream instability due to the incoming and reflecting ions in the shock transition region acts as the mechanism to generate collisionless plasma turbulence that sustains the shock.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/particle-in-cell-simulations-of-particle-energization-from-low-mach-number-fast-mode-shocks-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>The Dominance of Neutrino-Driven Convection in Core-Collapse Supernovae</title>
		<link>http://voxcharta.org/2012/05/16/the-dominance-of-neutrino-driven-convection-in-core-collapse-supernovae/</link>
		<comments>http://voxcharta.org/2012/05/16/the-dominance-of-neutrino-driven-convection-in-core-collapse-supernovae/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:57:25 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[buoyancy]]></category>
		<category><![CDATA[contexts]]></category>
		<category><![CDATA[convection theory]]></category>
		<category><![CDATA[core collapse supernova]]></category>
		<category><![CDATA[core collapse supernovae]]></category>
		<category><![CDATA[dominance]]></category>
		<category><![CDATA[driven convection]]></category>
		<category><![CDATA[equipartition]]></category>
		<category><![CDATA[explosion]]></category>
		<category><![CDATA[instabilities]]></category>
		<category><![CDATA[kinetic energy]]></category>
		<category><![CDATA[motion]]></category>
		<category><![CDATA[natural consequence]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[tangential component]]></category>
		<category><![CDATA[turbulence theory]]></category>
		<category><![CDATA[turbulent dissipation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/the-dominance-of-neutrino-driven-convection-in-core-collapse-supernovae/</guid>
		<description><![CDATA[Multi-dimensional instabilities have become an important ingredient in core-collapse supernova (CCSN) theory. Therefore, it is necessary to understand the driving mechanism of the dominant instability. Comparing 3D CCSN simulations with turbulence theory, we find that buoyancy-driven convection dominates post-shock turbulence. In general, the convective fluxes and kinetic energies in the neutrino-heated region are consistent with [...]]]></description>
			<content:encoded><![CDATA[<p>Multi-dimensional instabilities have become an important ingredient in core-collapse supernova (CCSN) theory. Therefore, it is necessary to understand the driving mechanism of the dominant instability. Comparing 3D CCSN simulations with turbulence theory, we find that buoyancy-driven convection dominates post-shock turbulence. In general, the convective fluxes and kinetic energies in the neutrino-heated region are consistent with expectations of buoyancy-driven convection. Specifically, the convective flux is positive where buoyancy actively drives convection, and the radial and tangential components of the kinetic energy are in rough equipartition (i.e. K_r ~ K_{\theta} + K_{\phi}). Both results are natural consequences of buoyancy-driven convection, and are commonly observed in simulations of convection in other contexts. Most compelling, though, is the consistency between 3D CCSN simulations and predictions of neutrino-driven convection theory. For one, global buoyant driving is balanced by global turbulent dissipation. Secondly, the convective luminosity and turbulent dissipation are linearly proportional to the driving neutrino power. Thirdly, we accurately calculate the shock radius only if we include turbulent ram pressure in the shock conditions. In all, these results suggest that in neutrino-driven explosions the multi-dimensional motions are consistent with neutrino-driven convection, and there is little need to invoke alternative instabilities such as the standing accretion shock instability.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/the-dominance-of-neutrino-driven-convection-in-core-collapse-supernovae/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Detection of Weak Circumstellar Gas around the DAZ White Dwarf WD 1124-293: Evidence for the Accretion of Multiple Asteroids</title>
		<link>http://voxcharta.org/2012/05/16/detection-of-weak-circumstellar-gas-around-the-daz-white-dwarf-wd-1124-293-evidence-for-the-accretion-of-multiple-asteroids/</link>
		<comments>http://voxcharta.org/2012/05/16/detection-of-weak-circumstellar-gas-around-the-daz-white-dwarf-wd-1124-293-evidence-for-the-accretion-of-multiple-asteroids/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:54:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[archival data]]></category>
		<category><![CDATA[asteroids]]></category>
		<category><![CDATA[dusty disk]]></category>
		<category><![CDATA[epochs]]></category>
		<category><![CDATA[equivalent width]]></category>
		<category><![CDATA[infrared excess]]></category>
		<category><![CDATA[k line]]></category>
		<category><![CDATA[las campanas observatory]]></category>
		<category><![CDATA[local interstellar medium]]></category>
		<category><![CDATA[planetary companion]]></category>
		<category><![CDATA[planetary system]]></category>
		<category><![CDATA[sightline]]></category>
		<category><![CDATA[spectrograph]]></category>
		<category><![CDATA[term trend]]></category>
		<category><![CDATA[tidal disruption]]></category>
		<category><![CDATA[white dwarf]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/detection-of-weak-circumstellar-gas-around-the-daz-white-dwarf-wd-1124-293-evidence-for-the-accretion-of-multiple-asteroids/</guid>
		<description><![CDATA[Single metal polluted white dwarfs with no dusty disks are believed to be actively accreting metals from a circumstellar disk of gas caused by the destruction of asteroids perturbed by planetary systems. We report, for the first time, the detection of circumstellar Ca~II gas in absorption around the DAZ WD~1124-293, which lacks an infrared excess. [...]]]></description>
			<content:encoded><![CDATA[<p>Single metal polluted white dwarfs with no dusty disks are believed to be actively accreting metals from a circumstellar disk of gas caused by the destruction of asteroids perturbed by planetary systems. We report, for the first time, the detection of circumstellar Ca~II gas in absorption around the DAZ WD~1124-293, which lacks an infrared excess. We constrain the gas to $&gt;$7 $R_{\rm WD}$ and $&lt;$32000~AU, and estimate it to be at $\sim$54~R$_{\rm WD}$, well within WD~1124-293&#039;s tidal disruption radius. This detection is based on several epochs of spectroscopy around the Ca~II H and K lines ($\lambda$=3968\AA, 3933\AA) with the MIKE spectrograph on the Magellan/Clay Telescope at Las Campanas Observatory. We confirm the circumstellar nature of the gas by observing nearby sightlines and finding no evidence for gas from the local interstellar medium. Through archival data we have measured the equivalent width of the two photospheric Ca lines over a period of 11 years. We see $$ R$_{\rm \oplus}$ using the WASP survey. The presence of gas in orbit around WD~1124-293 implies that most DAZs could harbor planetary systems. Since 25-30\% of white dwarfs show metal line absorption, the dynamical process for perturbing small bodies must be robust.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/detection-of-weak-circumstellar-gas-around-the-daz-white-dwarf-wd-1124-293-evidence-for-the-accretion-of-multiple-asteroids/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Inter-Eruption Timescale of Classical Novae from Expansion of the Z Camelopardalis Shell</title>
		<link>http://voxcharta.org/2012/05/16/the-inter-eruption-timescale-of-classical-novae-from-expansion-of-the-z-camelopardalis-shell/</link>
		<comments>http://voxcharta.org/2012/05/16/the-inter-eruption-timescale-of-classical-novae-from-expansion-of-the-z-camelopardalis-shell/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:53:31 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[220 years]]></category>
		<category><![CDATA[astrologers]]></category>
		<category><![CDATA[bce]]></category>
		<category><![CDATA[bright nova]]></category>
		<category><![CDATA[camelopardalis]]></category>
		<category><![CDATA[classical novae]]></category>
		<category><![CDATA[deceleration]]></category>
		<category><![CDATA[dwarf nova]]></category>
		<category><![CDATA[dwarf novae]]></category>
		<category><![CDATA[ejecta]]></category>
		<category><![CDATA[interstellar matter]]></category>
		<category><![CDATA[Measurement]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[nova eruptions]]></category>
		<category><![CDATA[nova shell]]></category>
		<category><![CDATA[outburst]]></category>
		<category><![CDATA[radius]]></category>
		<category><![CDATA[suggestion]]></category>
		<category><![CDATA[timescale]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/the-inter-eruption-timescale-of-classical-novae-from-expansion-of-the-z-camelopardalis-shell/</guid>
		<description><![CDATA[The dwarf nova Z Camelopardalis is surrounded by the largest known classical nova shell. This shell demonstrates that at least some dwarf novae must have undergone classical nova eruptions in the past, and that at least some classical novae become dwarf novae long after their nova thermonuclear outbursts. The current size of the shell, its [...]]]></description>
			<content:encoded><![CDATA[<p>The dwarf nova Z Camelopardalis is surrounded by the largest known classical nova shell. This shell demonstrates that at least some dwarf novae must have undergone classical nova eruptions in the past, and that at least some classical novae become dwarf novae long after their nova thermonuclear outbursts. The current size of the shell, its known distance, and the largest observed nova ejection velocity set a lower limit to the time since Z Cam&#8217;s last outburst of 220 years. The brightest part of the Z Cam shell&#8217;s radius is currently p ~ 1690 pixels. No expansion of the radius of the brightest part of the ejecta was detected, with an upper limit of pdot  5,000 years ago. However, including the important effect of deceleration as the ejecta sweeps up interstellar matter in its snowplow phase reduces the lower limit to 1300 years. This is the first strong test of the prediction of nova thermonuclear runaway theory that the inter-outburst times of classical novae are longer than 1000 yr. The intriguing suggestion that Z Cam was a bright nova, recorded by Chinese imperial astrologers in October &#8211; November 77 BCE, is consistent with our measurements. If Z Cam was indeed the nova of 77 BCE we predict that its ejecta are currently expanding at 85 km/s, or 0.11 arcsec/yr. Detection and measurement of this rate of expansion are doable in just a few years.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/the-inter-eruption-timescale-of-classical-novae-from-expansion-of-the-z-camelopardalis-shell/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>The equilibrium tide in stars and giant planets: I &#8211; the coplanar case</title>
		<link>http://voxcharta.org/2012/05/16/the-equilibrium-tide-in-stars-and-giant-planets-i-the-coplanar-case/</link>
		<comments>http://voxcharta.org/2012/05/16/the-equilibrium-tide-in-stars-and-giant-planets-i-the-coplanar-case/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:53:11 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[characteristic evolution]]></category>
		<category><![CDATA[constant time delay]]></category>
		<category><![CDATA[convective envelope]]></category>
		<category><![CDATA[dynamical evolution]]></category>
		<category><![CDATA[eddy viscosity]]></category>
		<category><![CDATA[evolution equation]]></category>
		<category><![CDATA[extrasolar planet]]></category>
		<category><![CDATA[fluid bodies]]></category>
		<category><![CDATA[giant planet]]></category>
		<category><![CDATA[imaginary part]]></category>
		<category><![CDATA[orbital evolution]]></category>
		<category><![CDATA[parent star]]></category>
		<category><![CDATA[physical mechanism]]></category>
		<category><![CDATA[point mass]]></category>
		<category><![CDATA[quality factor]]></category>
		<category><![CDATA[tidal dissipation]]></category>
		<category><![CDATA[tidal flow]]></category>
		<category><![CDATA[tidal interaction]]></category>
		<category><![CDATA[turnover rate]]></category>
		<category><![CDATA[velocity field]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/the-equilibrium-tide-in-stars-and-giant-planets-i-the-coplanar-case/</guid>
		<description><![CDATA[Since 1995, more than 500 extrasolar planets have been discovered orbiting very close to their parent star, where they experience strong tidal interactions. Their orbital evolution depends on the physical mechanisms that cause tidal dissipation, and these are still not well understood. We refine the theory of the equilibrium tide in fluid bodies that are [...]]]></description>
			<content:encoded><![CDATA[<p>Since 1995, more than 500 extrasolar planets have been discovered orbiting very close to their parent star, where they experience strong tidal interactions. Their orbital evolution depends on the physical mechanisms that cause tidal dissipation, and these are still not well understood. We refine the theory of the equilibrium tide in fluid bodies that are partly or entirely convective, to predict the dynamical evolution of the systems. In particular, we examine the validity of modeling the tidal dissipation by the quality factor Q, as is commonly done. We consider here the simplest case where the considered star or planet rotates uniformly, all spins are aligned, and the companion is reduced to a point-mass. The first manifestation of the tide is to distort the shape of the star or planet adiabatically along the line of centers. This generates the divergence-free velocity field of the adiabatic equilibrium tide which is decoupled from the dynamical tide. The tidal kinetic energy is dissipated into heat through turbulent friction, which is modeled here as an eddy-viscosity acting on the adiabatic tidal flow. This dissipation induces a second velocity field, the dissipative equilibrium tide, which is in quadrature with the exciting potential; it is responsible for the imaginary part of the disturbing function, which is implemented in the dynamical evolution equations, from which one derives characteristic evolution times. The rate at which the system evolves depends on the physical properties of tidal dissipation, and specifically on how the eddy viscosity varies with tidal frequency and on the thickness of the convective envelope for the fluid equilibrium tide. At low frequency, this tide retards by a constant time delay, whereas it lags by a constant angle when the tidal frequency exceeds the convective turnover rate.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/the-equilibrium-tide-in-stars-and-giant-planets-i-the-coplanar-case/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Solving the Puzzle of the Massive Star System Theta 2 Orionis A</title>
		<link>http://voxcharta.org/2012/05/16/solving-the-puzzle-of-the-massive-star-system-theta-2-orionis-a/</link>
		<comments>http://voxcharta.org/2012/05/16/solving-the-puzzle-of-the-massive-star-system-theta-2-orionis-a/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:52:56 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acis]]></category>
		<category><![CDATA[arcsec]]></category>
		<category><![CDATA[Chandra]]></category>
		<category><![CDATA[dipole field]]></category>
		<category><![CDATA[intermediate mass]]></category>
		<category><![CDATA[magnetic confinement]]></category>
		<category><![CDATA[magnetic field strength]]></category>
		<category><![CDATA[magnetic reconnection]]></category>
		<category><![CDATA[magnetosphere]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[ori]]></category>
		<category><![CDATA[position angle]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[speckle interferometry]]></category>
		<category><![CDATA[spectroscopic binary]]></category>
		<category><![CDATA[star system]]></category>
		<category><![CDATA[wind shock]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/solving-the-puzzle-of-the-massive-star-system-theta-2-orionis-a/</guid>
		<description><![CDATA[The young O9.5 V spectroscopic binary Theta 2 Ori A shows moderately hard X-ray emission and relatively narrow X-ray lines, suggesting that it may be a Magnetically Confined Wind Shock (MCWS) source, similar to its more massive analogue Theta 1 Ori C. X-ray flares occurring near periastron led to the suggestion that the flares are [...]]]></description>
			<content:encoded><![CDATA[<p>The young O9.5 V spectroscopic binary Theta 2 Ori A shows moderately hard X-ray emission and relatively narrow X-ray lines, suggesting that it may be a Magnetically Confined Wind Shock (MCWS) source, similar to its more massive analogue Theta 1 Ori C. X-ray flares occurring near periastron led to the suggestion that the flares are produced via magnetic reconnection as magnetospheres on both components of the Theta 2 Ori A binary interact at closest approach.   We use a series of high-resolution spectropolarimetric observations of Theta 2 Ori A to place an upper limit on the magnetic field strength of 135 G (95% credible region). Such a weak dipole field would not produce magnetic confinement, or a large magnetosphere. A sub-pixel analysis of the Chandra ACIS images of Theta 2 Ori A obtained during quiescence and flaring show that the hard, flaring X-rays are offset from the soft, quiescent emission by 0.4 arcsec. If the soft emission is associated with the A1/A2 spectroscopic binary, the offset and position angle of the hard, flaring source place it at the location of the intermediate-mass A3 companion, discovered via speckle interferometry. The spectropolarimetric and X-ray results taken together point to the A3 companion, not the massive A1/A2 binary, as the source of hard, flaring X-ray emission.   We also discuss a similar analysis performed for the magnetic Bp star Sigma Ori E. We find a similar origin for its X-ray flaring.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/solving-the-puzzle-of-the-massive-star-system-theta-2-orionis-a/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>The magnetic fields and magnetospheres of hot stars</title>
		<link>http://voxcharta.org/2012/05/16/the-magnetic-fields-and-magnetospheres-of-hot-stars/</link>
		<comments>http://voxcharta.org/2012/05/16/the-magnetic-fields-and-magnetospheres-of-hot-stars/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:50:18 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[canada france]]></category>
		<category><![CDATA[characterisation]]></category>
		<category><![CDATA[direct evidence]]></category>
		<category><![CDATA[hawaii telescope]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[new generation]]></category>
		<category><![CDATA[observing tools]]></category>
		<category><![CDATA[resolution spectroscopy]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/the-magnetic-fields-and-magnetospheres-of-hot-stars/</guid>
		<description><![CDATA[Strong advances in direct evidence of magnetic fields in hot massive stars have been possible thanks to the new generation of high-resolution spectropolarimeters such as ESPaDOnS (on the Canada-France-Hawaii Telescope) or HARPSpol (on the 3.6m ESO telescope). UV and optical high-resolution spectroscopy has also been very useful to study the magnetospheres of massive stars. In [...]]]></description>
			<content:encoded><![CDATA[<p>Strong advances in direct evidence of magnetic fields in hot massive stars have been possible thanks to the new generation of high-resolution spectropolarimeters such as ESPaDOnS (on the Canada-France-Hawaii Telescope) or HARPSpol (on the 3.6m ESO telescope). UV and optical high-resolution spectroscopy has also been very useful to study the magnetospheres of massive stars. In this contribution I review the observing tools and our current knowledge concerning the detection and characterisation of the magnetic fields and magnetospheres in hot stars.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/the-magnetic-fields-and-magnetospheres-of-hot-stars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Coronal activity cycles in nearby G and K stars &#8211; XMM-Newton monitoring of 61 Cygni and Alpha Centauri</title>
		<link>http://voxcharta.org/2012/05/16/coronal-activity-cycles-in-nearby-g-and-k-stars-xmm-newton-monitoring-of-61-cygni-and-alpha-centauri/</link>
		<comments>http://voxcharta.org/2012/05/16/coronal-activity-cycles-in-nearby-g-and-k-stars-xmm-newton-monitoring-of-61-cygni-and-alpha-centauri/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:48:12 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[61 cygni]]></category>
		<category><![CDATA[activity cycles]]></category>
		<category><![CDATA[alpha cen]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[average temperature]]></category>
		<category><![CDATA[binaries]]></category>
		<category><![CDATA[brightness variation]]></category>
		<category><![CDATA[k star]]></category>
		<category><![CDATA[k7v]]></category>
		<category><![CDATA[magnetic activity]]></category>
		<category><![CDATA[order of magnitude]]></category>
		<category><![CDATA[plasma components]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[ray observations]]></category>
		<category><![CDATA[spectral changes]]></category>
		<category><![CDATA[term evolution]]></category>
		<category><![CDATA[variability]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xmm newton]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/coronal-activity-cycles-in-nearby-g-and-k-stars-xmm-newton-monitoring-of-61-cygni-and-alpha-centauri/</guid>
		<description><![CDATA[We use X-ray observations of the nearby binaries 61 Cyg A/B (K5V and K7V) and Alpha Cen A/B (G2V and K1V) to study the long-term evolution of magnetic activity in weakly to moderately active G + K dwarfs over nearly a decade. Specifically we search for X-ray activity cycles and related coronal changes and compare [...]]]></description>
			<content:encoded><![CDATA[<p>We use X-ray observations of the nearby binaries 61 Cyg A/B (K5V and K7V) and Alpha Cen A/B (G2V and K1V) to study the long-term evolution of magnetic activity in weakly to moderately active G + K dwarfs over nearly a decade. Specifically we search for X-ray activity cycles and related coronal changes and compare them to the solar behavior. For 61 Cyg A we find a regular coronal activity cycle analog to its 7.3 yr chromospheric cycle. The X-ray brightness variations are with a factor of three significantly lower than on the Sun, yet the changes of coronal properties resemble the solar behavior with larger variations occurring in the respective hotter plasma components. 61 Cyg B does not show a clear cyclic coronal trend so far, but the X-ray data matches the more irregular chromospheric cycle. Both Alpha Cen stars exhibit significant long-term X-ray variability. Alpha Cen A shows indications for cyclic variability of an order of magnitude with a period of about 12-15 years; the Alpha Cen B data suggests an X-ray cycle with an amplitude of about six to eight and a period of 8-9 years. The sample stars exhibit X-ray luminosities ranging between Lx &lt; 1&#215;10^26 &#8211; 3&#215;10^27 erg s^-1 in the 0.2-2.0 keV band and have coronae dominated by cool plasma with variable average temperatures of around 1.0-2.5 MK. We find that coronal activity cycles are apparently a common phenomenon in older, slowly rotating G and K stars. The spectral changes of the coronal X-ray emission over the cycles are solar-like in all studied targets.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/coronal-activity-cycles-in-nearby-g-and-k-stars-xmm-newton-monitoring-of-61-cygni-and-alpha-centauri/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Progenitor-Explosion Connection and Remnant Birth Masses for Neutrino-Driven Supernovae of Iron-Core Progenitors</title>
		<link>http://voxcharta.org/2012/05/16/progenitor-explosion-connection-and-remnant-birth-masses-for-neutrino-driven-supernovae-of-iron-core-progenitors/</link>
		<comments>http://voxcharta.org/2012/05/16/progenitor-explosion-connection-and-remnant-birth-masses-for-neutrino-driven-supernovae-of-iron-core-progenitors/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:47:39 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[blast wave]]></category>
		<category><![CDATA[boundary condition]]></category>
		<category><![CDATA[driven wind]]></category>
		<category><![CDATA[empirical distribution]]></category>
		<category><![CDATA[energetic explosions]]></category>
		<category><![CDATA[energy release]]></category>
		<category><![CDATA[free parameter]]></category>
		<category><![CDATA[high density]]></category>
		<category><![CDATA[hydrogen envelope]]></category>
		<category><![CDATA[inner boundary]]></category>
		<category><![CDATA[iron core]]></category>
		<category><![CDATA[main sequence]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[nickel production]]></category>
		<category><![CDATA[progenitor]]></category>
		<category><![CDATA[solar mass]]></category>
		<category><![CDATA[solar metallicity]]></category>
		<category><![CDATA[spherical symmetry]]></category>
		<category><![CDATA[stellar structure]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/progenitor-explosion-connection-and-remnant-birth-masses-for-neutrino-driven-supernovae-of-iron-core-progenitors/</guid>
		<description><![CDATA[We perform hydrodynamic supernova simulations in spherical symmetry for over 100 single stars of solar metallicity to explore the progenitor-explosion and progenitor-remnant connections established by the neutrino-driven mechanism. We use an approximative treatment of neutrino transport and replace the high-density interior of the neutron star (NS) by an inner boundary condition based on an analytic [...]]]></description>
			<content:encoded><![CDATA[<p>We perform hydrodynamic supernova simulations in spherical symmetry for over 100 single stars of solar metallicity to explore the progenitor-explosion and progenitor-remnant connections established by the neutrino-driven mechanism. We use an approximative treatment of neutrino transport and replace the high-density interior of the neutron star (NS) by an inner boundary condition based on an analytic proto-NS core-cooling model, whose free parameters are chosen such that explosion energy, nickel production, and energy release by the compact remnant of progenitors around 20 solar masses are compatible with Supernova 1987A. Thus we are able to simulate the accretion phase, initiation of the explosion, subsequent neutrino-driven wind phase for 15-20 s, and the further evolution of the blast wave for hours to days until fallback is completed. Our results challenge long-standing paradigms. We find that remnant mass, launch time, and properties of the explosion depend strongly on the stellar structure and exhibit large variability even in narrow intervals of the progenitors&#8217; zero-age-main-sequence mass. While all progenitors with masses below about 15 solar masses yield NSs, black hole (BH) as well as NS formation is possible for more massive stars, where partial loss of the hydrogen envelope leads to weak reverse shocks and weak fallback. Our NS masses of ~1.2-2.0 solar masses and BH masses &gt;6 solar masses are compatible with a possible lack of low-mass BHs in the empirical distribution. Neutrino heating accounts for SN energies between some 10^{50} erg and about 2*10^{51} erg, but can hardly explain more energetic explosions and nickel masses higher than 0.1-0.2 solar masses. These seem to require an alternative SN mechanism.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/progenitor-explosion-connection-and-remnant-birth-masses-for-neutrino-driven-supernovae-of-iron-core-progenitors/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Chemical compositions of thin-disk, high-metallicity red horizontal-branch field stars</title>
		<link>http://voxcharta.org/2012/05/16/chemical-compositions-of-thin-disk-high-metallicity-red-horizontal-branch-field-stars/</link>
		<comments>http://voxcharta.org/2012/05/16/chemical-compositions-of-thin-disk-high-metallicity-red-horizontal-branch-field-stars/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:47:24 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[atmospheric parameters]]></category>
		<category><![CDATA[chemical composition]]></category>
		<category><![CDATA[eff]]></category>
		<category><![CDATA[equivalent width]]></category>
		<category><![CDATA[field star]]></category>
		<category><![CDATA[horizontal branch]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[M. Smith]]></category>
		<category><![CDATA[mcdonald observatory]]></category>
		<category><![CDATA[neutron]]></category>
		<category><![CDATA[ratios]]></category>
		<category><![CDATA[relative abundance]]></category>
		<category><![CDATA[smith telescope]]></category>
		<category><![CDATA[solar metallicity]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectrum analyses]]></category>
		<category><![CDATA[stellar evolution]]></category>
		<category><![CDATA[target star]]></category>
		<category><![CDATA[thin disk]]></category>
		<category><![CDATA[velocities]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/chemical-compositions-of-thin-disk-high-metallicity-red-horizontal-branch-field-stars/</guid>
		<description><![CDATA[We present a detailed abundance analysis and atmospheric parameters of 76 stars from a survey to identify field Galactic red horizontal-branch (RHB) stars. High-resolution echelle spectra (R\simeq60,000, S/N&#62;=100) were obtained with 2.7 m Smith Telescope at McDonald Observatory. The target stars were selected only by color and parallax information. Overall metallicities and relative abundances of [...]]]></description>
			<content:encoded><![CDATA[<p>We present a detailed abundance analysis and atmospheric parameters of 76 stars from a survey to identify field Galactic red horizontal-branch (RHB) stars. High-resolution echelle spectra (R\simeq60,000, S/N&gt;=100) were obtained with 2.7 m Smith Telescope at McDonald Observatory. The target stars were selected only by color and parallax information. Overall metallicities and relative abundances of proton-capture elements (C I, N I, O I, Li I), alpha-elements (Ca I and Si I), and neutron-capture elements (Eu II and La II) were determined by either equivalent width or synthetic spectrum analyses. We used CN features at 7995-8040 {\AA} region in order to determine 12^C/13^C ratios of our targets. Investigation of the evolutionary stages, using spectroscopic T_eff and log g values along with derived 12^C/13^C ratios, revealed the presence of 18 probable RHB stars in our sample. We also derived kinematics of the stars with available distance information. Taking into account both the kinematics and probable evolutionary stages, we conclude that our sample contains five thick disk and 13 thin disk RHB stars. Up until now, RHB stars have been considered as members of the thick disk, and were expected to have large space velocities and sub-solar metallicities. However, our sample is dominated by low velocity solar-metallicity RHB stars; their existence cannot be easily explained with standard stellar evolution.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/chemical-compositions-of-thin-disk-high-metallicity-red-horizontal-branch-field-stars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Self-cancellation of ephemeral regions in the quiet Sun</title>
		<link>http://voxcharta.org/2012/05/16/self-cancellation-of-ephemeral-regions-in-the-quiet-sun/</link>
		<comments>http://voxcharta.org/2012/05/16/self-cancellation-of-ephemeral-regions-in-the-quiet-sun/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:43:52 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cancellation]]></category>
		<category><![CDATA[energy release]]></category>
		<category><![CDATA[ephemeral regions]]></category>
		<category><![CDATA[ers]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[imager]]></category>
		<category><![CDATA[magnetic energy]]></category>
		<category><![CDATA[magnetic flux]]></category>
		<category><![CDATA[magnetic loop]]></category>
		<category><![CDATA[ners]]></category>
		<category><![CDATA[observatory]]></category>
		<category><![CDATA[patches]]></category>
		<category><![CDATA[polarity]]></category>
		<category><![CDATA[quiet sun]]></category>
		<category><![CDATA[sers]]></category>
		<category><![CDATA[submergence]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/self-cancellation-of-ephemeral-regions-in-the-quiet-sun/</guid>
		<description><![CDATA[With the observations from the Helioseismic and Magnetic Imager aboard the Solar Dynamics Observatory, we statistically investigate the ephemeral regions (ERs) in the quiet Sun. We find that there are two types of ERs: normal ERs (NERs) and self-cancelled ERs (SERs). Each NER emerges and grows with separation of its opposite polarity patches which will [...]]]></description>
			<content:encoded><![CDATA[<p>With the observations from the Helioseismic and Magnetic Imager aboard the Solar Dynamics Observatory, we statistically investigate the ephemeral regions (ERs) in the quiet Sun. We find that there are two types of ERs: normal ERs (NERs) and self-cancelled ERs (SERs). Each NER emerges and grows with separation of its opposite polarity patches which will cancel or coalesce with other surrounding magnetic flux. Each SER also emerges and grows and its dipolar patches separate at first, but a part of magnetic flux of the SER will move together and cancel gradually, which is described with the term &#8220;self-cancellation&#8221; by us. We identify 2988 ERs among which there are 190 SERs, about 6.4% of the ERs. The mean value of self-cancellation fraction of SERs is 62.5%, and the total self-cancelled flux of SERs is 9.8% of the total ER flux. Our results also reveal that the higher the ER magnetic flux is, (i) the easier the performance of ER self-cancellation is, (ii) the smaller the self-cancellation fraction is, and (iii) the more the self-cancelled flux is. We think that the self-cancellation of SERs is caused by the submergence of magnetic loops connecting the dipolar patches, without magnetic energy release.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/self-cancellation-of-ephemeral-regions-in-the-quiet-sun/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Non-thermal burst-on-tail of long-duration solar event on 2003 October 26</title>
		<link>http://voxcharta.org/2012/05/16/non-thermal-burst-on-tail-of-long-duration-solar-event-on-2003-october-26/</link>
		<comments>http://voxcharta.org/2012/05/16/non-thermal-burst-on-tail-of-long-duration-solar-event-on-2003-october-26/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:43:20 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[burst]]></category>
		<category><![CDATA[duration]]></category>
		<category><![CDATA[flare]]></category>
		<category><![CDATA[impulsive phase]]></category>
		<category><![CDATA[lde]]></category>
		<category><![CDATA[magnetic loop]]></category>
		<category><![CDATA[microwave emission]]></category>
		<category><![CDATA[october 26]]></category>
		<category><![CDATA[phenomenon]]></category>
		<category><![CDATA[plasma]]></category>
		<category><![CDATA[population]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[scale loops]]></category>
		<category><![CDATA[soft x]]></category>
		<category><![CDATA[solar event]]></category>
		<category><![CDATA[spatial scale]]></category>
		<category><![CDATA[thermal electrons]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/non-thermal-burst-on-tail-of-long-duration-solar-event-on-2003-october-26/</guid>
		<description><![CDATA[On the base of one particular long-duration solar event (LDE) of X1.2-class on 2003 October 26 it is shown that observable response of active region plasma (flux of soft X-ray emission, emission measure and temperature) to accelerated electrons can change drastically in time. This LDE is outstanding among others due to the presence of very [...]]]></description>
			<content:encoded><![CDATA[<p>On the base of one particular long-duration solar event (LDE) of X1.2-class on 2003 October 26 it is shown that observable response of active region plasma (flux of soft X-ray emission, emission measure and temperature) to accelerated electrons can change drastically in time. This LDE is outstanding among others due to the presence of very strong &#8220;burst-on-tail&#8221; of non-thermal hard X-ray and microwave emissions about 90 min after its onset without significant response in the range of soft X-ray emission. Based on the spatially-resolved observations of the flare region a following interpretation of this phenomenon is proposed. During the &#8220;burst-on-tail&#8221; accelerated electrons were injected into magnetic loops of larger spatial scale than during the impulsive phase bursts. This was due to the natural for LDEs growth of the flaring loops. Therefore, precipitation of similar population of non-thermal electrons into footpoints of the larger-scale loops resulted in much smaller fluxes of soft X-ray emission, temperature and emission measure of plasma evaporated into their coronal volume.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/non-thermal-burst-on-tail-of-long-duration-solar-event-on-2003-october-26/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Simultaneous Observations of a Large-Scale Wave Event in the Solar Atmosphere: From Photosphere to Corona</title>
		<link>http://voxcharta.org/2012/05/16/simultaneous-observations-of-a-large-scale-wave-event-in-the-solar-atmosphere-from-photosphere-to-corona/</link>
		<comments>http://voxcharta.org/2012/05/16/simultaneous-observations-of-a-large-scale-wave-event-in-the-solar-atmosphere-from-photosphere-to-corona/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:42:49 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[aia]]></category>
		<category><![CDATA[coronal mass ejection]]></category>
		<category><![CDATA[deceleration]]></category>
		<category><![CDATA[euv observations]]></category>
		<category><![CDATA[hida]]></category>
		<category><![CDATA[high spatial resolution]]></category>
		<category><![CDATA[initial stage]]></category>
		<category><![CDATA[photosphere]]></category>
		<category><![CDATA[primary wave]]></category>
		<category><![CDATA[reconfiguration]]></category>
		<category><![CDATA[research telescope]]></category>
		<category><![CDATA[resolution observations]]></category>
		<category><![CDATA[shock wave]]></category>
		<category><![CDATA[simultaneous observations]]></category>
		<category><![CDATA[solar atmosphere]]></category>
		<category><![CDATA[solar magnetic activity]]></category>
		<category><![CDATA[solar surface]]></category>
		<category><![CDATA[transition region]]></category>
		<category><![CDATA[wave event]]></category>
		<category><![CDATA[wave speed]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/simultaneous-observations-of-a-large-scale-wave-event-in-the-solar-atmosphere-from-photosphere-to-corona/</guid>
		<description><![CDATA[For the first time, we report a large-scale wave that was observed simultaneously in the photosphere, chromosphere, transition region and low corona layers of the solar atmosphere. Using the high temporal and high spatial resolution observations taken by the Solar Magnetic Activity Research Telescope at Hida Observatory and the Atmospheric Imaging Assembly (AIA) onboard Solar [...]]]></description>
			<content:encoded><![CDATA[<p>For the first time, we report a large-scale wave that was observed simultaneously in the photosphere, chromosphere, transition region and low corona layers of the solar atmosphere. Using the high temporal and high spatial resolution observations taken by the Solar Magnetic Activity Research Telescope at Hida Observatory and the Atmospheric Imaging Assembly (AIA) onboard Solar Dynamic Observatory, we find that the wave evolved synchronously at different heights of the solar atmosphere, and it propagated at a speed of 605 km/s and showed a significant deceleration (-424 m/s2) in the extreme-ultraviolet (EUV) observations. During the initial stage, the wave speed in the EUV observations was 1000 km/s, similar to those measured from the AIA 1700 {\AA} (967 km/s) and 1600 {\AA} (893 km/s) observations. The wave was reflected by a remote region with open fields, and a slower wave-like feature at a speed of 220 km/s was also identified following the primary fast wave. In addition, a type-II radio burst was observed to be associated with the wave. We conclude that this wave should be a fast magnetosonic shock wave, which was firstly driven by the associated coronal mass ejection and then propagated freely in the corona. As the shock wave propagated, its legs swept the solar surface and thereby resulted in the wave signatures observed in the lower layers of the solar atmosphere. The slower wave-like structure following the primary wave was probably caused by the reconfiguration of the low coronal magnetic fields, as predicted in the field-line stretching model.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/simultaneous-observations-of-a-large-scale-wave-event-in-the-solar-atmosphere-from-photosphere-to-corona/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Measuring the mass accretion rates of Herbig Ae/Be stars with X-shooter</title>
		<link>http://voxcharta.org/2012/05/16/measuring-the-mass-accretion-rates-of-herbig-aebe-stars-with-x-shooter/</link>
		<comments>http://voxcharta.org/2012/05/16/measuring-the-mass-accretion-rates-of-herbig-aebe-stars-with-x-shooter/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:42:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion rates]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[brown dwarf]]></category>
		<category><![CDATA[calibration]]></category>
		<category><![CDATA[herbig]]></category>
		<category><![CDATA[high sensitivity]]></category>
		<category><![CDATA[medium resolution]]></category>
		<category><![CDATA[rate variability]]></category>
		<category><![CDATA[shooter]]></category>
		<category><![CDATA[spectral data]]></category>
		<category><![CDATA[spectral diagnostics]]></category>
		<category><![CDATA[spectrum]]></category>
		<category><![CDATA[Sun]]></category>
		<category><![CDATA[t tauri]]></category>
		<category><![CDATA[target]]></category>
		<category><![CDATA[tens]]></category>
		<category><![CDATA[time scale]]></category>
		<category><![CDATA[type star]]></category>
		<category><![CDATA[ut2]]></category>
		<category><![CDATA[wavelength range]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/measuring-the-mass-accretion-rates-of-herbig-aebe-stars-with-x-shooter/</guid>
		<description><![CDATA[We present the results of our observations of eight magnetic Herbig Ae/Be stars obtained with the X-shooter spectrograph mounted on UT2 at the VLT. X-shooter provides a simultaneous, medium-resolution and high-sensitivity spectrum over the entire wavelength range from 300 to 2500 nm. We estimate the mass accretion rates M_acc of the targets from 13 different [...]]]></description>
			<content:encoded><![CDATA[<p>We present the results of our observations of eight magnetic Herbig Ae/Be stars obtained with the X-shooter spectrograph mounted on UT2 at the VLT. X-shooter provides a simultaneous, medium-resolution and high-sensitivity spectrum over the entire wavelength range from 300 to 2500 nm. We estimate the mass accretion rates M_acc of the targets from 13 different spectral diagnostics using empiric calibrations derived previously for T Tauri-type stars and brown dwarfs. We have estimated the mass accretion rates of our targets, which range from 2&#215;10^-9 to 2&#215;10^-7 M_sun/yr. Furthermore, we have found accretion rate variability with amplitudes of 0.10-0.40 dex taking place on time scales from one day to tens of days. Additional future night-to-night observations need to be carried out to investigate the character of M_acc variability in details. Our study shows that the majority of the calibrational relations can be applied to Herbig Ae/Be stars, but several of them need to be re-calibrated on the basis of new spectral data for a larger number of Herbig Ae/Be stars.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/measuring-the-mass-accretion-rates-of-herbig-aebe-stars-with-x-shooter/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Evidence for the Wave Nature of an Extreme Ultraviolet Wave Observed by the Atmospheric Imaging Assembly Onboard the Solar Dynamics Observatory</title>
		<link>http://voxcharta.org/2012/05/16/evidence-for-the-wave-nature-of-an-extreme-ultraviolet-wave-observed-by-the-atmospheric-imaging-assembly-onboard-the-solar-dynamics-observatory/</link>
		<comments>http://voxcharta.org/2012/05/16/evidence-for-the-wave-nature-of-an-extreme-ultraviolet-wave-observed-by-the-atmospheric-imaging-assembly-onboard-the-solar-dynamics-observatory/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:42:28 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[deceleration]]></category>
		<category><![CDATA[dispersive nature]]></category>
		<category><![CDATA[euv]]></category>
		<category><![CDATA[filament]]></category>
		<category><![CDATA[flank]]></category>
		<category><![CDATA[initial period]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[mach number]]></category>
		<category><![CDATA[mass ejection]]></category>
		<category><![CDATA[photosphere]]></category>
		<category><![CDATA[polar coronal hole]]></category>
		<category><![CDATA[quiet sun]]></category>
		<category><![CDATA[reflection effect]]></category>
		<category><![CDATA[refraction]]></category>
		<category><![CDATA[resolution observations]]></category>
		<category><![CDATA[solar terrestrial relations observatory]]></category>
		<category><![CDATA[sound speed]]></category>
		<category><![CDATA[spatial resolution]]></category>
		<category><![CDATA[wave nature]]></category>
		<category><![CDATA[wavefront]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/evidence-for-the-wave-nature-of-an-extreme-ultraviolet-wave-observed-by-the-atmospheric-imaging-assembly-onboard-the-solar-dynamics-observatory/</guid>
		<description><![CDATA[Extreme Ultraviolet (EUV) waves have been found for about 15 years. However, significant controversy remains over their physical natures and origins. In this paper, we report an EUV wave that was accompanied by an X1.9 flare and a partial halo coronal mass ejection. Using high temporal and spatial resolution observations taken by the {\em Solar [...]]]></description>
			<content:encoded><![CDATA[<p>Extreme Ultraviolet (EUV) waves have been found for about 15 years. However, significant controversy remains over their physical natures and origins. In this paper, we report an EUV wave that was accompanied by an X1.9 flare and a partial halo coronal mass ejection. Using high temporal and spatial resolution observations taken by the {\em Solar Dynamics Observatory} and the Solar-TErrestrial RElations Observatory, we are able to investigate the detailed kinematics of the EUV wave. We find several arguments that support the fast-mode wave scenario: (1) The speed of the EUV wave (570 km/s) is higher than the sound speed of quiet-Sun corona. (2) Significant deceleration of the EUV wave (-130 m/s2) is found during its propagation. (3) The EUV wave resulted in the oscillations of a loop and a filament along its propagation path, and a reflected wave from the polar coronal hole is also detected. (4) Refraction or reflection effect is observed when the EUV wave was passing through two coronal bright points. (5) The dimming region behind the wavefront stopped to expand when the wavefront started to become diffuse. (6) The profiles of the wavefront exhibited a dispersive nature, and the magnetosonic Mach number of the EUV wave derived from the highest intensity jump is about 1.4. In addition, triangulation indicates that the EUV wave propagated within a height range of about 60-100 Mm above the photosphere. We propose that the EUV wave observed should be a nonlinear fast-mode magnetosonic wave that propagated freely in the corona after it was driven by the CME expanding flanks during the initial period.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/evidence-for-the-wave-nature-of-an-extreme-ultraviolet-wave-observed-by-the-atmospheric-imaging-assembly-onboard-the-solar-dynamics-observatory/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Buildup of Magnetic Shear and Free Energy During Flux Emergence and Cancellation</title>
		<link>http://voxcharta.org/2012/05/16/buildup-of-magnetic-shear-and-free-energy-during-flux-emergence-and-cancellation/</link>
		<comments>http://voxcharta.org/2012/05/16/buildup-of-magnetic-shear-and-free-energy-during-flux-emergence-and-cancellation/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:40:49 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cancellation]]></category>
		<category><![CDATA[emergence]]></category>
		<category><![CDATA[energy flux]]></category>
		<category><![CDATA[filament]]></category>
		<category><![CDATA[flow velocity]]></category>
		<category><![CDATA[free energy]]></category>
		<category><![CDATA[inversion]]></category>
		<category><![CDATA[magnetic energy]]></category>
		<category><![CDATA[magnetic field line]]></category>
		<category><![CDATA[magnetic flux]]></category>
		<category><![CDATA[magnetic polarity]]></category>
		<category><![CDATA[magnetic shear]]></category>
		<category><![CDATA[mass ejection]]></category>
		<category><![CDATA[photosphere]]></category>
		<category><![CDATA[pil]]></category>
		<category><![CDATA[polarity]]></category>
		<category><![CDATA[reconnection]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[solar corona]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/buildup-of-magnetic-shear-and-free-energy-during-flux-emergence-and-cancellation/</guid>
		<description><![CDATA[We examine a simulation of flux emergence and cancellation, which shows a complex sequence of processes that accumulate free magnetic energy in the solar corona essential for the eruptive events such as coronal mass ejections (CMEs), filament eruptions and flares. The flow velocity at the surface and in the corona shows a consistent shearing pattern [...]]]></description>
			<content:encoded><![CDATA[<p>We examine a simulation of flux emergence and cancellation, which shows a complex sequence of processes that accumulate free magnetic energy in the solar corona essential for the eruptive events such as coronal mass ejections (CMEs), filament eruptions and flares. The flow velocity at the surface and in the corona shows a consistent shearing pattern along the polarity inversion line (PIL), which together with the rotation of the magnetic polarities, builds up the magnetic shear. Tether-cutting reconnection above the PIL then produces longer sheared magnetic field lines that extend higher into the corona, where a sigmoidal structure forms. Most significantly, reconnection and upward energy-flux transfer are found to occur even as magnetic flux is submerging and appears to cancel at the photosphere. A comparison of the simulated coronal field with the corresponding coronal potential field graphically shows the development of nonpotential fields during the emergence of the magnetic flux and formation of sunspots.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/buildup-of-magnetic-shear-and-free-energy-during-flux-emergence-and-cancellation/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>General relativistic simulations of black hole-neutron star mergers: Effects of magnetic fields [Replacement]</title>
		<link>http://voxcharta.org/2012/05/16/general-relativistic-simulations-of-black-hole-neutron-star-mergers-effects-of-magnetic-fields-replacement-3/</link>
		<comments>http://voxcharta.org/2012/05/16/general-relativistic-simulations-of-black-hole-neutron-star-mergers-effects-of-magnetic-fields-replacement-3/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:39:25 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[analyze this]]></category>
		<category><![CDATA[bhs]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[collimation]]></category>
		<category><![CDATA[disk formation]]></category>
		<category><![CDATA[disk mass]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[gravitational waveforms]]></category>
		<category><![CDATA[GRB]]></category>
		<category><![CDATA[ligo]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetic field configuration]]></category>
		<category><![CDATA[magnetic field line]]></category>
		<category><![CDATA[magnetohydrodynamic]]></category>
		<category><![CDATA[merger evolution]]></category>
		<category><![CDATA[neutron star mergers]]></category>
		<category><![CDATA[orbital angular momentum]]></category>
		<category><![CDATA[progenitor]]></category>
		<category><![CDATA[relativistic jet]]></category>
		<category><![CDATA[remnant]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/general-relativistic-simulations-of-black-hole-neutron-star-mergers-effects-of-magnetic-fields-replacement-3/</guid>
		<description><![CDATA[As a neutron star (NS) is tidally disrupted by a black hole (BH) companion at the end of a BH-NS binary inspiral, its magnetic fields will be stretched and amplified. If sufficiently strong, these magnetic fields may impact the gravitational waveforms, merger evolution and mass of the remnant disk. Formation of highly-collimated magnetic field lines [...]]]></description>
			<content:encoded><![CDATA[<p>As a neutron star (NS) is tidally disrupted by a black hole (BH) companion at the end of a BH-NS binary inspiral, its magnetic fields will be stretched and amplified. If sufficiently strong, these magnetic fields may impact the gravitational waveforms, merger evolution and mass of the remnant disk. Formation of highly-collimated magnetic field lines in the disk+spinning BH remnant may launch relativistic jets, providing the engine for a short-hard GRB. We analyze this scenario through fully general relativistic, magnetohydrodynamic (GRMHD) BHNS simulations from inspiral through merger and disk formation. Different initial magnetic field configurations and strengths are chosen for the NS interior for both nonspinning and moderately spinning (a/M=0.75) BHs aligned with the orbital angular momentum. Only strong interior (Bmax~10^17 G) initial magnetic fields in the NS significantly influence merger dynamics, enhancing the remnant disk mass by 100% and 40% in the nonspinning and spinning BH cases, respectively. However, detecting the imprint of even a strong magnetic field may be challenging for Advanced LIGO. Though there is no evidence of mass outflows or magnetic field collimation during the preliminary simulations we have performed, higher resolution, coupled with longer disk evolutions and different initial magnetic field configurations, may be required to definitively assess the possibility of BHNS binaries as short-hard GRB progenitors.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/general-relativistic-simulations-of-black-hole-neutron-star-mergers-effects-of-magnetic-fields-replacement-3/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>On the relativistic precession and oscillation frequencies of test particles around rapidly rotating compact stars [Replacement]</title>
		<link>http://voxcharta.org/2012/05/16/on-the-relativistic-precession-and-oscillation-frequencies-of-test-particles-around-rapidly-rotating-compact-stars-replacement/</link>
		<comments>http://voxcharta.org/2012/05/16/on-the-relativistic-precession-and-oscillation-frequencies-of-test-particles-around-rapidly-rotating-compact-stars-replacement/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:39:12 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[analytic model]]></category>
		<category><![CDATA[circular orbit]]></category>
		<category><![CDATA[compact star]]></category>
		<category><![CDATA[equation of state]]></category>
		<category><![CDATA[field equation]]></category>
		<category><![CDATA[isco]]></category>
		<category><![CDATA[mass x]]></category>
		<category><![CDATA[maxwell field]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[nuclear matter]]></category>
		<category><![CDATA[numerical solution]]></category>
		<category><![CDATA[oscillation frequency]]></category>
		<category><![CDATA[parametric solution]]></category>
		<category><![CDATA[periodic oscillation]]></category>
		<category><![CDATA[precession]]></category>
		<category><![CDATA[rapid rotation]]></category>
		<category><![CDATA[ray binaries]]></category>
		<category><![CDATA[relativistic astrophysics]]></category>
		<category><![CDATA[test particle]]></category>
		<category><![CDATA[vertical motion]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/on-the-relativistic-precession-and-oscillation-frequencies-of-test-particles-around-rapidly-rotating-compact-stars-replacement/</guid>
		<description><![CDATA[Whether analytic exact vacuum(electrovacuum) solutions of the Einstein(Einstein-Maxwell) field equations can accurately describe or not the exterior spacetime of compact stars remains still an interesting open question in Relativistic Astrophysics. As an attempt to establish their level of accuracy, the radii of the Innermost Stable Circular Orbits (ISCOs) of test particles given by analytic exterior [...]]]></description>
			<content:encoded><![CDATA[<p>Whether analytic exact vacuum(electrovacuum) solutions of the Einstein(Einstein-Maxwell) field equations can accurately describe or not the exterior spacetime of compact stars remains still an interesting open question in Relativistic Astrophysics. As an attempt to establish their level of accuracy, the radii of the Innermost Stable Circular Orbits (ISCOs) of test particles given by analytic exterior spacetime geometries have been compared with the ones given by numerical solutions for neutron stars (NSs) obeying a realistic equation of state (EoS). It has been so shown that the six-parametric solution of Pach\&#8217;on, Rueda, and Sanabria (2006) (hereafter PRS) is more accurate to describe the NS ISCO radii than other analytic models. We propose here an additional test of accuracy for analytic exterior geometries based on the comparison of orbital frequencies of neutral test particles. We compute the Keplerian, frame-dragging, as well as the precession and oscillation frequencies of the radial and vertical motions of neutral test particles for the Kerr and PRS geometries; then we compare them with the numerical values obtained by Morsink and Stella (1999) for realistic NSs. We identify the role of high-order multipole moments such as the mass quadrupole and current octupole in the determination of the orbital frequencies especially in the rapid rotation regime. The results of this work are relevant to cast a separatrix between black hole (BH) and NS signatures as well as probe the nuclear matter EoS and NS parameters from the Quasi-Periodic Oscillations (QPOs) observed in Low Mass X-Ray Binaries.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/on-the-relativistic-precession-and-oscillation-frequencies-of-test-particles-around-rapidly-rotating-compact-stars-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Dust-acoustic waves and stability in the permeating dusty plasma: I. Maxwellian distribution [Replacement]</title>
		<link>http://voxcharta.org/2012/05/16/dust-acoustic-waves-and-stability-in-the-permeating-dusty-plasma-i-maxwellian-distribution-replacement-3/</link>
		<comments>http://voxcharta.org/2012/05/16/dust-acoustic-waves-and-stability-in-the-permeating-dusty-plasma-i-maxwellian-distribution-replacement-3/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:37:26 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acoustic wave]]></category>
		<category><![CDATA[cometary plasma]]></category>
		<category><![CDATA[criterion]]></category>
		<category><![CDATA[dependence]]></category>
		<category><![CDATA[dusty plasma]]></category>
		<category><![CDATA[insight]]></category>
		<category><![CDATA[interplanetary space]]></category>
		<category><![CDATA[maxwellian velocity distribution]]></category>
		<category><![CDATA[numerical analyses]]></category>
		<category><![CDATA[phase velocity]]></category>
		<category><![CDATA[plasma tail]]></category>
		<category><![CDATA[space plasma]]></category>
		<category><![CDATA[wave frequency]]></category>
		<category><![CDATA[wave number]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/dust-acoustic-waves-and-stability-in-the-permeating-dusty-plasma-i-maxwellian-distribution-replacement-3/</guid>
		<description><![CDATA[The dust-acoustic waves and their stability in the permeating dusty plasma with the Maxwellian velocity distribution are investigated. We derive the dust-acoustic wave frequency and instability growth rate in two limiting physical cases that the thermal velocity of the flowing dusty plasma is (a) much larger than, and (b) much smaller than the phase velocity [...]]]></description>
			<content:encoded><![CDATA[<p>The dust-acoustic waves and their stability in the permeating dusty plasma with the Maxwellian velocity distribution are investigated. We derive the dust-acoustic wave frequency and instability growth rate in two limiting physical cases that the thermal velocity of the flowing dusty plasma is (a) much larger than, and (b) much smaller than the phase velocity of the waves. We find that the stability of the waves depend strongly on the velocity of the flowing dusty plasma in the permeating dusty plasma. The numerical analyses are made based on the example that a cometary plasma tail is passing through the interplanetary space plasma. We show that, in case (a), the waves are generally unstable for any flowing velocity, but in case (b), the waves become unstable only when the wave number is small and the flowing velocity is large. When the physical conditions are between these two limiting cases, we gain a strong insight into the dependence of the stability criterions on the physical conditions in the permeating dusty plasma.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/dust-acoustic-waves-and-stability-in-the-permeating-dusty-plasma-i-maxwellian-distribution-replacement-3/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Nonlinear wave propagation and reconnection at magnetic X-points in the Hall MHD regime [Replacement]</title>
		<link>http://voxcharta.org/2012/05/16/nonlinear-wave-propagation-and-reconnection-at-magnetic-x-points-in-the-hall-mhd-regime-replacement/</link>
		<comments>http://voxcharta.org/2012/05/16/nonlinear-wave-propagation-and-reconnection-at-magnetic-x-points-in-the-hall-mhd-regime-replacement/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:37:04 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[annulus]]></category>
		<category><![CDATA[coronal plasma]]></category>
		<category><![CDATA[dispersive nature]]></category>
		<category><![CDATA[dissipation]]></category>
		<category><![CDATA[energy release]]></category>
		<category><![CDATA[ion cyclotron]]></category>
		<category><![CDATA[key role]]></category>
		<category><![CDATA[lagrangian]]></category>
		<category><![CDATA[magnetic energy]]></category>
		<category><![CDATA[magnetic environment]]></category>
		<category><![CDATA[null point]]></category>
		<category><![CDATA[nulls]]></category>
		<category><![CDATA[reconnection]]></category>
		<category><![CDATA[resistivity]]></category>
		<category><![CDATA[skin depth]]></category>
		<category><![CDATA[solar atmosphere]]></category>
		<category><![CDATA[timescale]]></category>
		<category><![CDATA[topological features]]></category>
		<category><![CDATA[wave propagation]]></category>
		<category><![CDATA[whistler]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/nonlinear-wave-propagation-and-reconnection-at-magnetic-x-points-in-the-hall-mhd-regime-replacement/</guid>
		<description><![CDATA[The highly dynamical, complex nature of the solar atmosphere naturally implies the presence of waves in a topologically varied magnetic environment. Here, the interaction of waves with topological features such as null points is inevitable and potentially important for energetics. The low resistivity of the solar coronal plasma implies that non-MHD effects should be considered [...]]]></description>
			<content:encoded><![CDATA[<p>The highly dynamical, complex nature of the solar atmosphere naturally implies the presence of waves in a topologically varied magnetic environment. Here, the interaction of waves with topological features such as null points is inevitable and potentially important for energetics. The low resistivity of the solar coronal plasma implies that non-MHD effects should be considered in studies of magnetic energy release in this environment. This paper investigates the role of the Hall term in the propagation and dissipation of waves, their interaction with 2D magnetic X-points and the nature of the resulting reconnection. A Lagrangian remap shock-capturing code (Lare2d) is used to study the evolution of an initial fast magnetoacoustic wave annulus for a range of values of the ion skin depth in resistive Hall MHD. A magnetic null-point finding algorithm is also used to locate and track the evolution of the multiple null-points that are formed in the system. Depending on the ratio of ion skin depth to system size, our model demonstrates that Hall effects can play a key role in the wave-null interaction. In particular, the initial fast-wave pulse now consists of whistler and ion-cyclotron components; the dispersive nature of the whistler wave leads to (i) earlier interaction with the null, (ii) the creation of multiple additional, transient nulls and, hence, an increased number of energy release sites. In the Hall regime, the relevant timescales (such as the onset of reconnection and the period of the oscillatory relaxation) of the system are reduced significantly, and the reconnection rate is enhanced.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/nonlinear-wave-propagation-and-reconnection-at-magnetic-x-points-in-the-hall-mhd-regime-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Study of a Prominence Eruption using PROBA2/SWAP and STEREO/EUVI Data [Replacement]</title>
		<link>http://voxcharta.org/2012/05/16/study-of-a-prominence-eruption-using-proba2swap-and-stereoeuvi-data-replacement/</link>
		<comments>http://voxcharta.org/2012/05/16/study-of-a-prominence-eruption-using-proba2swap-and-stereoeuvi-data-replacement/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:34:30 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[13 april]]></category>
		<category><![CDATA[acceleration]]></category>
		<category><![CDATA[coronal magnetic field]]></category>
		<category><![CDATA[degrees of freedom]]></category>
		<category><![CDATA[eruptive prominence]]></category>
		<category><![CDATA[first model]]></category>
		<category><![CDATA[five degrees]]></category>
		<category><![CDATA[images]]></category>
		<category><![CDATA[mathematical model]]></category>
		<category><![CDATA[polynomial function]]></category>
		<category><![CDATA[prominence]]></category>
		<category><![CDATA[propagation]]></category>
		<category><![CDATA[reconnection]]></category>
		<category><![CDATA[relaxation]]></category>
		<category><![CDATA[spacecraft]]></category>
		<category><![CDATA[spline]]></category>
		<category><![CDATA[true direction]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/study-of-a-prominence-eruption-using-proba2swap-and-stereoeuvi-data-replacement/</guid>
		<description><![CDATA[Observations of the early rise and propagation phases of solar eruptive prominences can provide clues about the forces acting on them through the behavior of their acceleration with height. We have analyzed such an event, observed on 13 April 2010 by SWAP on PROBA2 and EUVI on STEREO. A feature at the top of the [...]]]></description>
			<content:encoded><![CDATA[<p>Observations of the early rise and propagation phases of solar eruptive prominences can provide clues about the forces acting on them through the behavior of their acceleration with height. We have analyzed such an event, observed on 13 April 2010 by SWAP on PROBA2 and EUVI on STEREO. A feature at the top of the erupting prominence was identified and tracked in images from the three spacecraft. The triangulation technique was used to derive the true direction of propagation of this feature. The reconstructed points were fitted with two mathematical models: i) a power-law polynomial function and ii) a cubic smoothing spline, in order to derive the accelerations. The first model is characterized by five degrees of freedom while the second one is characterized by ten degrees of freedom. The results show that the acceleration increases smoothly and it is continuously increasing with height. We conclude that the prominence is not accelerated immediately by local reconnection but rather is swept away as part of a large-scale relaxation of the coronal magnetic field.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/study-of-a-prominence-eruption-using-proba2swap-and-stereoeuvi-data-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Propagating Disturbances in Coronal Loops: A Detailed Analysis of Propagation Speeds [Replacement]</title>
		<link>http://voxcharta.org/2012/05/16/propagating-disturbances-in-coronal-loops-a-detailed-analysis-of-propagation-speeds-replacement/</link>
		<comments>http://voxcharta.org/2012/05/16/propagating-disturbances-in-coronal-loops-a-detailed-analysis-of-propagation-speeds-replacement/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:33:46 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[aia]]></category>
		<category><![CDATA[asymmetry]]></category>
		<category><![CDATA[coronal]]></category>
		<category><![CDATA[doppler velocity]]></category>
		<category><![CDATA[intensity]]></category>
		<category><![CDATA[observatory]]></category>
		<category><![CDATA[outer solar atmosphere]]></category>
		<category><![CDATA[periodic disturbances]]></category>
		<category><![CDATA[propagation]]></category>
		<category><![CDATA[regions of the sun]]></category>
		<category><![CDATA[schrijver]]></category>
		<category><![CDATA[sunspot]]></category>
		<category><![CDATA[sunspot region]]></category>
		<category><![CDATA[temperature dependence]]></category>
		<category><![CDATA[velocities]]></category>
		<category><![CDATA[wave]]></category>
		<category><![CDATA[wavelength]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/propagating-disturbances-in-coronal-loops-a-detailed-analysis-of-propagation-speeds-replacement/</guid>
		<description><![CDATA[Quasi-periodic disturbances have been observed in the outer solar atmosphere for many years now. Although first interpreted as upflows (Schrijver et al. (1999)), they have been widely regarded as slow magnetoacoustic waves, due to observed velocities and periods. However, recent observations have questioned this interpretation, as periodic disturbances in Doppler velocity, line width and profile [...]]]></description>
			<content:encoded><![CDATA[<p>Quasi-periodic disturbances have been observed in the outer solar atmosphere for many years now. Although first interpreted as upflows (Schrijver et al. (1999)), they have been widely regarded as slow magnetoacoustic waves, due to observed velocities and periods. However, recent observations have questioned this interpretation, as periodic disturbances in Doppler velocity, line width and profile asymmetry were found to be in phase with the intensity oscillations (De Pontieu et al. (2010),Tian1 et al. (2011))}, suggesting the disturbances could be quasi-periodic upflows. Here we conduct a detailed analysis of the velocities of these disturbances across several wavelengths using the Atmospheric Imaging Assembly (AIA) on board the Solar Dynamics Observatory (SDO). We analysed 41 examples, including both sunspot and non sunspot regions of the Sun. We found that the velocities of propagating disturbances (PDs) located at sunspots are more likely to be temperature dependent, whereas the velocities of PDs at non sunspot locations do not show a clear temperature dependence. We also considered on what scale the underlying driver is affecting the properties of the PDs. Finally, we found that removing the contribution due to the cooler ions in the 193 A wavelength suggests that a substantial part of the 193 emission of sunspot PDs can be contributed to the cool component of 193\AA.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/propagating-disturbances-in-coronal-loops-a-detailed-analysis-of-propagation-speeds-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Particle-In-Cell Simulation of Electron Acceleration in Solar Coronal Jets [Replacement]</title>
		<link>http://voxcharta.org/2012/05/16/particle-in-cell-simulation-of-electron-acceleration-in-solar-coronal-jets-replacement/</link>
		<comments>http://voxcharta.org/2012/05/16/particle-in-cell-simulation-of-electron-acceleration-in-solar-coronal-jets-replacement/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:31:06 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration mechanism]]></category>
		<category><![CDATA[boundary condition]]></category>
		<category><![CDATA[cell simulation]]></category>
		<category><![CDATA[cells]]></category>
		<category><![CDATA[current sheet]]></category>
		<category><![CDATA[electric current]]></category>
		<category><![CDATA[electron]]></category>
		<category><![CDATA[electron acceleration]]></category>
		<category><![CDATA[investigations]]></category>
		<category><![CDATA[jets]]></category>
		<category><![CDATA[losses]]></category>
		<category><![CDATA[magnetic flux rope]]></category>
		<category><![CDATA[magnetic reconnection]]></category>
		<category><![CDATA[mesh refinement]]></category>
		<category><![CDATA[mhd simulation]]></category>
		<category><![CDATA[numerical resolution]]></category>
		<category><![CDATA[open magnetic field]]></category>
		<category><![CDATA[particle acceleration]]></category>
		<category><![CDATA[snapshot]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/particle-in-cell-simulation-of-electron-acceleration-in-solar-coronal-jets-replacement/</guid>
		<description><![CDATA[We investigate electron acceleration resulting from 3D magnetic reconnection between an emerging, twisted magnetic flux rope and a pre-existing weak, open magnetic field. We first follow the rise of an unstable, twisted flux tube with a resistive MHD simulation where the numerical resolution is enhanced by using fixed mesh refinement. As in previous MHD investigations [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate electron acceleration resulting from 3D magnetic reconnection between an emerging, twisted magnetic flux rope and a pre-existing weak, open magnetic field. We first follow the rise of an unstable, twisted flux tube with a resistive MHD simulation where the numerical resolution is enhanced by using fixed mesh refinement. As in previous MHD investigations of similar situations the rise of the flux tube into the pre-existing inclined coronal magnetic field results in the formation of a solar coronal jet. A snapshot of the MHD model is then used as an initial and boundary condition for a particle-in-cell simulation, using up to half a billion cells and over 20 billion charged particle. Particle acceleration occurs mainly in the reconnection current sheet, with accelerated electrons displaying a power law dN/dE distribution with an index of about -1.65. The main acceleration mechanism is a systematic electric field, striving to maintaining the electric current in the current sheet against losses caused by electrons not being able to stay in the current sheet for more than a few seconds at a time.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/particle-in-cell-simulation-of-electron-acceleration-in-solar-coronal-jets-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>High-Contrast NIR Polarization Imaging of MWC480</title>
		<link>http://voxcharta.org/2012/05/15/high-contrast-nir-polarization-imaging-of-mwc480/</link>
		<comments>http://voxcharta.org/2012/05/15/high-contrast-nir-polarization-imaging-of-mwc480/#comments</comments>
		<pubDate>Wed, 16 May 2012 01:06:57 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[differential]]></category>
		<category><![CDATA[dust disk]]></category>
		<category><![CDATA[giant planet]]></category>
		<category><![CDATA[grain growth]]></category>
		<category><![CDATA[herbig]]></category>
		<category><![CDATA[high contrast]]></category>
		<category><![CDATA[hst nicmos]]></category>
		<category><![CDATA[literature]]></category>
		<category><![CDATA[measures]]></category>
		<category><![CDATA[polarization]]></category>
		<category><![CDATA[radius]]></category>
		<category><![CDATA[scattered light]]></category>
		<category><![CDATA[signature]]></category>
		<category><![CDATA[spectral energy distribution]]></category>
		<category><![CDATA[subaru]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/high-contrast-nir-polarization-imaging-of-mwc480/</guid>
		<description><![CDATA[One of the key predictions of modeling from the IR excess of Herbig Ae stars is that for protoplanetary disks, where significant grain growth and settling has occurred, the dust disk has flattened to the point that it can be partially or largely shadowed by the innermost material at or near the dust sublimation radius. [...]]]></description>
			<content:encoded><![CDATA[<p>One of the key predictions of modeling from the IR excess of Herbig Ae stars is that for protoplanetary disks, where significant grain growth and settling has occurred, the dust disk has flattened to the point that it can be partially or largely shadowed by the innermost material at or near the dust sublimation radius. When the self-shadowing has already started, the outer disk is expected to be detected in scattered light only in the exceptional cases that the scale height of the dust disk at the sublimation radius is smaller than usual. High-contrast imaging combined with the IR spectral energy distribution allow us to measure the degree of flattening of the disk, as well as to determine the properties of the outer disk. We present polarimetric differential imaging in $H$ band obtained with Subaru/HiCIAO of one such system, MWC 480. The HiCIAO data were obtained at a historic minimum of the NIR excess. The disk is detected in scattered light from 0\farcs2-1\farcs0 (27.4-137AU). Together with the marginal detection of the disk from 1998 February 24 by HST/NICMOS, our data constrain the opening half angle for the disk to lie between 1.3$\leq\theta\leq 2.2^\circ$. When compared with similar measures in CO for the gas disk from the literature, the dust disk subtends only $\sim$30% of the gas disk scale height (H/R$\sim$0.03). Such a dust disk is a factor of 5-7 flatter than transitional disks, which have structural signatures that giant planets have formed.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/high-contrast-nir-polarization-imaging-of-mwc480/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Violation of Chandrasekhar Mass Limit: The Exciting Potential of Strongly Magnetized White Dwarfs</title>
		<link>http://voxcharta.org/2012/05/15/violation-of-chandrasekhar-mass-limit-the-exciting-potential-of-strongly-magnetized-white-dwarfs/</link>
		<comments>http://voxcharta.org/2012/05/15/violation-of-chandrasekhar-mass-limit-the-exciting-potential-of-strongly-magnetized-white-dwarfs/#comments</comments>
		<pubDate>Wed, 16 May 2012 01:06:33 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[chandrasekhar mass]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[electron]]></category>
		<category><![CDATA[electron gas]]></category>
		<category><![CDATA[equation of state]]></category>
		<category><![CDATA[existence]]></category>
		<category><![CDATA[landau level]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[mass limit]]></category>
		<category><![CDATA[mass radius]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[quantization]]></category>
		<category><![CDATA[Sun]]></category>
		<category><![CDATA[white dwarf]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/violation-of-chandrasekhar-mass-limit-the-exciting-potential-of-strongly-magnetized-white-dwarfs/</guid>
		<description><![CDATA[We consider a relativistic, degenerate, electron gas under the influence of a strong magnetic field, which describes magnetized white dwarfs. Landau quantization changes the density of states available to the electrons, thus modifying the underlying equation of state. In the presence of very strong magnetic fields a maximum of either one, two or three Landau [...]]]></description>
			<content:encoded><![CDATA[<p>We consider a relativistic, degenerate, electron gas under the influence of a strong magnetic field, which describes magnetized white dwarfs. Landau quantization changes the density of states available to the electrons, thus modifying the underlying equation of state. In the presence of very strong magnetic fields a maximum of either one, two or three Landau level(s) is/are occupied. We obtain the mass-radius relations for such white dwarfs and their detailed investigation leads us to propose the existence of white dwarfs having a mass ~2.3M_Sun, which overwhelmingly exceeds the Chandrasekhar mass limit.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/violation-of-chandrasekhar-mass-limit-the-exciting-potential-of-strongly-magnetized-white-dwarfs/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The bipolar outflow and disk of the brown dwarf ISO217</title>
		<link>http://voxcharta.org/2012/05/15/the-bipolar-outflow-and-disk-of-the-brown-dwarf-iso217/</link>
		<comments>http://voxcharta.org/2012/05/15/the-bipolar-outflow-and-disk-of-the-brown-dwarf-iso217/#comments</comments>
		<pubDate>Wed, 16 May 2012 01:05:00 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion disk]]></category>
		<category><![CDATA[astrometry]]></category>
		<category><![CDATA[asymmetry]]></category>
		<category><![CDATA[brown dwarf]]></category>
		<category><![CDATA[brown dwarf candidate]]></category>
		<category><![CDATA[disk inclination]]></category>
		<category><![CDATA[disk mass]]></category>
		<category><![CDATA[disk model]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[grain growth]]></category>
		<category><![CDATA[herschel]]></category>
		<category><![CDATA[inclination angle]]></category>
		<category><![CDATA[lobes]]></category>
		<category><![CDATA[msun]]></category>
		<category><![CDATA[outflow]]></category>
		<category><![CDATA[pac]]></category>
		<category><![CDATA[spatial extension]]></category>
		<category><![CDATA[t tauri]]></category>
		<category><![CDATA[vlt spectra]]></category>
		<category><![CDATA[whelan]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/the-bipolar-outflow-and-disk-of-the-brown-dwarf-iso217/</guid>
		<description><![CDATA[We show that the very young brown dwarf candidate ISO217 (M6.25) is driving an intrinsically asymmetric bipolar outflow with a stronger and slightly faster red-shifted component based on spectro-astrometry of forbidden [SII] emission lines observed in UVES/VLT spectra taken in 2009. ISO217 is only one out of a handful of brown dwarfs and VLMS (M5-M8) [...]]]></description>
			<content:encoded><![CDATA[<p>We show that the very young brown dwarf candidate ISO217 (M6.25) is driving an intrinsically asymmetric bipolar outflow with a stronger and slightly faster red-shifted component based on spectro-astrometry of forbidden [SII] emission lines observed in UVES/VLT spectra taken in 2009. ISO217 is only one out of a handful of brown dwarfs and VLMS (M5-M8) for which the existence of an outflow has been detected and which show that the T Tauri phase continues at the substellar limit. We measure a spatial extension of the outflow of +/-190mas (+/-30AU) and velocities of +/-40-50kms/s. We show that the strong velocity asymmetry between both lobes of a factor of 2 found in 2007 by Whelan et al. might be smaller than originally anticipated and likely evolves over a period of a few years. We detect also forbidden [FeII]7155 emission, which could potentially originate at the hot inner region of the outflow. To understand the ISO217 system, we have determined the properties of its accretion disk based on radiative transfer modeling of the SED. Our disk model is in very good agreement with Herschel/PACS data at 70mu. We find that the disk is flared and intermediately inclined (~45deg). The total disk mass (4e-6 Msun) is small compared to the accretion and outflow rate of ISO217 (~1e-10 Msun/yr). We suggest to explain this discrepancy by either a larger disk mass than inferred from the model (strong undetected grain growth) and/or by an on average lower accretion and outflow rate than the determined values. We show that a disk inclination significantly exceeding 45deg, as suggested from Halpha modeling and from the fact that both lobes of the outflow are visible, is not consistent with the SED data. Thus, despite its intermediate inclination angle, the disk of this brown dwarf appears to not obscure the red outflow component in [SII], which is very rarely seen for T Tauri objects (only one other case).</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/the-bipolar-outflow-and-disk-of-the-brown-dwarf-iso217/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>The Absence of Ex-Companions in Type Ia Supernova Remnants</title>
		<link>http://voxcharta.org/2012/05/15/the-absence-of-ex-companions-in-type-ia-supernova-remnants/</link>
		<comments>http://voxcharta.org/2012/05/15/the-absence-of-ex-companions-in-type-ia-supernova-remnants/#comments</comments>
		<pubDate>Wed, 16 May 2012 01:04:33 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[100 000 years]]></category>
		<category><![CDATA[absence]]></category>
		<category><![CDATA[acceleration]]></category>
		<category><![CDATA[angular momentum]]></category>
		<category><![CDATA[companion]]></category>
		<category><![CDATA[companion star]]></category>
		<category><![CDATA[deep imaging]]></category>
		<category><![CDATA[exact nature]]></category>
		<category><![CDATA[explosion images]]></category>
		<category><![CDATA[large magellanic cloud]]></category>
		<category><![CDATA[natures]]></category>
		<category><![CDATA[probes]]></category>
		<category><![CDATA[progenitor]]></category>
		<category><![CDATA[remnant]]></category>
		<category><![CDATA[SNe]]></category>
		<category><![CDATA[supernova remnant]]></category>
		<category><![CDATA[systematic uncertainty]]></category>
		<category><![CDATA[type ia]]></category>
		<category><![CDATA[white dwarf]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/the-absence-of-ex-companions-in-type-ia-supernova-remnants/</guid>
		<description><![CDATA[Type Ia supernovae (SNe Ia) play important roles in our study of the expansion and acceleration of the Universe, but because we do not know the exact nature or natures of the progenitors, there is a systematic uncertainty that must be resolved if SNe Ia are to become more precise cosmic probes. No progenitor system [...]]]></description>
			<content:encoded><![CDATA[<p>Type Ia supernovae (SNe Ia) play important roles in our study of the expansion and acceleration of the Universe, but because we do not know the exact nature or natures of the progenitors, there is a systematic uncertainty that must be resolved if SNe Ia are to become more precise cosmic probes. No progenitor system has ever been identified either in the pre- or post-explosion images of a Ia event. There have been recent claims for and against the detection of ex-companion stars in several SNe Ia remnants. These studies, however, usually ignore the angular momentum gain of the progenitor white dwarf, which leads to a spin-up phase and a subsequent spin-down phase before explosion. For spin-down timescales greater than 100,000 years, the donor star could be too dim to detect by the time of explosion. Here we revisit the current limits on ex-companion stars to SNR 0509-67.5, a 400 year old remnant in the Large Magellanic Cloud. If the effects of possible angular momentum gain on the white dwarf are included, a wide range of single-degenerate progenitor models are allowed for this remnant. We demonstrate that the current absence of evidence for ex-companion stars in this remnant, as well as other SNe Ia remnants, does not necessarily provide the evidence of absence for ex-companions. We discuss potential ways to identify such ex-companion stars through deep imaging observations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/the-absence-of-ex-companions-in-type-ia-supernova-remnants/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Non-local thermodynamic equilibrium inversions from a 3D MHD chromospheric model</title>
		<link>http://voxcharta.org/2012/05/15/non-local-thermodynamic-equilibrium-inversions-from-a-3d-mhd-chromospheric-model/</link>
		<comments>http://voxcharta.org/2012/05/15/non-local-thermodynamic-equilibrium-inversions-from-a-3d-mhd-chromospheric-model/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:59:36 +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[3d mhd]]></category>
		<category><![CDATA[atomic level]]></category>
		<category><![CDATA[diagnostic capability]]></category>
		<category><![CDATA[gaussian noise]]></category>
		<category><![CDATA[inversion]]></category>
		<category><![CDATA[inversion code]]></category>
		<category><![CDATA[inversion method]]></category>
		<category><![CDATA[inversion technique]]></category>
		<category><![CDATA[level populations]]></category>
		<category><![CDATA[line profile]]></category>
		<category><![CDATA[linear polarization]]></category>
		<category><![CDATA[magnetic field line]]></category>
		<category><![CDATA[model atmosphere]]></category>
		<category><![CDATA[original model]]></category>
		<category><![CDATA[photon flux]]></category>
		<category><![CDATA[quiet sun]]></category>
		<category><![CDATA[solar atmosphere]]></category>
		<category><![CDATA[solar chromosphere]]></category>
		<category><![CDATA[thermodynamic equilibrium]]></category>
		<category><![CDATA[zeeman effect]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/non-local-thermodynamic-equilibrium-inversions-from-a-3d-mhd-chromospheric-model/</guid>
		<description><![CDATA[The structure of the solar chromosphere is believed to be governed by magnetic fields, even in quiet-Sun regions that have a relatively weak photospheric field. During the past decade inversion methods have emerged as powerful tools for analyzing the chromosphere of active regions. The applicability of inversions to infer the stratification of the physical conditions [...]]]></description>
			<content:encoded><![CDATA[<p>The structure of the solar chromosphere is believed to be governed by magnetic fields, even in quiet-Sun regions that have a relatively weak photospheric field. During the past decade inversion methods have emerged as powerful tools for analyzing the chromosphere of active regions. The applicability of inversions to infer the stratification of the physical conditions in a dynamic 3D solar chromosphere has not yet been studied in detail.   This study aims to establish the diagnostic capabilities of non-local thermodynamical equilibrium (NLTE) inversion techniques of Stokes profiles induced by the Zeeman effect in the Ca II 8542 line.   We computed the Ca II atomic level populations in a snapshot from a 3D radiation-MHD simulation of the quiet solar atmosphere in non-LTE using the 3D radiative transfer code Multi3d. These populations were used to compute synthetic full-Stokes profiles in the Ca II 8542 line using 1.5D radiative transfer and the inversion code Nicole. The profiles were then spectrally degraded to account for finite filter width and Gaussian noise was added to account for finite photon flux. These profiles were inverted using Nicole and the results were compared with the original model atmosphere.   Our NLTE inversions applied to quiet-Sun synthetic observations provide reasonably good estimates of the chromospheric magnetic field, line-of-sight velocities and somewhat less accurate, but still very useful, estimates of the temperature. Three dimensional scattering of photons cause cool pockets in the chromosphere to be invisible in the line profile and consequently they are also not recovered by the inversions. To successfully detect Stokes linear polarization in this quiet snapshot, a noise level below 10^{-3.5} is necessary.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/non-local-thermodynamic-equilibrium-inversions-from-a-3d-mhd-chromospheric-model/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Diagnosing small- and large-scale structure in the winds of hot, massive OB-star</title>
		<link>http://voxcharta.org/2012/05/15/diagnosing-small-and-large-scale-structure-in-the-winds-of-hot-massive-ob-star/</link>
		<comments>http://voxcharta.org/2012/05/15/diagnosing-small-and-large-scale-structure-in-the-winds-of-hot-massive-ob-star/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:53:24 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[balmer]]></category>
		<category><![CDATA[consequence]]></category>
		<category><![CDATA[estimates]]></category>
		<category><![CDATA[line emission]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magneto]]></category>
		<category><![CDATA[mass loss rates]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[o star]]></category>
		<category><![CDATA[outflow]]></category>
		<category><![CDATA[radiative transfer]]></category>
		<category><![CDATA[scale structure]]></category>
		<category><![CDATA[scale wind]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[spatial scale]]></category>
		<category><![CDATA[spectral diagnostics]]></category>
		<category><![CDATA[subset]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/diagnosing-small-and-large-scale-structure-in-the-winds-of-hot-massive-ob-star/</guid>
		<description><![CDATA[It is observationally as well as theoretically well established that the winds of hot, massive OB-stars are highly structured on a broad range of spatial scales. This paper first discusses consequences of the small-scale structures associated with the strong instability inherent to the line-driving of these winds. We demonstrate the importance of a proper treatment [...]]]></description>
			<content:encoded><![CDATA[<p>It is observationally as well as theoretically well established that the winds of hot, massive OB-stars are highly structured on a broad range of spatial scales. This paper first discusses consequences of the small-scale structures associated with the strong instability inherent to the line-driving of these winds. We demonstrate the importance of a proper treatment of such wind clumping to obtain reliable estimates of mass-loss rates, and also show that instability simulations that are perturbed at the lower boundary indeed display significant clumping quite close to the wind base, in general agreement with observations. But a growing subset of massive stars has also been found to possess strong surface magnetic fields, which may channel the star&#8217;s outflow and induce also large-scale wind structures and cyclic behavior of spectral diagnostics. The paper concludes by showing that multi-dimensional, magneto-hydrodynamical wind simulations, together with detailed radiative-transfer modeling, can reproduce remarkably well the periodic Balmer line emission observed in slowly rotating magnetic O stars like HD191612.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/diagnosing-small-and-large-scale-structure-in-the-winds-of-hot-massive-ob-star/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Rapid Disappearance of Penumbra-Like Features Near a Flaring Polarity Inversion Line: The Hinode Observations</title>
		<link>http://voxcharta.org/2012/05/15/rapid-disappearance-of-penumbra-like-features-near-a-flaring-polarity-inversion-line-the-hinode-observations/</link>
		<comments>http://voxcharta.org/2012/05/15/rapid-disappearance-of-penumbra-like-features-near-a-flaring-polarity-inversion-line-the-hinode-observations/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:48:21 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[class flare]]></category>
		<category><![CDATA[inversion]]></category>
		<category><![CDATA[lct]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[moat]]></category>
		<category><![CDATA[morphology]]></category>
		<category><![CDATA[penumbra]]></category>
		<category><![CDATA[pil]]></category>
		<category><![CDATA[polarity]]></category>
		<category><![CDATA[pore]]></category>
		<category><![CDATA[rapid disappearance]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[region noaa]]></category>
		<category><![CDATA[spatial correlation]]></category>
		<category><![CDATA[spectro]]></category>
		<category><![CDATA[submergence]]></category>
		<category><![CDATA[sunspot]]></category>
		<category><![CDATA[vertical component]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/rapid-disappearance-of-penumbra-like-features-near-a-flaring-polarity-inversion-line-the-hinode-observations/</guid>
		<description><![CDATA[We present the observations of penumbra like features (PLFs) near a polarity inversion line (PIL) of flaring region. The PIL is located at the moat boundary of active region (NOAA 10960). The PLFs appear similar to sunspot penumbrae in morphology but occupy small area, about 6$\times10^{7}$ km$^{2}$, and are not associated with sunspot or pore. [...]]]></description>
			<content:encoded><![CDATA[<p>We present the observations of penumbra like features (PLFs) near a polarity inversion line (PIL) of flaring region. The PIL is located at the moat boundary of active region (NOAA 10960). The PLFs appear similar to sunspot penumbrae in morphology but occupy small area, about 6$\times10^{7}$ km$^{2}$, and are not associated with sunspot or pore. We observed a rapid disappearance of the PLFs after a C1.7 class flare, which occurred close to the PIL. The local correlation tracking (LCT) of these features shows presence of horizontal flows directed away from the end-points of the PLFs, similar to the radial outward flow found around regular sunspots, which is also known as the moat flow. Hard X-ray emission, coincident with the location of the PLFs, is found in RHESSI observations, suggesting a spatial correlation between the occurrence of the flare and decay of the PLFs. Vector magnetic field derived from the observations obtained by Hinode spectro-polarimeter SOT/SP instrument, before and after the flare, shows a significant change in the horizontal as well as the vertical component of the field, after the flare. The weakening of both the components of the magnetic field in the flare interval suggests that rapid cancellation and/or submergence of the magnetic field in PLFs occurred during the flare interval.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/rapid-disappearance-of-penumbra-like-features-near-a-flaring-polarity-inversion-line-the-hinode-observations/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Resolving the Circumstellar Disk Around the Massive Protostar Driving the HH 80-81 Jet</title>
		<link>http://voxcharta.org/2012/05/15/resolving-the-circumstellar-disk-around-the-massive-protostar-driving-the-hh-80-81-jet/</link>
		<comments>http://voxcharta.org/2012/05/15/resolving-the-circumstellar-disk-around-the-massive-protostar-driving-the-hh-80-81-jet/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:46:17 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion disk]]></category>
		<category><![CDATA[continuum emission]]></category>
		<category><![CDATA[dust emission]]></category>
		<category><![CDATA[high angular resolution]]></category>
		<category><![CDATA[ira]]></category>
		<category><![CDATA[micron]]></category>
		<category><![CDATA[molecule]]></category>
		<category><![CDATA[morphology]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[protostar]]></category>
		<category><![CDATA[radio jet]]></category>
		<category><![CDATA[radius]]></category>
		<category><![CDATA[resolution observations]]></category>
		<category><![CDATA[resolutions]]></category>
		<category><![CDATA[scales]]></category>
		<category><![CDATA[submillimeter array]]></category>
		<category><![CDATA[submillimeter observations]]></category>
		<category><![CDATA[subtraction]]></category>
		<category><![CDATA[sulfur oxide]]></category>
		<category><![CDATA[very large array]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/resolving-the-circumstellar-disk-around-the-massive-protostar-driving-the-hh-80-81-jet/</guid>
		<description><![CDATA[We present new high-angular resolution observations toward the driving source of the HH 80-81 jet (IRAS 18162-2048). Continuum emission was observed with the Very Large Array at 7 mm and 1.3 cm, and with the Submillimeter Array at 860 microns, with angular resolutions of ~0&#8243;1 and ~0&#8243;8 respectively. Submillimeter observations of the sulfur oxide (SO) [...]]]></description>
			<content:encoded><![CDATA[<p>We present new high-angular resolution observations toward the driving source of the HH 80-81 jet (IRAS 18162-2048). Continuum emission was observed with the Very Large Array at 7 mm and 1.3 cm, and with the Submillimeter Array at 860 microns, with angular resolutions of ~0&#8243;1 and ~0&#8243;8 respectively. Submillimeter observations of the sulfur oxide (SO) molecule are reported as well. At 1.3 cm the emission traces the well-known radio jet, while at 7 mm the continuum morphology is quadrupolar and seems to be produced by a combination of free-free and dust emission. An elongated structure perpendicular to the jet remains in the 7 mm image after subtraction of the free-free contribution. This structure is interpreted as a compact accretion disk of ~200 AU radius. Our interpretation is favored by the presence of rotation in our SO observations observed at larger scales. The observations presented here add to the small list of cases where the hundred-AU scale emission from a circumstellar disk around a massive protostar has been resolved.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/resolving-the-circumstellar-disk-around-the-massive-protostar-driving-the-hh-80-81-jet/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>9 Sgr: uncovering an O-type spectroscopic binary with an 8.6 year period</title>
		<link>http://voxcharta.org/2012/05/15/9-sgr-uncovering-an-o-type-spectroscopic-binary-with-an-8-6-year-period/</link>
		<comments>http://voxcharta.org/2012/05/15/9-sgr-uncovering-an-o-type-spectroscopic-binary-with-an-8-6-year-period/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:45:12 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[binary system]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[interaction zone]]></category>
		<category><![CDATA[manifestation]]></category>
		<category><![CDATA[multiplicity]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[paradigm]]></category>
		<category><![CDATA[radial velocity]]></category>
		<category><![CDATA[radio emission]]></category>
		<category><![CDATA[search method]]></category>
		<category><![CDATA[SGR]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[type star]]></category>
		<category><![CDATA[wind interaction]]></category>
		<category><![CDATA[wind wind]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/9-sgr-uncovering-an-o-type-spectroscopic-binary-with-an-8-6-year-period/</guid>
		<description><![CDATA[The O-type object 9 Sgr is a well-known synchrotron radio emitter. This feature is usually attributed to colliding-wind binary systems, but 9 Sgr was long considered a single star. We have conducted a long-term spectroscopic monitoring of this star to investigate its multiplicity and search for evidence for wind-wind interactions. Radial velocities are determined and [...]]]></description>
			<content:encoded><![CDATA[<p>The O-type object 9 Sgr is a well-known synchrotron radio emitter. This feature is usually attributed to colliding-wind binary systems, but 9 Sgr was long considered a single star. We have conducted a long-term spectroscopic monitoring of this star to investigate its multiplicity and search for evidence for wind-wind interactions. Radial velocities are determined and analysed using various period search methods. Spectral disentangling is applied to separate the spectra of the components of the binary system. We derive the first ever orbital solution of 9 Sgr. The system is found to consist of an O3.5 V((f+)) primary and an O5- 5.5 V((f)) secondary moving around each other on a highly eccentric (e = 0.7), 8.6 year orbit. The spectra reveal no variable emission lines that could be formed in the wind interaction zone in agreement with the expected properties of the interaction in such a wide system. Our results provide further support to the paradigm of synchrotron radio emission from early-type stars being a manifestation of interacting winds in a binary system.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/9-sgr-uncovering-an-o-type-spectroscopic-binary-with-an-8-6-year-period/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Superluminous Light Curves from Supernovae Exploding in a Dense Wind</title>
		<link>http://voxcharta.org/2012/05/15/superluminous-light-curves-from-supernovae-exploding-in-a-dense-wind/</link>
		<comments>http://voxcharta.org/2012/05/15/superluminous-light-curves-from-supernovae-exploding-in-a-dense-wind/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:38:06 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[circumstellar material]]></category>
		<category><![CDATA[core collapse]]></category>
		<category><![CDATA[diffusion model]]></category>
		<category><![CDATA[kinetic energy]]></category>
		<category><![CDATA[last decade]]></category>
		<category><![CDATA[light curve]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[peak luminosity]]></category>
		<category><![CDATA[progenitor]]></category>
		<category><![CDATA[qualitative behavior]]></category>
		<category><![CDATA[radiated energy]]></category>
		<category><![CDATA[sn 2006gy]]></category>
		<category><![CDATA[SNe]]></category>
		<category><![CDATA[steady wind]]></category>
		<category><![CDATA[subclass]]></category>
		<category><![CDATA[Supernova]]></category>
		<category><![CDATA[supernovae]]></category>
		<category><![CDATA[wind observations]]></category>
		<category><![CDATA[wind parameters]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/superluminous-light-curves-from-supernovae-exploding-in-a-dense-wind/</guid>
		<description><![CDATA[Observations from the last decade have indicated the existence of a general class of superluminous supernovae (SLSNe), in which the peak luminosity exceeds 10^{44} erg/s. Here we focus on a subclass of these events, where the light curve is also tens of days wide, so the total radiated energy is order 10^{51} erg. If the [...]]]></description>
			<content:encoded><![CDATA[<p>Observations from the last decade have indicated the existence of a general class of superluminous supernovae (SLSNe), in which the peak luminosity exceeds 10^{44} erg/s. Here we focus on a subclass of these events, where the light curve is also tens of days wide, so the total radiated energy is order 10^{51} erg. If the origin of these SLSNe is a core-collapse-driven explosion of a massive star, then the mechanism which converts the explosion energy into radiation must be very efficient (much more than in typical core collapse SNe, where this efficiency is of order one percent). We examine the scenario where the radiated luminosity is due to efficient conversion of kinetic energy of the ejected stellar envelope into radiation by interaction with an optically thick, pre-existing circumstellar material (CSM), presumably the product of a steady wind from the progenitor. We base the analysis on a simple, numerically solved, hydrodynamic diffusion model, which allows us to identify the qualitative behavior of the observable light curves, and to relate them to the parameters of the wind. We specifically show that a wide and superluminous supernova requires the mass of the relevant wind material to be comparable to that of ejected material from the exploding progenitor. We find the wind parameters which explain the peak luminosity and width of the bolometric light curves of three particular SLSNe, namely, SN 2005ap, SN 2006gy, and SN 2010gx, and show that they are best fitted with a wind that extends to a radius of order 10^{15} cm. These results serve as an additional indication that at least some SLSNe are powered by interaction of the ejected material with a steady wind of similar mass.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/superluminous-light-curves-from-supernovae-exploding-in-a-dense-wind/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>[Fe III] emission lines in the planetary nebula NGC 2392</title>
		<link>http://voxcharta.org/2012/05/15/fe-iii-emission-lines-in-the-planetary-nebula-ngc-2392/</link>
		<comments>http://voxcharta.org/2012/05/15/fe-iii-emission-lines-in-the-planetary-nebula-ngc-2392/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:37:47 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bipolar]]></category>
		<category><![CDATA[bipolar nebula]]></category>
		<category><![CDATA[central regions]]></category>
		<category><![CDATA[chemical composition]]></category>
		<category><![CDATA[double shell]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[hypothesis]]></category>
		<category><![CDATA[intrinsic structure]]></category>
		<category><![CDATA[lobes]]></category>
		<category><![CDATA[morpho]]></category>
		<category><![CDATA[nebula ngc]]></category>
		<category><![CDATA[ngc 2392]]></category>
		<category><![CDATA[outer regions]]></category>
		<category><![CDATA[planetary nebula]]></category>
		<category><![CDATA[slit]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectroscopic observation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/fe-iii-emission-lines-in-the-planetary-nebula-ngc-2392/</guid>
		<description><![CDATA[NGC 2392 is a young double-shell planetary nebula (PN). Its intrinsic structure and shaping mechanism are still not fully understood. In this paper we present new spectroscopic observations of NGC 2392. The slits were placed at two different locations to obtain the spectra of the inner and outer regions. Several [Fe III] lines are clearly [...]]]></description>
			<content:encoded><![CDATA[<p>NGC 2392 is a young double-shell planetary nebula (PN). Its intrinsic structure and shaping mechanism are still not fully understood. In this paper we present new spectroscopic observations of NGC 2392. The slits were placed at two different locations to obtain the spectra of the inner and outer regions. Several [Fe III] lines are clearly detected in the inner region. We infer that NGC 2392 might have an intrinsic structure similar to the bipolar nebula Mz 3, which also exhibits a number of [Fe III}] lines arising from the central regions. In this scenario, the inner and outer regions of NGC 2392 correspond to the inner lobes and the outer outflows of Mz 3, respectively. We construct a three-dimensional morpho-kinematic model to examine our hypothesis. We also compare the physical conditions and chemical composition of the inner and outer regions, and discuss the implications on the formation of this type of PN.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/fe-iii-emission-lines-in-the-planetary-nebula-ngc-2392/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>All solutions of the n = 5 Lane-Emden equation [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/15/all-solutions-of-the-n-5-lane-emden-equation-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/15/all-solutions-of-the-n-5-lane-emden-equation-cross-listing/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:37:18 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[elliptic functions]]></category>
		<category><![CDATA[emden]]></category>
		<category><![CDATA[formulae]]></category>
		<category><![CDATA[jacobian]]></category>
		<category><![CDATA[new solution]]></category>
		<category><![CDATA[real solution]]></category>
		<category><![CDATA[symmetry]]></category>
		<category><![CDATA[weierstrass]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/all-solutions-of-the-n-5-lane-emden-equation-cross-listing/</guid>
		<description><![CDATA[All real solutions of the Lane-Emden equation for n = 5 are obtained in terms of Jacobian and Weierstrass elliptic functions. A new family of solutions is found. It is expressed by remarkably simple formulae involving Jacobian elliptic functions only. The general properties and discrete scaling symmetries of these new solutions are discussed. We also [...]]]></description>
			<content:encoded><![CDATA[<p>All real solutions of the Lane-Emden equation for n = 5 are obtained in terms of Jacobian and Weierstrass elliptic functions. A new family of solutions is found. It is expressed by remarkably simple formulae involving Jacobian elliptic functions only. The general properties and discrete scaling symmetries of these new solutions are discussed. We also comment on their possible applications.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/all-solutions-of-the-n-5-lane-emden-equation-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Particle-In-Cell Simulation of Electron Acceleration in Solar Coronal Jets</title>
		<link>http://voxcharta.org/2012/05/15/particle-in-cell-simulation-of-electron-acceleration-in-solar-coronal-jets/</link>
		<comments>http://voxcharta.org/2012/05/15/particle-in-cell-simulation-of-electron-acceleration-in-solar-coronal-jets/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:37:09 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration mechanism]]></category>
		<category><![CDATA[boundary condition]]></category>
		<category><![CDATA[cell simulation]]></category>
		<category><![CDATA[cells]]></category>
		<category><![CDATA[current sheet]]></category>
		<category><![CDATA[electric current]]></category>
		<category><![CDATA[electron]]></category>
		<category><![CDATA[electron acceleration]]></category>
		<category><![CDATA[investigations]]></category>
		<category><![CDATA[jets]]></category>
		<category><![CDATA[losses]]></category>
		<category><![CDATA[magnetic flux rope]]></category>
		<category><![CDATA[magnetic reconnection]]></category>
		<category><![CDATA[mesh refinement]]></category>
		<category><![CDATA[mhd simulation]]></category>
		<category><![CDATA[numerical resolution]]></category>
		<category><![CDATA[open magnetic field]]></category>
		<category><![CDATA[particle acceleration]]></category>
		<category><![CDATA[snapshot]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/particle-in-cell-simulation-of-electron-acceleration-in-solar-coronal-jets/</guid>
		<description><![CDATA[We investigate electron acceleration resulting from 3D magnetic reconnection between an emerging, twisted magnetic flux rope and a pre-existing weak, open magnetic field. We first follow the rise of an unstable, twisted flux tube with a resistive MHD simulation where the numerical resolution is enhanced by using fixed mesh refinement. As in previous MHD investigations [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate electron acceleration resulting from 3D magnetic reconnection between an emerging, twisted magnetic flux rope and a pre-existing weak, open magnetic field. We first follow the rise of an unstable, twisted flux tube with a resistive MHD simulation where the numerical resolution is enhanced by using fixed mesh refinement. As in previous MHD investigations of similar situations the rise of the flux tube into the pre-existing inclined coronal magnetic field results in the formation of a solar coronal jet. A snapshot of the MHD model is then used as an initial and boundary condition for a particle-in-cell simulation, using up to half a billion cells and over 20 billion charged particle. Particle acceleration occurs mainly in the reconnection current sheet, with accelerated electrons displaying a power law dN/dE distribution with an index of about -1.65. The main acceleration mechanism is a systematic electric field, striving to maintaining the electric current in the current sheet against losses caused by electrons not being able to stay in the current sheet for more than a few seconds at a time.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/particle-in-cell-simulation-of-electron-acceleration-in-solar-coronal-jets/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Rapidly rotating axisymmetric neutron stars with quark cores [Replacement]</title>
		<link>http://voxcharta.org/2012/05/15/rapidly-rotating-axisymmetric-neutron-stars-with-quark-cores-replacement/</link>
		<comments>http://voxcharta.org/2012/05/15/rapidly-rotating-axisymmetric-neutron-stars-with-quark-cores-replacement/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:34:49 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[compact star]]></category>
		<category><![CDATA[energy density]]></category>
		<category><![CDATA[equation of state]]></category>
		<category><![CDATA[flow data]]></category>
		<category><![CDATA[hadronic]]></category>
		<category><![CDATA[heavy ion collisions]]></category>
		<category><![CDATA[maximum frequency]]></category>
		<category><![CDATA[maximum mass]]></category>
		<category><![CDATA[millisecond pulsar]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[neutron star matter]]></category>
		<category><![CDATA[nuclear equation]]></category>
		<category><![CDATA[nuclear matter]]></category>
		<category><![CDATA[nucleon]]></category>
		<category><![CDATA[odot]]></category>
		<category><![CDATA[pulsars]]></category>
		<category><![CDATA[rotating stars]]></category>
		<category><![CDATA[solar mass]]></category>
		<category><![CDATA[systematic study]]></category>
		<category><![CDATA[thin crust]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/rapidly-rotating-axisymmetric-neutron-stars-with-quark-cores-replacement/</guid>
		<description><![CDATA[We present a systematic study of the properties of pure hadronic and hybrid compact stars. The nuclear equation of state (EoS) for beta-equilibrated neutron star matter was obtained using density dependent effective nucleon-nucleon interaction which satisfies the constraints from the observed flow data from heavy-ion collisions. The energy density of quark matter is lower than [...]]]></description>
			<content:encoded><![CDATA[<p>We present a systematic study of the properties of pure hadronic and hybrid compact stars. The nuclear equation of state (EoS) for beta-equilibrated neutron star matter was obtained using density dependent effective nucleon-nucleon interaction which satisfies the constraints from the observed flow data from heavy-ion collisions. The energy density of quark matter is lower than that of this nuclear EoS at higher densities implying the possibility of transition to quark matter inside the core. We solve the Einstein&#8217;s equations for rotating stars using pure nuclear matter and quark core. The beta- equilibrated neutron star matter with a thin crust is able to describe highly massive compact stars but find that the nuclear to quark matter deconfinement transition inside neutron stars causes reduction in their masses. Recent observations of the binary millisecond pulsar J1614-2230 by P. B. Demorest et al. [1] suggest that the masses lie within 1.97\pm0.04 M\odot where M\odot is the solar mass. In conformity with recent observations, pure nucleonic EoS determines that the maximum mass of NS rotating with frequency below r-mode instability is ~1.95 M\odot with radius ~10 kilometers. Although compact stars with quark cores rotating with Kepler&#8217;s frequency have masses up to ~2 M\odot, but if the maximum frequency is limited by the r-mode instability, the maximum mass ~1.7 M\odot turns out to be lower than the observed mass of 1.97\pm0.04 M\odot, by far the highest yet measured with such certainty, implying exclusion of quark cores for such massive pulsars.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/rapidly-rotating-axisymmetric-neutron-stars-with-quark-cores-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Protostellar disk formation and transport of angular momentum during magnetized core collapse [Replacement]</title>
		<link>http://voxcharta.org/2012/05/15/protostellar-disk-formation-and-transport-of-angular-momentum-during-magnetized-core-collapse-replacement/</link>
		<comments>http://voxcharta.org/2012/05/15/protostellar-disk-formation-and-transport-of-angular-momentum-during-magnetized-core-collapse-replacement/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:33:17 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[amr]]></category>
		<category><![CDATA[angular momentum]]></category>
		<category><![CDATA[cavity]]></category>
		<category><![CDATA[core collapse]]></category>
		<category><![CDATA[critical value]]></category>
		<category><![CDATA[dense core]]></category>
		<category><![CDATA[disk formation]]></category>
		<category><![CDATA[field intensity]]></category>
		<category><![CDATA[fragmentation]]></category>
		<category><![CDATA[gravitational collapse]]></category>
		<category><![CDATA[initial configuration]]></category>
		<category><![CDATA[initial core]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[mhd simulation]]></category>
		<category><![CDATA[outflow]]></category>
		<category><![CDATA[rotation axis]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[theoretical study]]></category>
		<category><![CDATA[ubiquity]]></category>
		<category><![CDATA[variance]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/protostellar-disk-formation-and-transport-of-angular-momentum-during-magnetized-core-collapse-replacement/</guid>
		<description><![CDATA[Theoretical studies of collapsing clouds have found that even a relatively weak magnetic field (B) may prevent the formation of disks and their fragmentation. However, most previous studies have been limited to cases where B and the rotation axis of the cloud are aligned. We study the transport of angular momentum, and its effects on [...]]]></description>
			<content:encoded><![CDATA[<p>Theoretical studies of collapsing clouds have found that even a relatively weak magnetic field (B) may prevent the formation of disks and their fragmentation. However, most previous studies have been limited to cases where B and the rotation axis of the cloud are aligned. We study the transport of angular momentum, and its effects on disk formation, for non-aligned initial configurations and a range magnetic intensities. We perform 3D AMR MHD simulations of magnetically supercritical collapsing dense cores using the code Ramses. We compute the contributions of the processes transporting angular momentum (J), in the envelope and the region of the disk. We clearly define what could be defined as centrifugally supported disks and study their properties. At variance with earlier analyses, we show that the transport of J acts less efficiently in collapsing cores with non-aligned rotation axis and B. Analytically, this result can be understood by taking into account the bending of field lines occurring during the gravitational collapse. For the transport of J, we conclude that magnetic braking in the mean direction of B tends to dominate over both the gravitational and outflow transport of J. We find that massive disks, containing at least 10% of the initial core mass, can form during the earliest stages of star formation even for mass-to-flux ratios as small as 3 to 5 times the critical value. At higher field intensities, the early formation of massive disks is prevented. Given the ubiquity of Class I disks, and because the early formation of massive disks can take place at moderate magnetic intensities, we speculate that for stronger fields, disks will form later, when most of the envelope will have been accreted. In addition, we speculate that some observed early massive disks may actually be outflow cavities, mistaken for disks by projection effects. (Abridged version of the abstract.)</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/protostellar-disk-formation-and-transport-of-angular-momentum-during-magnetized-core-collapse-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Observable QPOs produced by steep pulse profiles in Magnetar Flares [Replacement]</title>
		<link>http://voxcharta.org/2012/05/15/observable-qpos-produced-by-steep-pulse-profiles-in-magnetar-flares-replacement/</link>
		<comments>http://voxcharta.org/2012/05/15/observable-qpos-produced-by-steep-pulse-profiles-in-magnetar-flares-replacement/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:32:47 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[amplification]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[beam of light]]></category>
		<category><![CDATA[direct observation]]></category>
		<category><![CDATA[flare]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[geometry]]></category>
		<category><![CDATA[gradient]]></category>
		<category><![CDATA[harmonics]]></category>
		<category><![CDATA[light curve]]></category>
		<category><![CDATA[line of sight]]></category>
		<category><![CDATA[modulation]]></category>
		<category><![CDATA[oscillation]]></category>
		<category><![CDATA[periodic oscillation]]></category>
		<category><![CDATA[power spectrum]]></category>
		<category><![CDATA[pulse profile]]></category>
		<category><![CDATA[SGR]]></category>
		<category><![CDATA[starquake]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/observable-qpos-produced-by-steep-pulse-profiles-in-magnetar-flares-replacement/</guid>
		<description><![CDATA[Strong quasi-periodic oscillations in the tails of the giant gamma-ray flares seen in SGR 1806-20 and SGR 1900+14 are thought to be produced by starquakes in the flaring magnetar. However, the large fractional amplitudes (up to ~20%) observed are difficult to reconcile with predicted amplitudes of starquakes. Here we demonstrate that the steeply pulsed emission [...]]]></description>
			<content:encoded><![CDATA[<p>Strong quasi-periodic oscillations in the tails of the giant gamma-ray flares seen in SGR 1806-20 and SGR 1900+14 are thought to be produced by starquakes in the flaring magnetar. However, the large fractional amplitudes (up to ~20%) observed are difficult to reconcile with predicted amplitudes of starquakes. Here we demonstrate that the steeply pulsed emission profile in the tail of the giant flare can enhance the observed amplitude of the underlying oscillation, analogously to a beam of light oscillating in and out of the line of sight. This mechanism will also broaden the feature in the power spectrum and introduce power at harmonics of the oscillation. The observed strength of the oscillation depends on the amplitude of the underlying starquake, the orientation and location of the emission on the surface of the star, and the gradient of the light curve profile. While the amplification of the signal can be significant, we demonstrate that even with uncertainties in the emission geometry, this effect is not sufficient to produce the observed QPOs. This result excludes the direct observation of a starquake, and suggests that the observed variations come from modulations in the intensity of the emission.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/observable-qpos-produced-by-steep-pulse-profiles-in-magnetar-flares-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>An HST Imaging Survey of Low-Mass Stars in the Chamaeleon I Star Forming region</title>
		<link>http://voxcharta.org/2012/05/14/an-hst-imaging-survey-of-low-mass-stars-in-the-chamaeleon-i-star-forming-region/</link>
		<comments>http://voxcharta.org/2012/05/14/an-hst-imaging-survey-of-low-mass-stars-in-the-chamaeleon-i-star-forming-region/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:51:04 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion rates]]></category>
		<category><![CDATA[alpha 2]]></category>
		<category><![CDATA[chamaeleon]]></category>
		<category><![CDATA[disk parameters]]></category>
		<category><![CDATA[fitting tool]]></category>
		<category><![CDATA[hst imaging]]></category>
		<category><![CDATA[mass loss]]></category>
		<category><![CDATA[mass star]]></category>
		<category><![CDATA[mm data]]></category>
		<category><![CDATA[narrow band filters]]></category>
		<category><![CDATA[optical data]]></category>
		<category><![CDATA[outlier]]></category>
		<category><![CDATA[photometry]]></category>
		<category><![CDATA[region images]]></category>
		<category><![CDATA[spectral energy distribution]]></category>
		<category><![CDATA[spectral index]]></category>
		<category><![CDATA[t tauri]]></category>
		<category><![CDATA[tauri stars]]></category>
		<category><![CDATA[v band]]></category>
		<category><![CDATA[wfpc2 observations]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/an-hst-imaging-survey-of-low-mass-stars-in-the-chamaeleon-i-star-forming-region/</guid>
		<description><![CDATA[We present new HST/WFPC2 observations of 20 fields centered around T Tauri stars in the Chamaeleon I star forming region. Images have been obtained in the F631N ([OI]6300A), F656N (Ha) and F673N ([SII]6716A+6731A) narrow-band filters, plus the Johnson V-band equivalent F547M filter. We detect 31 T Tauri stars falling within our fields. We discuss the [...]]]></description>
			<content:encoded><![CDATA[<p>We present new HST/WFPC2 observations of 20 fields centered around T Tauri stars in the Chamaeleon I star forming region. Images have been obtained in the F631N ([OI]6300A), F656N (Ha) and F673N ([SII]6716A+6731A) narrow-band filters, plus the Johnson V-band equivalent F547M filter. We detect 31 T Tauri stars falling within our fields. We discuss the optical morphology of 10 sources showing evidence of either binarity, circumstellar material, or mass loss. We supplement our photometry with a compilation of optical, infrared and sub-millimeter data from the literature, together with new sub-mm data for three objects, to build the Spectral Energy Distributions (SED) of 19 single sources. Using an SED model fitting tool, we self-consistently estimate a number of stellar and disk parameters, while mass accretion rates are directly derived from our Ha photometry. We find that bolometric luminosities derived from dereddened optical data tend to be underestimated in systems with high alpha(2-24} IR spectral index, suggesting that disks seen nearly edge-on may occasionally be interpreted as low luminosity (and therefore more evolved) sources. On the other hand, the same alpha(2-24) spectral index, a tracer of the amount of dust in the warmer layers of the circumstellar disks, and the mass accretion rate appear to decay with the isocronal stellar age, suggesting that the observed age spread (~0.5-5 Myr) within the cluster is real. Our sample contains a few outliers that may have dissipated their circumstellar disks on shorter time-scale.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/an-hst-imaging-survey-of-low-mass-stars-in-the-chamaeleon-i-star-forming-region/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>WASP-42 b and WASP-49 b: two new transiting Saturns</title>
		<link>http://voxcharta.org/2012/05/14/wasp-42-b-and-wasp-49-b-two-new-transiting-saturns/</link>
		<comments>http://voxcharta.org/2012/05/14/wasp-42-b-and-wasp-49-b-two-new-transiting-saturns/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:49:21 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[equilibrium]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[photometry]]></category>
		<category><![CDATA[radius]]></category>
		<category><![CDATA[telescopes]]></category>
		<category><![CDATA[transiting planet]]></category>
		<category><![CDATA[wasp]]></category>
		<category><![CDATA[zero eccentricity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/wasp-42-b-and-wasp-49-b-two-new-transiting-saturns/</guid>
		<description><![CDATA[We report the discovery of two new transiting planets from the WASP survey. WASP-42 b is a 0.500 +- 0.035 M_J planet orbiting a K1 star at a separation of 0.0548 +- 0.0017 AU with a period of 4.9816872 +- 0.0000073 days. The radius of WASP-42 is 1.080 +- 0.057 R_J while its equilibrium temperature [...]]]></description>
			<content:encoded><![CDATA[<p>We report the discovery of two new transiting planets from the WASP survey. WASP-42 b is a 0.500 +- 0.035 M_J planet orbiting a K1 star at a separation of 0.0548 +- 0.0017 AU with a period of 4.9816872 +- 0.0000073 days. The radius of WASP-42 is 1.080 +- 0.057 R_J while its equilibrium temperature is T_eq = 995 +- 34 K. We detect some evidence of a small but non-zero eccentricity of e = 0.060 +- 0.013. WASP-49 b is a 0.378 +- 0.027 M_J planet around an old G6 star. It has a period of 2.7817387 +- 5.6 x 10-6 days and a separation of 0.0379 +- 0.0011 AU. This planet is slightly bloated, having a radius of 1.115 +- 0.056 R_J and an equilibrium temperature of T_eq = 1369 +- 42 K. Both planets have been followed up intensively in photometry, in total we have obtained 5 full and one partial transit light curves of WASP-42 and 4 full and one partial light curves of WASP-49 using the Euler-Swiss, TRAPPIST and Faulkes South telescopes.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/wasp-42-b-and-wasp-49-b-two-new-transiting-saturns/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Relativistic Solution for a Class of Static Compact Charged Star in Pseudo Spheroidal Space-Time</title>
		<link>http://voxcharta.org/2012/05/14/relativistic-solution-for-a-class-of-static-compact-charged-star-in-pseudo-spheroidal-space-time/</link>
		<comments>http://voxcharta.org/2012/05/14/relativistic-solution-for-a-class-of-static-compact-charged-star-in-pseudo-spheroidal-space-time/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:46:34 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[compact object]]></category>
		<category><![CDATA[compact star]]></category>
		<category><![CDATA[dependence]]></category>
		<category><![CDATA[einstein]]></category>
		<category><![CDATA[equation of state]]></category>
		<category><![CDATA[geometry]]></category>
		<category><![CDATA[linear equation]]></category>
		<category><![CDATA[maxwell equations]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[physical aspect]]></category>
		<category><![CDATA[qualitative analysis]]></category>
		<category><![CDATA[space time]]></category>
		<category><![CDATA[sphere]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/relativistic-solution-for-a-class-of-static-compact-charged-star-in-pseudo-spheroidal-space-time/</guid>
		<description><![CDATA[Considering Vaidya-Tikekar metric, we obtain a class of solutions of the Einstein-Maxwell equations for a charged static fluid sphere. The physical 3-space (t=constant) here is described by pseudo-spheroidal geometry. The relativistic solution for the theory is used to obtain models for charged compact objects, thereafter a qualitative analysis of the physical aspects of compact objects [...]]]></description>
			<content:encoded><![CDATA[<p>Considering Vaidya-Tikekar metric, we obtain a class of solutions of the Einstein-Maxwell equations for a charged static fluid sphere. The physical 3-space (t=constant) here is described by pseudo-spheroidal geometry. The relativistic solution for the theory is used to obtain models for charged compact objects, thereafter a qualitative analysis of the physical aspects of compact objects are studied. The dependence of some of the properties of a superdense star on the parameters of the three geometry is explored. We note that the spheroidicity parameter $a$, plays an important role for determining the properties of a compact object. A non-linear equation of state is required to describe a charged compact object with pseudo-spheroidal geometry which we have shown for known masses of compact objects. We also note that the size of a static compact charged star is more than that of a static compact star without charge.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/relativistic-solution-for-a-class-of-static-compact-charged-star-in-pseudo-spheroidal-space-time/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Variable Stars in the Globular Cluster M14</title>
		<link>http://voxcharta.org/2012/05/14/variable-stars-in-the-globular-cluster-m14/</link>
		<comments>http://voxcharta.org/2012/05/14/variable-stars-in-the-globular-cluster-m14/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:46:23 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[exceptions]]></category>
		<category><![CDATA[globular cluster]]></category>
		<category><![CDATA[image subtraction]]></category>
		<category><![CDATA[period]]></category>
		<category><![CDATA[phe]]></category>
		<category><![CDATA[rr lyrae stars]]></category>
		<category><![CDATA[uma]]></category>
		<category><![CDATA[variable star]]></category>
		<category><![CDATA[variables]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/variable-stars-in-the-globular-cluster-m14/</guid>
		<description><![CDATA[Using an image subtraction method we have searched for variable stars in the globular cluster M14. We confirmed 62 previously known catalogued variables. In addition to the previoulsy known variables we have identified 71 new variables. We have confirmed the periods of most of the cataloged variables with just a few exceptions. Of the the [...]]]></description>
			<content:encoded><![CDATA[<p>Using an image subtraction method we have searched for variable stars in the globular cluster M14. We confirmed 62 previously known catalogued variables. In addition to the previoulsy known variables we have identified 71 new variables. We have confirmed the periods of most of the cataloged variables with just a few exceptions. Of the the total number of confirmed variables, we found a total of 112 RR Lyrae stars, several of which exhibited the Blazhko Effect. Of the total we classified 55 RR0, 57 RR1, 19 variables with periods greater than 2 days, a W UMa contact binary, and an SX Phe star. We present the periods of previously found variables as well as the periods, classification, and lightcurves of the newly discovered variables.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/variable-stars-in-the-globular-cluster-m14/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A 3D Radiative Transfer Code for Modeling the Hanle Effect in the Lyman-alpha line</title>
		<link>http://voxcharta.org/2012/05/14/a-3d-radiative-transfer-code-for-modeling-the-hanle-effect-in-the-lyman-alpha-line/</link>
		<comments>http://voxcharta.org/2012/05/14/a-3d-radiative-transfer-code-for-modeling-the-hanle-effect-in-the-lyman-alpha-line/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:43:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[alpha line]]></category>
		<category><![CDATA[hanle effect]]></category>
		<category><![CDATA[intensity]]></category>
		<category><![CDATA[linear polarization]]></category>
		<category><![CDATA[lyman alpha]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetism]]></category>
		<category><![CDATA[modeling tools]]></category>
		<category><![CDATA[outer solar atmosphere]]></category>
		<category><![CDATA[signal]]></category>
		<category><![CDATA[solar transition region]]></category>
		<category><![CDATA[spectral line]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/a-3d-radiative-transfer-code-for-modeling-the-hanle-effect-in-the-lyman-alpha-line/</guid>
		<description><![CDATA[In order to obtain empirical information on the magnetism of the solar transition region we need to measure and interpret the linear polarization produced by scattering processes in FUV and EUV spectral lines. Via the Hanle effect such linear polarization signals are sensitive to the magnetic fields expected for the quiet and active regions of [...]]]></description>
			<content:encoded><![CDATA[<p>In order to obtain empirical information on the magnetism of the solar transition region we need to measure and interpret the linear polarization produced by scattering processes in FUV and EUV spectral lines. Via the Hanle effect such linear polarization signals are sensitive to the magnetic fields expected for the quiet and active regions of the outer solar atmosphere. For example, the Ly$\alpha$ line of H\,{\sc i} at 1216\,\AA\ is mainly sensitive to magnetic strengths between 10 and 100 G. The interpretation of the observed spectral line polarization requires the development of suitable modeling tools. To this end, we have developed a three-dimensional (3D), non-LTE multilevel radiative transfer code for modeling the intensity and linear polarization produced by scattering processes in spectral lines and its modification by the Hanle effect.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/a-3d-radiative-transfer-code-for-modeling-the-hanle-effect-in-the-lyman-alpha-line/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Measuring the Initial Mass Function of Low Mass Stars and Brown Dwarfs</title>
		<link>http://voxcharta.org/2012/05/14/measuring-the-initial-mass-function-of-low-mass-stars-and-brown-dwarfs/</link>
		<comments>http://voxcharta.org/2012/05/14/measuring-the-initial-mass-function-of-low-mass-stars-and-brown-dwarfs/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:43:25 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[brown dwarf]]></category>
		<category><![CDATA[calibration]]></category>
		<category><![CDATA[cluster]]></category>
		<category><![CDATA[galactic disk]]></category>
		<category><![CDATA[imf]]></category>
		<category><![CDATA[initial mass function]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[mass star]]></category>
		<category><![CDATA[methodology]]></category>
		<category><![CDATA[systematic uncertainty]]></category>
		<category><![CDATA[theoretical model]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/measuring-the-initial-mass-function-of-low-mass-stars-and-brown-dwarfs/</guid>
		<description><![CDATA[I review efforts to determine the form and any lower limit to the initial mass function in the Galactic disk, using observations of low-mass stars and brown dwarfs in the field, young clusters and star forming regions. I focus on the methodologies that have been used and the uncertainties that exist due to observational limitations [...]]]></description>
			<content:encoded><![CDATA[<p>I review efforts to determine the form and any lower limit to the initial mass function in the Galactic disk, using observations of low-mass stars and brown dwarfs in the field, young clusters and star forming regions. I focus on the methodologies that have been used and the uncertainties that exist due to observational limitations and to systematic uncertainties in calibrations and theoretical models. I conclude that whilst it is possible that the low-mass IMFs deduced from the field and most young clusters are similar, there are too many problems to be sure; there are examples of low-mass cluster IMFs that appear to be very discrepant and the IMFs for brown dwarfs in the field and young clusters have yet to be reconciled convincingly.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/measuring-the-initial-mass-function-of-low-mass-stars-and-brown-dwarfs/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Chameleon stars supported by a cosmological scalar field</title>
		<link>http://voxcharta.org/2012/05/14/chameleon-stars-supported-by-a-cosmological-scalar-field/</link>
		<comments>http://voxcharta.org/2012/05/14/chameleon-stars-supported-by-a-cosmological-scalar-field/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:43:04 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[chameleon]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[coupling]]></category>
		<category><![CDATA[expansion of the universe]]></category>
		<category><![CDATA[matter content]]></category>
		<category><![CDATA[scalar field]]></category>
		<category><![CDATA[scales]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/chameleon-stars-supported-by-a-cosmological-scalar-field/</guid>
		<description><![CDATA[Starting from the assumption that the present accelerated expansion of the Universe is driven by a chameleon scalar field, the function describing a direct coupling between the matter content of the Universe and the scalar field is derived from cosmological considerations. In progressing from cosmology towards astrophysical scales, this function is used to estimate the [...]]]></description>
			<content:encoded><![CDATA[<p>Starting from the assumption that the present accelerated expansion of the Universe is driven by a chameleon scalar field, the function describing a direct coupling between the matter content of the Universe and the scalar field is derived from cosmological considerations. In progressing from cosmology towards astrophysical scales, this function is used to estimate the influence that such nonminimal coupling may have on the properties of usual (polytropic) stars whose matter can interact directly with the cosmological chameleon. It is shown that in order to obtain sizes and masses of compact configurations supported by the chameleon scalar field comparable to those of usual stars, it is necessary to assume that the pressure of the matter content of the Universe is substantially different from zero.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/chameleon-stars-supported-by-a-cosmological-scalar-field/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Solar neutrino physics with Borexino I [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/14/solar-neutrino-physics-with-borexino-i-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/14/solar-neutrino-physics-with-borexino-i-cross-listing/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:42:50 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[asymmetry]]></category>
		<category><![CDATA[borexino]]></category>
		<category><![CDATA[construction data]]></category>
		<category><![CDATA[direct evidence]]></category>
		<category><![CDATA[energy range]]></category>
		<category><![CDATA[energy threshold]]></category>
		<category><![CDATA[interaction rate]]></category>
		<category><![CDATA[invariance]]></category>
		<category><![CDATA[laboratori nazionali del gran sasso]]></category>
		<category><![CDATA[liquid scintillator]]></category>
		<category><![CDATA[neutrino interaction]]></category>
		<category><![CDATA[neutrino oscillation]]></category>
		<category><![CDATA[neutrino physics]]></category>
		<category><![CDATA[neutrino signal]]></category>
		<category><![CDATA[oscillation]]></category>
		<category><![CDATA[oscillation parameters]]></category>
		<category><![CDATA[solar neutrino]]></category>
		<category><![CDATA[solar neutrino data]]></category>
		<category><![CDATA[solar neutrino flux]]></category>
		<category><![CDATA[time measurement]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/solar-neutrino-physics-with-borexino-i-cross-listing/</guid>
		<description><![CDATA[Borexino is a large-volume liquid scintillator detector installed in the underground halls of the Laboratori Nazionali del Gran Sasso in Italy. After several years of construction, data taking started in May 2007. The Borexino phase I ended after about three years of data taking. Borexino provided the first real time measurement of the $^{7}$Be solar [...]]]></description>
			<content:encoded><![CDATA[<p>Borexino is a large-volume liquid scintillator detector installed in the underground halls of the Laboratori Nazionali del Gran Sasso in Italy. After several years of construction, data taking started in May 2007. The Borexino phase I ended after about three years of data taking. Borexino provided the first real time measurement of the $^{7}$Be solar neutrino interaction rate with accuracy better than 5% and confirmed the absence of its day-night asymmetry with 1.4% precision. This latter Borexino results alone rejects the LOW region of solar neutrino oscillation parameters at more than 8.5 $\sigma$ C.L. Combined with the other solar neutrino data, Borexino measurements isolate the MSW-LMA solution of neutrino oscillations without assuming CPT invariance in the neutrino sector. Borexino has also directly observed solar neutrinos in the 1.0-1.5 MeV energy range, leading to the first direct evidence of the $pep$ solar neutrino signal and the strongest constraint of the CNO solar neutrino flux up to date. Borexino provided the measurement of the solar $^{8}$B neutrino rate with 3 MeV energy threshold.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/solar-neutrino-physics-with-borexino-i-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Conditions for Gravitational Instability in Protoplanetary Disks</title>
		<link>http://voxcharta.org/2012/05/14/conditions-for-gravitational-instability-in-protoplanetary-disks/</link>
		<comments>http://voxcharta.org/2012/05/14/conditions-for-gravitational-instability-in-protoplanetary-disks/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:42:28 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion disk]]></category>
		<category><![CDATA[analytic model]]></category>
		<category><![CDATA[angular momentum]]></category>
		<category><![CDATA[central star]]></category>
		<category><![CDATA[cloud core]]></category>
		<category><![CDATA[coriolis force]]></category>
		<category><![CDATA[critical surface]]></category>
		<category><![CDATA[density profile]]></category>
		<category><![CDATA[giant planet]]></category>
		<category><![CDATA[gravitational instability]]></category>
		<category><![CDATA[gravitational stability]]></category>
		<category><![CDATA[momentum distribution]]></category>
		<category><![CDATA[opacity]]></category>
		<category><![CDATA[order of magnitude]]></category>
		<category><![CDATA[protoplanetary disk]]></category>
		<category><![CDATA[protostar]]></category>
		<category><![CDATA[surface density]]></category>
		<category><![CDATA[temperature dependence]]></category>
		<category><![CDATA[thermal equilibrium]]></category>
		<category><![CDATA[viscosity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/conditions-for-gravitational-instability-in-protoplanetary-disks/</guid>
		<description><![CDATA[Gravitational instability is one of considerable mechanisms to explain the formation of giant planets. We study the gravitational stability for the protoplanetary disks around a protostar. The temperature and Toomre&#8217;s Q-value are calculated by assuming local equilibrium between viscous heating and radiative cooling (local thermal equilibrium). We assume constant $\alpha$ viscosity and use a cooling [...]]]></description>
			<content:encoded><![CDATA[<p>Gravitational instability is one of considerable mechanisms to explain the formation of giant planets. We study the gravitational stability for the protoplanetary disks around a protostar. The temperature and Toomre&#8217;s Q-value are calculated by assuming local equilibrium between viscous heating and radiative cooling (local thermal equilibrium). We assume constant $\alpha$ viscosity and use a cooling function with realistic opacity. Then, we derive the critical surface density $\Sigma_{\rm{c}}$ that is necessary for a disk to become gravitationally unstable as a function of $r$. This critical surface density $\Sigma_{\rm c}$ is strongly affected by the temperature dependence of the opacity. At the radius $r_{\rm c}\sim 20$AU, where ices form, the value of $\Sigma_{\rm c}$ changes discontinuously by one order of magnitude. This $\Sigma_{\rm c}$ is determined only by local thermal process and criterion of gravitational instability. By comparing a given surface density profile to $\Sigma_{\rm c}$, one can discuss the gravitational instability of protoplanetary disks. As an example, we discuss the gravitational instability of two semi-analytic models for protoplanetary disks. One is the steady state accretion disk, which is realized after the viscous evolution. The other is the disk that has the same angular momentum distribution with its parent cloud core, which corresponds to the disk that has just formed. As a result, it is found that the disks tend to become gravitationally unstable for $r\ge r_{\rm c}$ because ices enable the disks to become low temperature. In the region closer to the protostar than $r_{\rm c}$, it is difficult for a typical protoplanetary disk to fragment because of the high temperature and the large Coriolis force. From this result, we conclude that the fragmentation near the central star is possible but difficult.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/conditions-for-gravitational-instability-in-protoplanetary-disks/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>TW Hya Association Membership and New WISE-detected Circumstellar Disks</title>
		<link>http://voxcharta.org/2012/05/14/tw-hya-association-membership-and-new-wise-detected-circumstellar-disks/</link>
		<comments>http://voxcharta.org/2012/05/14/tw-hya-association-membership-and-new-wise-detected-circumstellar-disks/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:41:34 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[30a]]></category>
		<category><![CDATA[association membership]]></category>
		<category><![CDATA[clear evidence]]></category>
		<category><![CDATA[disk geometry]]></category>
		<category><![CDATA[extinction]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[hya]]></category>
		<category><![CDATA[infrared survey]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[myr]]></category>
		<category><![CDATA[tw hydrae association]]></category>
		<category><![CDATA[twa]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/tw-hya-association-membership-and-new-wise-detected-circumstellar-disks/</guid>
		<description><![CDATA[We assess the current membership of the nearby, young TW Hydrae Association and examine newly proposed members with the Wide-field Infrared Survey Explorer (WISE) to search for infrared excess indicative of circumstellar disks. Newly proposed members TWA 30A, TWA 30B, TWA 31, and TWA 32 all show excess emission at 12 and 22 \mum providing [...]]]></description>
			<content:encoded><![CDATA[<p>We assess the current membership of the nearby, young TW Hydrae Association and examine newly proposed members with the Wide-field Infrared Survey Explorer (WISE) to search for infrared excess indicative of circumstellar disks. Newly proposed members TWA 30A, TWA 30B, TWA 31, and TWA 32 all show excess emission at 12 and 22 \mum providing clear evidence for substantial dusty circumstellar disks around these low-mass, ~8 Myr old stars that were previously shown to likely be accreting from circumstellar material. TWA 30B shows large amounts of self-extinction, likely due to an edge-on disk geometry. We also confirm previously reported circumstellar disks with WISE, and determine a 22 \mum excess fraction of 42+/- 9% based on our results.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/tw-hya-association-membership-and-new-wise-detected-circumstellar-disks/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Luminous [O III] and [N II] from Tidally Disrupted Horizontal Branch Stars</title>
		<link>http://voxcharta.org/2012/05/14/luminous-o-iii-and-n-ii-from-tidally-disrupted-horizontal-branch-stars/</link>
		<comments>http://voxcharta.org/2012/05/14/luminous-o-iii-and-n-ii-from-tidally-disrupted-horizontal-branch-stars/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:40:28 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[clump]]></category>
		<category><![CDATA[debris]]></category>
		<category><![CDATA[emission line spectrum]]></category>
		<category><![CDATA[horizontal branch stars]]></category>
		<category><![CDATA[lambda lambda]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[NGC]]></category>
		<category><![CDATA[optical emission lines]]></category>
		<category><![CDATA[Sun]]></category>
		<category><![CDATA[tidal disruption]]></category>
		<category><![CDATA[uv emission]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/luminous-o-iii-and-n-ii-from-tidally-disrupted-horizontal-branch-stars/</guid>
		<description><![CDATA[We model the emission lines generated in the photoionised debris of a tidally disrupted horizontal branch star. We find that at late times, the brightest optical emission lines are [N II] \lambda\lambda 6548,6583 and [O III] \lambda\lambda 4959,5007. Models of a red clump horizontal branch star undergoing mild disruption by a massive (50 &#8212; 100 [...]]]></description>
			<content:encoded><![CDATA[<p>We model the emission lines generated in the photoionised debris of a tidally disrupted horizontal branch star. We find that at late times, the brightest optical emission lines are [N II] \lambda\lambda 6548,6583 and [O III] \lambda\lambda 4959,5007. Models of a red clump horizontal branch star undergoing mild disruption by a massive (50 &#8212; 100 M_\sun) black hole yield an emission line spectrum that is in good agreement with that observed in the NGC 1399 globular cluster hosting the ultraluminous X-ray source CXOJ033831.8 &#8211; 352604. We make predictions for the UV emission line spectrum that can verify the tidal disruption scenario and constrain the mass of the BH.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/luminous-o-iii-and-n-ii-from-tidally-disrupted-horizontal-branch-stars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Properties of Galactic early-type O-supergiants: A combined FUV-UV and optical analysis</title>
		<link>http://voxcharta.org/2012/05/14/properties-of-galactic-early-type-o-supergiants-a-combined-fuv-uv-and-optical-analysis/</link>
		<comments>http://voxcharta.org/2012/05/14/properties-of-galactic-early-type-o-supergiants-a-combined-fuv-uv-and-optical-analysis/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:39:31 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[chemical composition]]></category>
		<category><![CDATA[evolutionary model]]></category>
		<category><![CDATA[evolutionary sequence]]></category>
		<category><![CDATA[evolutionary status]]></category>
		<category><![CDATA[fuv]]></category>
		<category><![CDATA[initial mass]]></category>
		<category><![CDATA[isochrone]]></category>
		<category><![CDATA[mass loss rates]]></category>
		<category><![CDATA[msun]]></category>
		<category><![CDATA[o star]]></category>
		<category><![CDATA[older stars]]></category>
		<category><![CDATA[optical analysis]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[supergiant]]></category>
		<category><![CDATA[surface chemical]]></category>
		<category><![CDATA[surface gravity]]></category>
		<category><![CDATA[terminal velocity]]></category>
		<category><![CDATA[wind code]]></category>
		<category><![CDATA[wind parameters]]></category>
		<category><![CDATA[wind profile]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/properties-of-galactic-early-type-o-supergiants-a-combined-fuv-uv-and-optical-analysis/</guid>
		<description><![CDATA[We aim to constrain the properties and evolutionary status of early and mid-spectral type supergiants (from O4 to O7.5). These posses the highest mass-loss rates among the O stars, and exhibit conspicuous wind profiles. Using the non-LTE wind code CMFGEN, we simultaneously analyzed the FUV-UV and optical spectral range to determine the photospheric properties and [...]]]></description>
			<content:encoded><![CDATA[<p>We aim to constrain the properties and evolutionary status of early and mid-spectral type supergiants (from O4 to O7.5). These posses the highest mass-loss rates among the O stars, and exhibit conspicuous wind profiles. Using the non-LTE wind code CMFGEN, we simultaneously analyzed the FUV-UV and optical spectral range to determine the photospheric properties and wind parameters. We derived effective temperatures, luminosities, surface gravities, surface abundances, mass-loss rates, wind terminal velocities, and clumping filling factors. The supergiants define a very clear evolutionary sequence, in terms of ages and masses, from younger and more massive stars to older stars with lower initial masses. O4 supergiants cluster around the 3 Myr isochrone and are more massive than 60 Msun, while the O5 to O7.5 stars have masses in the range 50 &#8211; 40 Msun and are 4 +/- 0.3 Myr old. The surface chemical composition is typical of evolved O supergiants (nitrogen-rich, carbon- and oxygen-poor). While the observed ranges of carbon and nitrogen mass-fractions are compatible with those expected from evolutionary models for the measured stellar masses, the N/C ratios as a function of age are inconsistent with the theoretical predictions for the four earliest (O4 spectral type) stars of the sample. We question the efficiency of rotational mixing as a function of age for these stars and suggest that another mechanism may be needed to explain the observed abundance patterns. Mass-loss rates derived with clumped-models range within a factor of three of the theoretical mass-loss rates. The corresponding volume-filling factors associated with small-scale clumping are 0.05 +/- 0.02. Clumping is found to start close to the photosphere for all but three stars, two of which are fast rotators.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/properties-of-galactic-early-type-o-supergiants-a-combined-fuv-uv-and-optical-analysis/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Dynamics of the Solar Radiative Zone</title>
		<link>http://voxcharta.org/2012/05/14/the-dynamics-of-the-solar-radiative-zone/</link>
		<comments>http://voxcharta.org/2012/05/14/the-dynamics-of-the-solar-radiative-zone/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:37:26 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[convective zone]]></category>
		<category><![CDATA[core rotation]]></category>
		<category><![CDATA[disparity]]></category>
		<category><![CDATA[estimates]]></category>
		<category><![CDATA[inference]]></category>
		<category><![CDATA[inner layers]]></category>
		<category><![CDATA[inversion]]></category>
		<category><![CDATA[layers of the sun]]></category>
		<category><![CDATA[methodology]]></category>
		<category><![CDATA[modes]]></category>
		<category><![CDATA[profile]]></category>
		<category><![CDATA[radiative zone]]></category>
		<category><![CDATA[rotation rate]]></category>
		<category><![CDATA[solar core]]></category>
		<category><![CDATA[solar cycle]]></category>
		<category><![CDATA[temporal variation]]></category>
		<category><![CDATA[uncertainty]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/the-dynamics-of-the-solar-radiative-zone/</guid>
		<description><![CDATA[The dynamics of the solar radiative interior are still poorly constrained by comparison to the convective zone. This disparity is even more marked when we attempt to derive meaningful temporal variations. Many data sets contain a small number of modes that are sensitive to the inner layers of the Sun, but we found that the [...]]]></description>
			<content:encoded><![CDATA[<p>The dynamics of the solar radiative interior are still poorly constrained by comparison to the convective zone. This disparity is even more marked when we attempt to derive meaningful temporal variations. Many data sets contain a small number of modes that are sensitive to the inner layers of the Sun, but we found that the estimates of their uncertainties are often inaccurate. As a result, these data sets allow us to obtain, at best, a low resolution estimate of the solar core rotation rate down to approximately 0.2R. We present inferences based on mode determination resulting from an alternate peak-fitting methodology aimed at increasing the amount of observed modes that are sensitive to the radiative zone, while special care was taken in the determination of their uncertainties. This methodology has been applied to MDI and GONG data, for the whole Solar Cycle 23, and to the newly available HMI data. The numerical inversions of all these data sets result in the best inferences to date of the rotation in the radiative region. These results and the method used to obtain them are discussed. The resulting profiles are shown and analyzed, and the significance of the detected changes discussed.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/the-dynamics-of-the-solar-radiative-zone/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Predictions of the Maximum Amplitude, Time of Occurrence, and Total Length of Solar Cycle 24</title>
		<link>http://voxcharta.org/2012/05/14/predictions-of-the-maximum-amplitude-time-of-occurrence-and-total-length-of-solar-cycle-24/</link>
		<comments>http://voxcharta.org/2012/05/14/predictions-of-the-maximum-amplitude-time-of-occurrence-and-total-length-of-solar-cycle-24/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:37:17 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[ascent time]]></category>
		<category><![CDATA[confidence interval]]></category>
		<category><![CDATA[correlation coefficient r]]></category>
		<category><![CDATA[curvature]]></category>
		<category><![CDATA[data base]]></category>
		<category><![CDATA[derivative]]></category>
		<category><![CDATA[incorporation]]></category>
		<category><![CDATA[intensity]]></category>
		<category><![CDATA[linear regression]]></category>
		<category><![CDATA[maximum amplitude]]></category>
		<category><![CDATA[maximum solar activity]]></category>
		<category><![CDATA[methodology]]></category>
		<category><![CDATA[occurrence]]></category>
		<category><![CDATA[predictive power]]></category>
		<category><![CDATA[solar cycle]]></category>
		<category><![CDATA[time series]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/predictions-of-the-maximum-amplitude-time-of-occurrence-and-total-length-of-solar-cycle-24/</guid>
		<description><![CDATA[In this work we predict the maximum amplitude, its time of occurrence, and the total length of Solar Cycle 24 by linear regression to the curvature (second derivative) at the preceding minimum of a smoothed version of the sunspots time series. We characterise the predictive power of the proposed methodology in a causal manner by [...]]]></description>
			<content:encoded><![CDATA[<p>In this work we predict the maximum amplitude, its time of occurrence, and the total length of Solar Cycle 24 by linear regression to the curvature (second derivative) at the preceding minimum of a smoothed version of the sunspots time series. We characterise the predictive power of the proposed methodology in a causal manner by an incremental incorporation of past solar cycles to the available data base. In regressing maximum cycle intensity to curvature at the leading minimum we obtain a correlation coefficient R \approx 0.91 and for the upcoming Cycle 24 a forecast of 78 (90% confidence interval: 56 &#8211; 106). Ascent time also appears to be highly correlated to the second derivative at the starting minimum (R \approx -0.77), predicting maximum solar activity for October 2013 (90% confidence interval: January 2013 to September 2014). Solar Cycle 24 should come to an end by February 2020 (90% confidence interval: January 2019 to July 2021), although in this case correlational evidence is weaker (R \approx -0.56).</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/predictions-of-the-maximum-amplitude-time-of-occurrence-and-total-length-of-solar-cycle-24/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Negative effective magnetic pressure in turbulent convection [Replacement]</title>
		<link>http://voxcharta.org/2012/05/14/negative-effective-magnetic-pressure-in-turbulent-convection-replacement-2/</link>
		<comments>http://voxcharta.org/2012/05/14/negative-effective-magnetic-pressure-in-turbulent-convection-replacement-2/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:36:57 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[anisotropy]]></category>
		<category><![CDATA[equation of state]]></category>
		<category><![CDATA[evolution equation]]></category>
		<category><![CDATA[isothermal layer]]></category>
		<category><![CDATA[large scale]]></category>
		<category><![CDATA[lorentz force]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetic pressure]]></category>
		<category><![CDATA[magnetic structure]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[turbulence effects]]></category>
		<category><![CDATA[turbulent convection]]></category>
		<category><![CDATA[vertical direction]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/negative-effective-magnetic-pressure-in-turbulent-convection-replacement-2/</guid>
		<description><![CDATA[We investigate the effects of weakly and strongly stratified turbulent convection on the mean effective Lorentz force, and especially on the mean effective magnetic pressure. Earlier studies with isotropically forced non-stratified and stratified turbulence have shown that the contribution of the turbulence to the mean magnetic pressure is negative for mean horizontal magnetic fields that [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate the effects of weakly and strongly stratified turbulent convection on the mean effective Lorentz force, and especially on the mean effective magnetic pressure. Earlier studies with isotropically forced non-stratified and stratified turbulence have shown that the contribution of the turbulence to the mean magnetic pressure is negative for mean horizontal magnetic fields that are smaller than the equipartition strength, so that the effective mean magnetic pressure that takes into account the turbulence effects, can be negative. Compared with earlier cases of forced turbulence with an isothermal equation of state, we find that the turbulence effect is similar to or even stronger in the present case of turbulent convection. This is argued to be due to the anisotropy of turbulence in the vertical direction. Another important difference compared with earlier studies is the presence of an evolution equation for the specific entropy. Mean-field modelling with entropy evolution indicates that the negative effective magnetic pressure can still lead to a large-scale instability which forms local flux concentrations, even though the specific entropy evolution tends to have a stabilizing effect when applied to a stably stratified (e.g., isothermal) layer. It is argued that this large-scale instability could be important for the formation of solar large-scale magnetic structures such as active regions.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/negative-effective-magnetic-pressure-in-turbulent-convection-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Characterization of Dwarf Novae Using SDSS Colors [Replacement]</title>
		<link>http://voxcharta.org/2012/05/14/characterization-of-dwarf-novae-using-sdss-colors-replacement/</link>
		<comments>http://voxcharta.org/2012/05/14/characterization-of-dwarf-novae-using-sdss-colors-replacement/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:36:07 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[artificial neural network]]></category>
		<category><![CDATA[cam type]]></category>
		<category><![CDATA[categorical classification]]></category>
		<category><![CDATA[characterization]]></category>
		<category><![CDATA[digital sky survey]]></category>
		<category><![CDATA[dwarf novae]]></category>
		<category><![CDATA[estimation]]></category>
		<category><![CDATA[faint object]]></category>
		<category><![CDATA[gap]]></category>
		<category><![CDATA[neural network analysis]]></category>
		<category><![CDATA[orbital period]]></category>
		<category><![CDATA[photometric accuracy]]></category>
		<category><![CDATA[quiescence]]></category>
		<category><![CDATA[sdss]]></category>
		<category><![CDATA[sigma]]></category>
		<category><![CDATA[sloan digital]]></category>
		<category><![CDATA[ss cyg]]></category>
		<category><![CDATA[time survey]]></category>
		<category><![CDATA[typical objects]]></category>
		<category><![CDATA[uncertainty]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/characterization-of-dwarf-novae-using-sdss-colors-replacement/</guid>
		<description><![CDATA[We have developed a method for estimating the orbital periods of dwarf novae from the Sloan Digital Sky Survey (SDSS) colors in quiescence using an artificial neural network. For typical objects below the period gap with sufficient photometric accuracy, we were able to estimate the orbital periods with an accuracy to a 1 sigma error [...]]]></description>
			<content:encoded><![CDATA[<p>We have developed a method for estimating the orbital periods of dwarf novae from the Sloan Digital Sky Survey (SDSS) colors in quiescence using an artificial neural network. For typical objects below the period gap with sufficient photometric accuracy, we were able to estimate the orbital periods with an accuracy to a 1 sigma error of 22 %. The error of estimation is worse for systems with longer orbital periods. We have also developed a neural-network-based method for categorical classification. This method has proven to be efficient in classifying objects into three categories (WZ Sge type, SU UMa type and SS Cyg/Z Cam type) and works for very faint objects to a limit of g=21. Using this method, we have investigated the distribution of the orbital periods of dwarf novae from a modern transient survey (Catalina Real-Time Survey). Using Bayesian analysis developed by Uemura et al. (2010, arXiv:1003.0945), we have found that the present sample tends to give a flatter distribution toward the shortest period and a shorter estimate of the period minimum, which may have resulted from the uncertainties in the neural network analysis and photometric errors. We also provide estimated orbital periods, estimated classifications and supplementary information on known dwarf novae with quiescent SDSS photometry.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/characterization-of-dwarf-novae-using-sdss-colors-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 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/14/the-gj-436-system-directly-determined-astrophysical-parameters-of-an-m-dwarf-and-implications-for-the-transiting-hot-neptune-replacement/</link>
		<comments>http://voxcharta.org/2012/05/14/the-gj-436-system-directly-determined-astrophysical-parameters-of-an-m-dwarf-and-implications-for-the-transiting-hot-neptune-replacement/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:34:50 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[curves]]></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/2012/05/14/the-gj-436-system-directly-determined-astrophysical-parameters-of-an-m-dwarf-and-implications-for-the-transiting-hot-neptune-replacement/</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 ($M_{\star} = 0.507^{+ 0.071}_{- 0.062} M_{\odot}$) and density ($\rho_* = 5.37^{+ 0.30}_{- 0.27} \rho_\odot$), planetary radius ($R_{p} = 0.369^{+ 0.015}_{- 0.015} R_{Jupiter}$), planetary mass ($M_{p} = 0.078^{+ 0.007}_{- 0.008} M_{Jupiter}$), implying a mean planetary density of $\rho_{p} = 1.55^{+ 0.12}_{- 0.10} \rho_{Jupiter}$. 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/2012/05/14/the-gj-436-system-directly-determined-astrophysical-parameters-of-an-m-dwarf-and-implications-for-the-transiting-hot-neptune-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Data Analysis of Gravitational Waves Signals from Millisecond Pulsars [Replacement]</title>
		<link>http://voxcharta.org/2012/05/14/data-analysis-of-gravitational-waves-signals-from-millisecond-pulsars-replacement/</link>
		<comments>http://voxcharta.org/2012/05/14/data-analysis-of-gravitational-waves-signals-from-millisecond-pulsars-replacement/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:33:21 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[allegro]]></category>
		<category><![CDATA[doppler]]></category>
		<category><![CDATA[estimates]]></category>
		<category><![CDATA[globular cluster]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[millisecond pulsar]]></category>
		<category><![CDATA[NGC]]></category>
		<category><![CDATA[power spectrum]]></category>
		<category><![CDATA[signal]]></category>
		<category><![CDATA[variation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/data-analysis-of-gravitational-waves-signals-from-millisecond-pulsars-replacement/</guid>
		<description><![CDATA[The present work is devoted to the detection of monochromatic gravitational wave signals emitted by pulsars using ALLEGRO&#8217;s data detector. We will present the region (in frequency) of millisecond pulsars of the globular cluster 47 Tucanae (NGC 104) in the band of detector. With this result it was possible to analyse the data in the [...]]]></description>
			<content:encoded><![CDATA[<p>The present work is devoted to the detection of monochromatic gravitational wave signals emitted by pulsars using ALLEGRO&#8217;s data detector. We will present the region (in frequency) of millisecond pulsars of the globular cluster 47 Tucanae (NGC 104) in the band of detector. With this result it was possible to analyse the data in the frequency ranges of the pulsars J1748-2446L and J1342+2822c, searching for annual Doppler variations using power spectrum estimates for the year 1999. We tested this method injecting a simulated signal in real data and we were able to detect it.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/data-analysis-of-gravitational-waves-signals-from-millisecond-pulsars-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A survey of nulling pulsars using the Giant Meterwave Radio Telescope [Replacement]</title>
		<link>http://voxcharta.org/2012/05/14/a-survey-of-nulling-pulsars-using-the-giant-meterwave-radio-telescope-replacement/</link>
		<comments>http://voxcharta.org/2012/05/14/a-survey-of-nulling-pulsars-using-the-giant-meterwave-radio-telescope-replacement/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:31:21 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[burst]]></category>
		<category><![CDATA[cessation]]></category>
		<category><![CDATA[detail analysis]]></category>
		<category><![CDATA[distributions]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[full detail]]></category>
		<category><![CDATA[interval]]></category>
		<category><![CDATA[null phase]]></category>
		<category><![CDATA[pulsars]]></category>
		<category><![CDATA[pulse energy]]></category>
		<category><![CDATA[pulses]]></category>
		<category><![CDATA[radio telescope]]></category>
		<category><![CDATA[stochastic poisson]]></category>
		<category><![CDATA[time scale]]></category>
		<category><![CDATA[transition]]></category>
		<category><![CDATA[vice verse]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/a-survey-of-nulling-pulsars-using-the-giant-meterwave-radio-telescope-replacement/</guid>
		<description><![CDATA[Several pulsars show sudden cessation of pulsed emission, which is known as pulsar nulling. In this paper, the nulling behaviour of 15 pulsars is presented. The nulling fractions of these pulsars, along with the degree of reduction in the pulse energy during the null phase, are reported for these pulsars. A quasi-periodic null-burst pattern is [...]]]></description>
			<content:encoded><![CDATA[<p>Several pulsars show sudden cessation of pulsed emission, which is known as pulsar nulling. In this paper, the nulling behaviour of 15 pulsars is presented. The nulling fractions of these pulsars, along with the degree of reduction in the pulse energy during the null phase, are reported for these pulsars. A quasi-periodic null-burst pattern is reported for PSR J1738-2330. The distributions of lengths of the null and the burst phases as well as the typical nulling time scales are estimated for eight strong pulsars. The nulling pattern of four pulsars with similar nulling fraction are found to be different from each other, suggesting that the fraction of null pulses does not quantify the nulling behaviour of a pulsar in full detail. Analysis of these distributions also indicate that while the null and the burst pulses occur in groups, the underlying distribution of the interval between a transition from the null to the burst phase and vice verse appears to be similar to that of a stochastic Poisson point process.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/a-survey-of-nulling-pulsars-using-the-giant-meterwave-radio-telescope-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Detection of Solar Rotational Variability in the LYRA 190 &#8211; 222 nm Spectral Band</title>
		<link>http://voxcharta.org/2012/05/13/detection-of-solar-rotational-variability-in-the-lyra-190-222-nm-spectral-band/</link>
		<comments>http://voxcharta.org/2012/05/13/detection-of-solar-rotational-variability-in-the-lyra-190-222-nm-spectral-band/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:52:39 +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[20 january]]></category>
		<category><![CDATA[7 january]]></category>
		<category><![CDATA[algorithm]]></category>
		<category><![CDATA[degradation]]></category>
		<category><![CDATA[herzberg]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[period of time]]></category>
		<category><![CDATA[solar irradiance]]></category>
		<category><![CDATA[solar variability]]></category>
		<category><![CDATA[solstice]]></category>
		<category><![CDATA[spectral band]]></category>
		<category><![CDATA[time observation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/detection-of-solar-rotational-variability-in-the-lyra-190-222-nm-spectral-band/</guid>
		<description><![CDATA[We analyze the variability of the spectral solar irradiance during the period from 7 January, 2010 until 20 January, 2010 as measured by the Herzberg channel (190-222 nm) of the Large Yield RAdiometer (LYRA) onboard PROBA2. In this period of time observations by the LYRA nominal unit experienced degradation and the signal produced by the [...]]]></description>
			<content:encoded><![CDATA[<p>We analyze the variability of the spectral solar irradiance during the period from 7 January, 2010 until 20 January, 2010 as measured by the Herzberg channel (190-222 nm) of the Large Yield RAdiometer (LYRA) onboard PROBA2. In this period of time observations by the LYRA nominal unit experienced degradation and the signal produced by the Herzberg channel frequently jumped from one level to another. Both these factors significantly complicates the analysis. We present the algorithm which allowed us to extract the solar variability from the LYRA data and compare the results with SORCE/SOLSTICE measurements and with modeling based on the Code for the Solar Irradiance (COSI).</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/detection-of-solar-rotational-variability-in-the-lyra-190-222-nm-spectral-band/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>A rare early-type star revealed in the Wing of the Small Magellanic Cloud</title>
		<link>http://voxcharta.org/2012/05/13/a-rare-early-type-star-revealed-in-the-wing-of-the-small-magellanic-cloud/</link>
		<comments>http://voxcharta.org/2012/05/13/a-rare-early-type-star-revealed-in-the-wing-of-the-small-magellanic-cloud/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:51:30 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[brightest star]]></category>
		<category><![CDATA[dominant source]]></category>
		<category><![CDATA[hydrogen]]></category>
		<category><![CDATA[inner edge]]></category>
		<category><![CDATA[ionising]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[mass loss]]></category>
		<category><![CDATA[modulus]]></category>
		<category><![CDATA[msun]]></category>
		<category><![CDATA[nebula]]></category>
		<category><![CDATA[nitrogen]]></category>
		<category><![CDATA[optical spectroscopy]]></category>
		<category><![CDATA[physical parameter]]></category>
		<category><![CDATA[small magellanic cloud]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[star model]]></category>
		<category><![CDATA[type dwarf]]></category>
		<category><![CDATA[type star]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/a-rare-early-type-star-revealed-in-the-wing-of-the-small-magellanic-cloud/</guid>
		<description><![CDATA[Sk 183 is the visually-brightest star in the N90 nebula, a young star-forming region in the Wing of the Small Magellanic Cloud (SMC). We present new optical spectroscopy from the Very Large Telescope which reveals Sk 183 to be one of the most massive O-type stars in the SMC. Classified as an O3-type dwarf on [...]]]></description>
			<content:encoded><![CDATA[<p>Sk 183 is the visually-brightest star in the N90 nebula, a young star-forming region in the Wing of the Small Magellanic Cloud (SMC). We present new optical spectroscopy from the Very Large Telescope which reveals Sk 183 to be one of the most massive O-type stars in the SMC. Classified as an O3-type dwarf on the basis of its nitrogen spectrum, the star also displays broadened He I absorption which suggests a later type. We propose that Sk 183 has a composite spectrum and that it is similar to another star in the SMC, MPG 324. This brings the number of rare O2- and O3-type stars known in the whole of the SMC to a mere three. We estimate physical parameters for Sk 183 from analysis of its spectrum. For a single-star model, we estimate an effective temperature of 46+/-2 kK, a low mass-loss rate of ~10^-7 Msun yr^-1, and a spectroscopic mass of 46^+9_-8 Msun (for an adopted distance modulus of 18.7 mag to the young population in the SMC Wing). An illustrative binary model requires a slightly hotter temperature (~47.5 kK) for the primary component. In either scenario, Sk 183 is the earliest-type star known in N90 and will therefore be the dominant source of hydrogen-ionising photons. This suggests Sk 183 is the primary influence on the star formation along the inner edge of the nebula.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/a-rare-early-type-star-revealed-in-the-wing-of-the-small-magellanic-cloud/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The primordial Li abundance derived from giant stars</title>
		<link>http://voxcharta.org/2012/05/13/the-primordial-li-abundance-derived-from-giant-stars/</link>
		<comments>http://voxcharta.org/2012/05/13/the-primordial-li-abundance-derived-from-giant-stars/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:51:15 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abundance]]></category>
		<category><![CDATA[atomic diffusion]]></category>
		<category><![CDATA[bang nucleosynthesis]]></category>
		<category><![CDATA[big bang]]></category>
		<category><![CDATA[bump]]></category>
		<category><![CDATA[dex]]></category>
		<category><![CDATA[discrepancy]]></category>
		<category><![CDATA[dredge]]></category>
		<category><![CDATA[dwarf star]]></category>
		<category><![CDATA[galactic halo]]></category>
		<category><![CDATA[giant star]]></category>
		<category><![CDATA[globular cluster]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[main sequence]]></category>
		<category><![CDATA[NGC]]></category>
		<category><![CDATA[plateau]]></category>
		<category><![CDATA[sequence phase]]></category>
		<category><![CDATA[span]]></category>
		<category><![CDATA[spite]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/the-primordial-li-abundance-derived-from-giant-stars/</guid>
		<description><![CDATA[In this contribution we discuss the use of the surface Li abundance in lower RGB stars as alternative diagnostic of the primordial Li abundance. These stars are located in the portion of the RGB after the completion of the First Dredge-Up and before the extra-mixing episode occurring at the RGB Bump magnitude level. They are [...]]]></description>
			<content:encoded><![CDATA[<p>In this contribution we discuss the use of the surface Li abundance in lower RGB stars as alternative diagnostic of the primordial Li abundance. These stars are located in the portion of the RGB after the completion of the First Dredge-Up and before the extra-mixing episode occurring at the RGB Bump magnitude level. They are sensitive to the total Li content left at the end of the Main Sequence phase and are significantly less sensitive to the efficiency of atomic diffusion when compared with dwarf stars. We analysed lower RGB stars in the Galactic Halo and in the globular clusters NGC 6397, NGC 6752 and M4. The final estimates of initial A(Li) span a narrow range of values (between 2.28 and 2.46 dex), in good agreement with the Spite Plateau and confirming the discrepancy with the values obtained from the standard Big Bang nucleosynthesis calculations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/the-primordial-li-abundance-derived-from-giant-stars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Mid-Infrared Extinction Mapping of Infrared Dark Clouds II. The Structure of Massive Starless Cores and Clumps</title>
		<link>http://voxcharta.org/2012/05/13/mid-infrared-extinction-mapping-of-infrared-dark-clouds-ii-the-structure-of-massive-starless-cores-and-clumps/</link>
		<comments>http://voxcharta.org/2012/05/13/mid-infrared-extinction-mapping-of-infrared-dark-clouds-ii-the-structure-of-massive-starless-cores-and-clumps/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:50:57 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[clump]]></category>
		<category><![CDATA[cm 2]]></category>
		<category><![CDATA[core]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[density profile]]></category>
		<category><![CDATA[extinction]]></category>
		<category><![CDATA[galactic foreground]]></category>
		<category><![CDATA[infrared dark clouds]]></category>
		<category><![CDATA[law index]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[mapping technique]]></category>
		<category><![CDATA[mass surface]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[saturation]]></category>
		<category><![CDATA[sigma c]]></category>
		<category><![CDATA[sphere]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[tentative evidence]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/mid-infrared-extinction-mapping-of-infrared-dark-clouds-ii-the-structure-of-massive-starless-cores-and-clumps/</guid>
		<description><![CDATA[(abridged) We develop the mid-infrared extinction (MIREX) mapping technique of Butler &#38; Tan (2009, Paper I), presenting a new method to correct for the Galactic foreground emission based on observed saturation in independent cores. Using Spitzer GLIMPSE 8 micron images, this allows us to accurately probe mass surface densities, Sigma, up to ~0.5g/cm^2 with 2&#8243; [...]]]></description>
			<content:encoded><![CDATA[<p>(abridged) We develop the mid-infrared extinction (MIREX) mapping technique of Butler &amp; Tan (2009, Paper I), presenting a new method to correct for the Galactic foreground emission based on observed saturation in independent cores. Using Spitzer GLIMPSE 8 micron images, this allows us to accurately probe mass surface densities, Sigma, up to ~0.5g/cm^2 with 2&#8243; resolution. We then characterize the structure of 42 massive starless and early-stage IRDC cores and their surrounding clumps, measuring Sigma_cl(r) from the core/clump centers. We first assess the properties of the core/clump at a scale where the total enclosed mass as projected on the sky is M_cl=60Msun. We find these objects have a mean radius of R_cl~0.1pc, mean Sigma_cl=0.3g/cm^2 and, if fit by a power law density profile rho_cl ~ r^{-k_{rho,cl}}, a mean value of k_{rho,cl}=1.1. If we assume a core is embedded in each clump and subtract the surrounding clump envelope to derive the core properties, we find a mean core density power law index of k_{rho,c} = 1.6. We repeat this analysis as a function of radius and derive the best-fitting power law plus uniform clump envelope model for each of the 42 core/clumps. The cores have typical masses of M_c~100Msun and mean Sigma_c~0.1g/cm^2, and are embedded in clumps with comparable mass surface densities. We conclude massive starless cores exist and are well-described by singular polytropic spheres. Their relatively low values of Sigma and the fact that they are IR dark may imply that their fragmentation is inhibited by magnetic fields rather than radiative heating. Comparing to massive star-forming cores, there is tentative evidence for an evolution towards higher densities and steeper density profiles as star formation proceeds.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/mid-infrared-extinction-mapping-of-infrared-dark-clouds-ii-the-structure-of-massive-starless-cores-and-clumps/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Determination of Electromagnetic Source Direction as an Eigenvalue Problem</title>
		<link>http://voxcharta.org/2012/05/13/determination-of-electromagnetic-source-direction-as-an-eigenvalue-problem/</link>
		<comments>http://voxcharta.org/2012/05/13/determination-of-electromagnetic-source-direction-as-an-eigenvalue-problem/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:50:30 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[29 january]]></category>
		<category><![CDATA[antenna system]]></category>
		<category><![CDATA[apparent source]]></category>
		<category><![CDATA[compact source]]></category>
		<category><![CDATA[decomposition technique]]></category>
		<category><![CDATA[dimensional manifold]]></category>
		<category><![CDATA[direct characterization]]></category>
		<category><![CDATA[eigenvalue decomposition]]></category>
		<category><![CDATA[eigenvalue problem]]></category>
		<category><![CDATA[ionospheric plasma]]></category>
		<category><![CDATA[linear regression]]></category>
		<category><![CDATA[onset time]]></category>
		<category><![CDATA[polarization]]></category>
		<category><![CDATA[radio bursts]]></category>
		<category><![CDATA[radio type]]></category>
		<category><![CDATA[relative timing]]></category>
		<category><![CDATA[solar phys]]></category>
		<category><![CDATA[source location]]></category>
		<category><![CDATA[travel time]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/determination-of-electromagnetic-source-direction-as-an-eigenvalue-problem/</guid>
		<description><![CDATA[Low-frequency solar and interplanetary radio bursts are generated at frequencies below the ionospheric plasma cutoff and must therefore be measured in space, with deployable antenna systems. The problem of measuring both the general direction and polarization of an electromagnetic source is commonly solved by iterative fitting methods such as linear regression that deal simultaneously with [...]]]></description>
			<content:encoded><![CDATA[<p>Low-frequency solar and interplanetary radio bursts are generated at frequencies below the ionospheric plasma cutoff and must therefore be measured in space, with deployable antenna systems. The problem of measuring both the general direction and polarization of an electromagnetic source is commonly solved by iterative fitting methods such as linear regression that deal simultaneously with both directional and polarization parameters. We have developed a scheme that separates the problem of deriving the source direction from that of determining the polarization, avoiding iteration in a multi-dimensional manifold. The crux of the method is to first determine the source direction independently of concerns as to its polarization. Once the source direction is known, its direct characterization in terms of Stokes vectors in a single iteration if desired, is relatively simple. This study applies the source-direction determination to radio signatures of flares received by STEREO. We studied two previously analyzed radio type III bursts and found that the results of the eigenvalue decomposition technique are consistent with those obtained previously by Reiner et al. (Solar Phys. 259, 255, 2009). For the type III burst observed on 7 December 2007, the difference in travel times from the derived source location to STEREO A and B is the same as the difference in the onset times of the burst profiles measured by the two spacecraft. This is consistent with emission originating from a single, relatively compact source. For the second event of 29 January 2008, the relative timing does not agree, suggesting emission from two sources separated by 0.1 AU, or perhaps from an elongated region encompassing the apparent source locations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/determination-of-electromagnetic-source-direction-as-an-eigenvalue-problem/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>The birth rate of SNe Ia from DD systems and CD systems</title>
		<link>http://voxcharta.org/2012/05/13/the-birth-rate-of-sne-ia-from-dd-systems-and-cd-systems/</link>
		<comments>http://voxcharta.org/2012/05/13/the-birth-rate-of-sne-ia-from-dd-systems-and-cd-systems/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:44:42 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[algorithm]]></category>
		<category><![CDATA[binary evolution]]></category>
		<category><![CDATA[birth rate]]></category>
		<category><![CDATA[cd systems]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[delay time]]></category>
		<category><![CDATA[dominant channel]]></category>
		<category><![CDATA[efficiency]]></category>
		<category><![CDATA[formalism]]></category>
		<category><![CDATA[gyr]]></category>
		<category><![CDATA[monte carlo simulation]]></category>
		<category><![CDATA[observation]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[shape]]></category>
		<category><![CDATA[SNe]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/the-birth-rate-of-sne-ia-from-dd-systems-and-cd-systems/</guid>
		<description><![CDATA[We make a series of Monte Carlo simulations by a rapid binary evolution code and take two treatments of CE evolution, i.e. $\alpha$-formalism and $\gamma$-algorithm. We find that only for the $\alpha$-formalism with a high CE ejection efficiency, the shape of DTD from DD systems may be consistent with that derived observationally, i.e. a power [...]]]></description>
			<content:encoded><![CDATA[<p>We make a series of Monte Carlo simulations by a rapid binary evolution code and take two treatments of CE evolution, i.e. $\alpha$-formalism and $\gamma$-algorithm. We find that only for the $\alpha$-formalism with a high CE ejection efficiency, the shape of DTD from DD systems may be consistent with that derived observationally, i.e. a power low of $\sim t^{\rm -1}$, while the value of the birth rate of SNe Ia marginally matches with observations. For the $\alpha$-formalism with a low CE ejection efficiency and the $\gamma$-algorithm, neither the shape of DTD nor the value of the birth rate can be compared with that from observations. Metallicity may not significantly change the shape of DTD, but a low metallicity may slightly increase the birth rate of SNe Ia by a factor of 2, especially for SNe Ia with long delay times. If the results from the single degenerate (SD) channel is incorporated into the DTD, both the shape of DTD and its value may be well consistent with observations for SNe Ia of younger than 2.5 Gyr, and SD and DD channels show a comparable contribution to total SNe Ia, while for SNe Ia with delay time longer than 2.5 Gyr, DD is the dominant channel and the birth rate is lower than that derived from observation by a factor up to $\sim4$. In addition, we calculate the evolution of various integral parameters of DD systems, and do not find any one suitable to explain the correlation between the brightness of SNe Ia and its delay time. Moreover, there are three channels producing core-degenerate(CD) systems which may contribute a few SNe Ia, but the contribution from CD systems to total SNe Ia is not more than 1%.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/the-birth-rate-of-sne-ia-from-dd-systems-and-cd-systems/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Orbital properties of an unusually low-mass sdB star in a close binary system with a white dwarf</title>
		<link>http://voxcharta.org/2012/05/13/orbital-properties-of-an-unusually-low-mass-sdb-star-in-a-close-binary-system-with-a-white-dwarf/</link>
		<comments>http://voxcharta.org/2012/05/13/orbital-properties-of-an-unusually-low-mass-sdb-star-in-a-close-binary-system-with-a-white-dwarf/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:44:11 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[arcsec]]></category>
		<category><![CDATA[atmospheric parameters]]></category>
		<category><![CDATA[binary system]]></category>
		<category><![CDATA[deformation]]></category>
		<category><![CDATA[flash loop]]></category>
		<category><![CDATA[gravitational field]]></category>
		<category><![CDATA[horizontal branch]]></category>
		<category><![CDATA[kepler]]></category>
		<category><![CDATA[light curve]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[maximum inclination]]></category>
		<category><![CDATA[odot]]></category>
		<category><![CDATA[orbital frequency]]></category>
		<category><![CDATA[orbital period]]></category>
		<category><![CDATA[photometric data]]></category>
		<category><![CDATA[radial velocity]]></category>
		<category><![CDATA[rare object]]></category>
		<category><![CDATA[similar systems]]></category>
		<category><![CDATA[white dwarf]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/orbital-properties-of-an-unusually-low-mass-sdb-star-in-a-close-binary-system-with-a-white-dwarf/</guid>
		<description><![CDATA[We have used 605 days of photometric data from the Kepler spacecraft to study KIC 6614501, a close binary system with an orbital period of 0.15749747(25) days (3.779939 hours), that consists of a low-mass subdwarf B (sdB) star and a white dwarf. As seen in many other similar systems, the gravitational field of the white [...]]]></description>
			<content:encoded><![CDATA[<p>We have used 605 days of photometric data from the Kepler spacecraft to study KIC 6614501, a close binary system with an orbital period of 0.15749747(25) days (3.779939 hours), that consists of a low-mass subdwarf B (sdB) star and a white dwarf. As seen in many other similar systems, the gravitational field of the white dwarf produces an ellipsoidal deformation of the sdB which appears in the light curve as a modulation at two times the orbital frequency. The ellipsoidal deformation of the sdB implies that the system has a maximum inclination of \sim40 degrees, with i \approx 20\degrees being the most likely. The orbital radial velocity of the sdB star is high enough to produce a Doppler beaming effect with an amplitude of 432 \pm 5 ppm, clearly visible in the folded light curve. The photometric amplitude that we obtain, K1 = 85.8 km/s, is \sim 12 per cent less than the spectroscopic RV amplitude of 97.2 \pm 2.0 km/s. The discrepancy is due to the photometric contamination from a close object at about 5 arcsec North West of KIC 6614501, which is difficult to remove. The atmospheric parameters of the sdB star, Teff = 23 700 \pm 500 K and log g = 5.70 \pm 0.10, imply that it is a rare object below the Extreme Horizontal Branch (EHB), similar to HD 188112 (Heber et al. 2003). The comparison with different evolutionary tracks suggests a mass between \sim 0.18 and \sim 0.25 M\odot, too low to sustain core helium burning. If the mass was close to 0.18-0.19 M\odot, the star could be already on the final He-core WD cooling track. A higher mass, up to \sim0.25 M\odot, would be compatible with a He-core WD progenitor undergoing a cooling phase in a H-shell flash loop. A third possibility, with a mass between \sim0.32 and \sim0.40 M\odot, can not be excluded and would imply that the sdB is a &#8220;normal&#8221; (but with an unusually low mass) EHB star burning He&#8230;</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/orbital-properties-of-an-unusually-low-mass-sdb-star-in-a-close-binary-system-with-a-white-dwarf/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Astrophysical objects observed by the MESSENGER X-ray spectrometer during Mercury flybys</title>
		<link>http://voxcharta.org/2012/05/13/astrophysical-objects-observed-by-the-messenger-x-ray-spectrometer-during-mercury-flybys/</link>
		<comments>http://voxcharta.org/2012/05/13/astrophysical-objects-observed-by-the-messenger-x-ray-spectrometer-during-mercury-flybys/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:43:07 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astrophysical objects]]></category>
		<category><![CDATA[astrophysical sources]]></category>
		<category><![CDATA[electron flux]]></category>
		<category><![CDATA[flyby]]></category>
		<category><![CDATA[instrument field]]></category>
		<category><![CDATA[intensity]]></category>
		<category><![CDATA[magnetosphere]]></category>
		<category><![CDATA[mercury]]></category>
		<category><![CDATA[mercury flybys]]></category>
		<category><![CDATA[messenger spacecraft]]></category>
		<category><![CDATA[orbit insertion]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[ray sources]]></category>
		<category><![CDATA[ray spectrometer]]></category>
		<category><![CDATA[suprathermal electrons]]></category>
		<category><![CDATA[telemetry]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/astrophysical-objects-observed-by-the-messenger-x-ray-spectrometer-during-mercury-flybys/</guid>
		<description><![CDATA[The MESSENGER spacecraft conducted its first flyby of Mercury on 14th January 2008, followed by two subsequent encounters on 6th October 2008 and 29th September 2009, prior to Mercury orbit insertion on 18th March 2011. We have reviewed MESSENGER flight telemetry and X-ray Spectrometer observations from the first two encounters, and correlate several prominent features [...]]]></description>
			<content:encoded><![CDATA[<p>The MESSENGER spacecraft conducted its first flyby of Mercury on 14th January 2008, followed by two subsequent encounters on 6th October 2008 and 29th September 2009, prior to Mercury orbit insertion on 18th March 2011. We have reviewed MESSENGER flight telemetry and X-ray Spectrometer observations from the first two encounters, and correlate several prominent features in the data with the presence of astrophysical X-ray sources in the instrument field of view. We find that two X-ray peaks attributed in earlier work to the detection of suprathermal electrons from the Mercury magnetosphere, are likely to contain a significant number of events that are of astrophysical origin. The intensities of these two peaks cannot be explained entirely on the basis of astrophysical sources, and we support the previous suprathermal explanation but suggest that the electron fluxes derived in those studies be revised to correct for a significant astrophysical signal.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/astrophysical-objects-observed-by-the-messenger-x-ray-spectrometer-during-mercury-flybys/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Heliospheric Observations of STEREO-Directed Coronal Mass Ejections in 2008&#8211;2010: Lessons for Future Observations of Earth-Directed CMEs</title>
		<link>http://voxcharta.org/2012/05/13/heliospheric-observations-of-stereo-directed-coronal-mass-ejections-in-2008-2010-lessons-for-future-observations-of-earth-directed-cmes/</link>
		<comments>http://voxcharta.org/2012/05/13/heliospheric-observations-of-stereo-directed-coronal-mass-ejections-in-2008-2010-lessons-for-future-observations-of-earth-directed-cmes/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:42:53 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[angle]]></category>
		<category><![CDATA[arrival time]]></category>
		<category><![CDATA[cme]]></category>
		<category><![CDATA[deg]]></category>
		<category><![CDATA[distance]]></category>
		<category><![CDATA[earth]]></category>
		<category><![CDATA[geometry]]></category>
		<category><![CDATA[heliospheric observations]]></category>
		<category><![CDATA[mass ejection]]></category>
		<category><![CDATA[phi]]></category>
		<category><![CDATA[propagation]]></category>
		<category><![CDATA[situ measurement]]></category>
		<category><![CDATA[stereo spacecraft]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/heliospheric-observations-of-stereo-directed-coronal-mass-ejections-in-2008-2010-lessons-for-future-observations-of-earth-directed-cmes/</guid>
		<description><![CDATA[We present a study of coronal mass ejections (CMEs) which impacted one of the STEREO spacecraft between January 2008 and early 2010. We focus our study on 20 CMEs which were observed remotely by the Heliospheric Imagers (HIs) onboard the other STEREO spacecraft up to large heliocentric distances. We compare the predictions of the Fixed-Phi [...]]]></description>
			<content:encoded><![CDATA[<p>We present a study of coronal mass ejections (CMEs) which impacted one of the STEREO spacecraft between January 2008 and early 2010. We focus our study on 20 CMEs which were observed remotely by the Heliospheric Imagers (HIs) onboard the other STEREO spacecraft up to large heliocentric distances. We compare the predictions of the Fixed-Phi and Harmonic Mean (HM) fitting methods, which only differ by the assumed geometry of the CME. It is possible to use these techniques to determine from remote-sensing observations the CME direction of propagation, arrival time and final speed which are compared to in situ measurements. We find evidence that for large viewing angles, the HM fitting method predicts the CME direction better. However, this may be due to the fact that only wide CMEs can be successfully observed when the CME propagates more than 100 deg from the observing spacecraft. Overall eight CMEs, originating from behind the limb as seen by one of the STEREO spacecraft can be tracked and their arrival time at the other STEREO spacecraft can be successfully predicted. This includes CMEs, such as the events on 4 December 2009 and 9 April 2010, which were viewed 130 deg away from their direction of propagation. Therefore, we predict that some Earth-directed CMEs will be observed by the HIs until early 2013, when the separation between Earth and one of the STEREO spacecraft will be similar to the separation of the two STEREO spacecraft in 2009&#8211;2010.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/heliospheric-observations-of-stereo-directed-coronal-mass-ejections-in-2008-2010-lessons-for-future-observations-of-earth-directed-cmes/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Optical photometric and spectral study of the new FU Orionis object V2493 Cyg (HBC 722)</title>
		<link>http://voxcharta.org/2012/05/13/optical-photometric-and-spectral-study-of-the-new-fu-orionis-object-v2493-cyg-hbc-722/</link>
		<comments>http://voxcharta.org/2012/05/13/optical-photometric-and-spectral-study-of-the-new-fu-orionis-object-v2493-cyg-hbc-722/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:41:54 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorption spectra]]></category>
		<category><![CDATA[brightness variation]]></category>
		<category><![CDATA[comparison star]]></category>
		<category><![CDATA[cyg]]></category>
		<category><![CDATA[gulf of mexico]]></category>
		<category><![CDATA[light curve]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[light variations]]></category>
		<category><![CDATA[main sequence star]]></category>
		<category><![CDATA[outburst]]></category>
		<category><![CDATA[photographic observations]]></category>
		<category><![CDATA[photographic plate]]></category>
		<category><![CDATA[photometric data]]></category>
		<category><![CDATA[photometric observations]]></category>
		<category><![CDATA[resolution spectroscopy]]></category>
		<category><![CDATA[spectral observation]]></category>
		<category><![CDATA[spectral property]]></category>
		<category><![CDATA[spectroscopic observation]]></category>
		<category><![CDATA[t tauri]]></category>
		<category><![CDATA[target]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/optical-photometric-and-spectral-study-of-the-new-fu-orionis-object-v2493-cyg-hbc-722/</guid>
		<description><![CDATA[We present new results from optical photometric and spectroscopic observations of the eruptive pre-main sequence star V2493 Cyg (HBC 722). The object has continued to undergo significant brightness variations over the past few months and is an ideal target for follow-up observations. We carried out CCD BVRI photometric observations in the field of V2493 Cyg [...]]]></description>
			<content:encoded><![CDATA[<p>We present new results from optical photometric and spectroscopic observations of the eruptive pre-main sequence star V2493 Cyg (HBC 722). The object has continued to undergo significant brightness variations over the past few months and is an ideal target for follow-up observations. We carried out CCD BVRI photometric observations in the field of V2493 Cyg (&#8220;Gulf of Mexico&#8221;) from August 1994 to April 2012, i.e. at the pre-outburst states and during the phases of the outburst. We acquired high, medium, and low resolution spectroscopy of V2493 Cyg during the outburst. To study the pre-outburst variability of the target and construct its historical light curve, we searched for archival observations in photographic plate collections. Both CCD and photographic observations were analyzed using 15 comparison stars in the field of V2493 Cyg. The pre-outburst photographic and CCD photometric observations of V2493 Cyg show low-amplitude light variations typical of T Tauri stars. The recent photometric data show a slow light decrease from October 2010 to June 2011 followed by an increase in brightness that continued until early 2012. The spectral observations of V2493 Cyg are typical of FU Orionis stars absorption spectra with strong P Cyg profiles of H alpha and Na I D lines. On the basis of photometric monitoring performed over the past two years, the spectral properties at the maximal light, as well as the shape of long-term light curves, we confirm that the observed outburst of V2493 Cyg is of FU Orionis type.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/optical-photometric-and-spectral-study-of-the-new-fu-orionis-object-v2493-cyg-hbc-722/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Lithium production in the merging of white dwarf stars</title>
		<link>http://voxcharta.org/2012/05/13/lithium-production-in-the-merging-of-white-dwarf-stars/</link>
		<comments>http://voxcharta.org/2012/05/13/lithium-production-in-the-merging-of-white-dwarf-stars/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:41:06 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[asymptotic giant branch]]></category>
		<category><![CDATA[borealis]]></category>
		<category><![CDATA[chemical composition]]></category>
		<category><![CDATA[coronae]]></category>
		<category><![CDATA[crb]]></category>
		<category><![CDATA[formation mechanism]]></category>
		<category><![CDATA[helium]]></category>
		<category><![CDATA[hydrogen]]></category>
		<category><![CDATA[latter scenario]]></category>
		<category><![CDATA[Lithium]]></category>
		<category><![CDATA[merger]]></category>
		<category><![CDATA[new star]]></category>
		<category><![CDATA[oxygen]]></category>
		<category><![CDATA[particle hydrodynamics]]></category>
		<category><![CDATA[production mechanism]]></category>
		<category><![CDATA[sph]]></category>
		<category><![CDATA[tracer particles]]></category>
		<category><![CDATA[two theories]]></category>
		<category><![CDATA[white dwarf]]></category>
		<category><![CDATA[white dwarf star]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/lithium-production-in-the-merging-of-white-dwarf-stars/</guid>
		<description><![CDATA[The origin of R Coronae Borealis stars has been elusive for over 200 years. Currently, two theories for their formation have been presented. These are the Final Flash scenario, in which a dying asymptotic giant branch (AGB) star throws off its atmosphere to reveal the hydrogen poor, heavily processed material underneath, and the double degenerate [...]]]></description>
			<content:encoded><![CDATA[<p>The origin of R Coronae Borealis stars has been elusive for over 200 years. Currently, two theories for their formation have been presented. These are the Final Flash scenario, in which a dying asymptotic giant branch (AGB) star throws off its atmosphere to reveal the hydrogen poor, heavily processed material underneath, and the double degenerate scenario, in which two white dwarfs merge to produce a new star with renewed vigour. Some theories predict that the temperatures reached during the latter scenario would destroy any lithium originally present in the white dwarfs. The observed lithium content of some R Coronae Borealis stars, therefore, is often interpreted as an indication that the Final Flash scenario best describes their formation. In this paper, it is shown that lithium production can, indeed, occur in the merging of a helium white dwarf with a carbon-oxygen white dwarf if their chemical composition, particularly that of 3He, is fully considered. The production mechanism is described in detail, and the sensitivity of lithium production to the merger environment is investigated. Nucleosynthesis post-processing calculations of smoothed-particle hydrodynamics (SPH) tracer particles are performed to show that any lithium produced in these environments will be concentrated towards the cloud of material surrounding the R CrB star. Measurements of the lithium content of these clouds would, therefore, provide a valuable insight into the formation mechanism of R CrB stars.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/lithium-production-in-the-merging-of-white-dwarf-stars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>CME acceleration and non-thermal flare characteristics</title>
		<link>http://voxcharta.org/2012/05/13/cme-acceleration-and-non-thermal-flare-characteristics/</link>
		<comments>http://voxcharta.org/2012/05/13/cme-acceleration-and-non-thermal-flare-characteristics/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:40:44 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration phase]]></category>
		<category><![CDATA[cme]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[correlation coefficient]]></category>
		<category><![CDATA[current sheet]]></category>
		<category><![CDATA[electron]]></category>
		<category><![CDATA[flare]]></category>
		<category><![CDATA[initiation]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetic reconnection]]></category>
		<category><![CDATA[mass ejection]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[particle acceleration]]></category>
		<category><![CDATA[peak acceleration]]></category>
		<category><![CDATA[peak velocity]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectral index]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/cme-acceleration-and-non-thermal-flare-characteristics/</guid>
		<description><![CDATA[We investigate the relationship between the main acceleration phase of coronal mass ejections (CMEs) and the particle acceleration in the associated flares as evidenced in RHESSI non-thermal X-rays for a set of 37 impulsive flare-CME events. CME peak velocity and peak acceleration yield distinct correlations with various parameters characterizing the flare-accelerated electron spectra. The highest [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate the relationship between the main acceleration phase of coronal mass ejections (CMEs) and the particle acceleration in the associated flares as evidenced in RHESSI non-thermal X-rays for a set of 37 impulsive flare-CME events. CME peak velocity and peak acceleration yield distinct correlations with various parameters characterizing the flare-accelerated electron spectra. The highest correlation coefficient is obtained for the relation of the CME peak velocity and the total energy in accelerated electrons (c = 0.85), supporting the idea that the acceleration of the CME and the particle acceleration in the associated flare draw their energy from a common source, probably magnetic reconnection in the current sheet behind the erupting structure. In general, the CME peak velocity shows somewhat higher correlations with the non-thermal flare parameters than the CME peak acceleration, except for the spectral index of the accelerated electron spectrum which yields a higher correlation with the CME peak acceleration (c = -0.6), indicating that the hardness of the flare-accelerated electron spectrum is tightly coupled to the impulsive acceleration process of the rising CME structure. We also obtained high correlations between the CME initiation height $h_0$ and the non-thermal flare parameters, with the highest correlation of $h_0$ to the spectral index of flare-accelerated electrons (c = 0.8). This means that CMEs erupting at low coronal heights, i.e.\ in regions of stronger magnetic fields, are accompanied with flares which are more efficient to accelerate electrons to high energies. In the majority of events (80%), the non-thermal flare emission starts after the CME acceleration (6 min), giving a current sheet length at the onset of magnetic reconnection of 21 \pm 7 Mm. The flare HXR peaks are well synchronized with the peak of the CME acceleration profile.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/cme-acceleration-and-non-thermal-flare-characteristics/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A survey of Nulling pulsars using Giant Meterwave Radio Telescope</title>
		<link>http://voxcharta.org/2012/05/13/a-survey-of-nulling-pulsars-using-giant-meterwave-radio-telescope/</link>
		<comments>http://voxcharta.org/2012/05/13/a-survey-of-nulling-pulsars-using-giant-meterwave-radio-telescope/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:39:30 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[burst]]></category>
		<category><![CDATA[cessation]]></category>
		<category><![CDATA[detail analysis]]></category>
		<category><![CDATA[distributions]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[full detail]]></category>
		<category><![CDATA[interval]]></category>
		<category><![CDATA[null phase]]></category>
		<category><![CDATA[pulsars]]></category>
		<category><![CDATA[pulse energy]]></category>
		<category><![CDATA[pulses]]></category>
		<category><![CDATA[radio telescope]]></category>
		<category><![CDATA[stochastic poisson]]></category>
		<category><![CDATA[time scale]]></category>
		<category><![CDATA[transition]]></category>
		<category><![CDATA[vice verse]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/a-survey-of-nulling-pulsars-using-giant-meterwave-radio-telescope/</guid>
		<description><![CDATA[Several pulsars show sudden cessation of pulsed emission, which is known as pulsar nulling. In this paper, the nulling behaviour of 15 pulsars is presented. The nulling fractions of these pulsars, along with the degree of reduction in the pulse energy during the null phase, are reported for these pulsars. A quasi-periodic null-burst pattern is [...]]]></description>
			<content:encoded><![CDATA[<p>Several pulsars show sudden cessation of pulsed emission, which is known as pulsar nulling. In this paper, the nulling behaviour of 15 pulsars is presented. The nulling fractions of these pulsars, along with the degree of reduction in the pulse energy during the null phase, are reported for these pulsars. A quasi-periodic null-burst pattern is reported for PSR J1738-2330. The distributions of lengths of the null and the burst phases as well as the typical nulling time scales are estimated for eight strong pulsars. The nulling pattern of four pulsars with similar nulling fraction are found to be different from each other, suggesting that the fraction of null pulses does not quantify the nulling behaviour of a pulsar in full detail. Analysis of these distributions also indicate that while the null and the burst pulses occur in groups, the underlying distribution of the interval between a transition from the null to the burst phase and vice verse appears to be similar to that of a stochastic Poisson point process.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/a-survey-of-nulling-pulsars-using-giant-meterwave-radio-telescope/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>HST and Optical Data Reveal White Dwarf Cooling, Spin and Periodicities in GW Librae 3-4 Years after Outburst</title>
		<link>http://voxcharta.org/2012/05/13/hst-and-optical-data-reveal-white-dwarf-cooling-spin-and-periodicities-in-gw-librae-3-4-years-after-outburst/</link>
		<comments>http://voxcharta.org/2012/05/13/hst-and-optical-data-reveal-white-dwarf-cooling-spin-and-periodicities-in-gw-librae-3-4-years-after-outburst/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:37:57 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[300k]]></category>
		<category><![CDATA[absorption line]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[dwarf nova]]></category>
		<category><![CDATA[gravitational redshift]]></category>
		<category><![CDATA[hubble space telescope]]></category>
		<category><![CDATA[inclination]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[nova system]]></category>
		<category><![CDATA[optical coverage]]></category>
		<category><![CDATA[optical data]]></category>
		<category><![CDATA[outburst]]></category>
		<category><![CDATA[quiescence]]></category>
		<category><![CDATA[radial pulsations]]></category>
		<category><![CDATA[rotation velocity]]></category>
		<category><![CDATA[timescale]]></category>
		<category><![CDATA[ultraviolet spectra]]></category>
		<category><![CDATA[uv spectra]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/hst-and-optical-data-reveal-white-dwarf-cooling-spin-and-periodicities-in-gw-librae-3-4-years-after-outburst/</guid>
		<description><![CDATA[Since the large amplitude 2007 outburst which heated its accreting, pulsating white dwarf, the dwarf nova system GW Librae has been cooling to its quiescent temperature. Our Hubble Space Telescope ultraviolet spectra combined with ground-based optical coverage during the 3rd and 4th year after outburst show that the fluxes and temperatures are still higher than [...]]]></description>
			<content:encoded><![CDATA[<p>Since the large amplitude 2007 outburst which heated its accreting, pulsating white dwarf, the dwarf nova system GW Librae has been cooling to its quiescent temperature. Our Hubble Space Telescope ultraviolet spectra combined with ground-based optical coverage during the 3rd and 4th year after outburst show that the fluxes and temperatures are still higher than quiescence (T=19,700K and 17,300K vs 16,000K pre-outburst for a log g=8.7 and d=100 pc). The K{wd} of 7.6+/-0.8 km/s determined from the CI1463 absorption line, as well as the gravitational redshift implies a white dwarf mass of 0.79+/-0.08 Msun. The widths of the UV lines imply a white dwarf rotation velocity vsin i of 40 km/s and a spin period of 209 s (for an inclination of 11 deg and a white dwarf radius of 7&#215;10^{8} cm). Light curves produced from the UV spectra in both years show a prominent multiplet near 290 s, with higher amplitude in the UV compared to the optical, and increased amplitude in 2011 vs 2010. As the presence of this set of periods is intermittent in the optical on weekly timescales, it is unclear how this relates to the non-radial pulsations evident during quiescence.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/hst-and-optical-data-reveal-white-dwarf-cooling-spin-and-periodicities-in-gw-librae-3-4-years-after-outburst/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A CME-driven shock analysis of the 14-Dec-2006 SEP event [Replacement]</title>
		<link>http://voxcharta.org/2012/05/13/a-cme-driven-shock-analysis-of-the-14-dec-2006-sep-event-replacement/</link>
		<comments>http://voxcharta.org/2012/05/13/a-cme-driven-shock-analysis-of-the-14-dec-2006-sep-event-replacement/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:35:23 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[anisotropic]]></category>
		<category><![CDATA[energy injection]]></category>
		<category><![CDATA[energy spectrum]]></category>
		<category><![CDATA[interplanetary shock]]></category>
		<category><![CDATA[mass ejection]]></category>
		<category><![CDATA[mev energy]]></category>
		<category><![CDATA[monte carlo simulation]]></category>
		<category><![CDATA[particle acceleration]]></category>
		<category><![CDATA[shock acceleration]]></category>
		<category><![CDATA[shock structure]]></category>
		<category><![CDATA[simulation result]]></category>
		<category><![CDATA[solar flare]]></category>
		<category><![CDATA[spacecraft]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/a-cme-driven-shock-analysis-of-the-14-dec-2006-sep-event-replacement/</guid>
		<description><![CDATA[Observations of the interplanetary shock provide us with strong evidence of particle acceleration to multi-MeV energies, even up to GeV energy, in a solar flare or coronal mass ejection (CME). Diffusive shock acceleration is an efficient mechanism for particle acceleration. For investigating the shock structure, the energy injection and energy spectrum of a CME-driven shock, [...]]]></description>
			<content:encoded><![CDATA[<p>Observations of the interplanetary shock provide us with strong evidence of particle acceleration to multi-MeV energies, even up to GeV energy, in a solar flare or coronal mass ejection (CME). Diffusive shock acceleration is an efficient mechanism for particle acceleration. For investigating the shock structure, the energy injection and energy spectrum of a CME-driven shock, we perform dynamical Monte Carlo simulation of the 14-Dec-2006 CME-driven shock using an anisotropic scattering law. The simulated results of the shock fine structure, particle injection, and energy spectrum are presented. We find that our simulation results give a good fit to the observations from multiple spacecraft.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/a-cme-driven-shock-analysis-of-the-14-dec-2006-sep-event-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Triggered star formation surrounding Wolf-Rayet star HD 211853 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/13/triggered-star-formation-surrounding-wolf-rayet-star-hd-211853-replacement/</link>
		<comments>http://voxcharta.org/2012/05/13/triggered-star-formation-surrounding-wolf-rayet-star-hd-211853-replacement/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:34:43 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[core]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[fragmentation]]></category>
		<category><![CDATA[gravitational collapse]]></category>
		<category><![CDATA[hi emission]]></category>
		<category><![CDATA[infrared emission]]></category>
		<category><![CDATA[ionized gas]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[large scale]]></category>
		<category><![CDATA[molecular emission]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[radiation]]></category>
		<category><![CDATA[radio]]></category>
		<category><![CDATA[sequential star formation]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[star hd]]></category>
		<category><![CDATA[stellar object]]></category>
		<category><![CDATA[wolf]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/triggered-star-formation-surrounding-wolf-rayet-star-hd-211853-replacement/</guid>
		<description><![CDATA[The environment surrounding Wolf-Rayet star HD 211853 is studied in molecular emission, infrared emission, as well as radio and HI emission. The molecular ring consists of well-separated cores, which have a volume density of 10$^{3}$ cm$^{-3}$ and kinematic temperature $\sim$20 K. Most of the cores are under gravitational collapse due to external pressure from the [...]]]></description>
			<content:encoded><![CDATA[<p>The environment surrounding Wolf-Rayet star HD 211853 is studied in molecular emission, infrared emission, as well as radio and HI emission. The molecular ring consists of well-separated cores, which have a volume density of 10$^{3}$ cm$^{-3}$ and kinematic temperature $\sim$20 K. Most of the cores are under gravitational collapse due to external pressure from the surrounding ionized gas. From SED modeling towards the young stellar objects (YSOs), sequential star formation is revealed on a large scale in space spreading from the Wolf-Rayet star to the molecular ring. A small scale sequential star formation is revealed towards core A, which harbors a very young star cluster. Triggered star formations is thus suggested. The presence of PDR, the fragmentation of the molecular ring, the collapse of the cores, the large scale sequential star formation indicate the &#8220;Collect and Collapse&#8221; process functions in this region. The star forming activities in core A seem to be affected by the &#8220;Radiation-Driven Implosion&#8221; (RDI) process.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/triggered-star-formation-surrounding-wolf-rayet-star-hd-211853-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Rapid Coagulation of Porous Dust Aggregates Outside the Snow Line: A Pathway to Successful Icy Planetesimal Formation [Replacement]</title>
		<link>http://voxcharta.org/2012/05/13/rapid-coagulation-of-porous-dust-aggregates-outside-the-snow-line-a-pathway-to-successful-icy-planetesimal-formation-replacement/</link>
		<comments>http://voxcharta.org/2012/05/13/rapid-coagulation-of-porous-dust-aggregates-outside-the-snow-line-a-pathway-to-successful-icy-planetesimal-formation-replacement/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:33:11 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration]]></category>
		<category><![CDATA[aggregate]]></category>
		<category><![CDATA[body simulation]]></category>
		<category><![CDATA[cm 3]]></category>
		<category><![CDATA[coagulation]]></category>
		<category><![CDATA[collisions]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[dust particle]]></category>
		<category><![CDATA[fragmentation]]></category>
		<category><![CDATA[gas molecule]]></category>
		<category><![CDATA[knudsen]]></category>
		<category><![CDATA[mean free path]]></category>
		<category><![CDATA[natural consequence]]></category>
		<category><![CDATA[orbital drift]]></category>
		<category><![CDATA[orbital radii]]></category>
		<category><![CDATA[planetesimal]]></category>
		<category><![CDATA[porosity evolution]]></category>
		<category><![CDATA[rapid growth]]></category>
		<category><![CDATA[snow line]]></category>
		<category><![CDATA[solar nebula]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/rapid-coagulation-of-porous-dust-aggregates-outside-the-snow-line-a-pathway-to-successful-icy-planetesimal-formation-replacement/</guid>
		<description><![CDATA[Rapid orbital drift of macroscopic dust particles is one of the major obstacles against planetesimal formation in protoplanetary disks. We reexamine this problem by considering porosity evolution of dust aggregates. We apply a porosity model based on recent N-body simulations of aggregate collisions, which allows us to study the porosity change upon collision for a [...]]]></description>
			<content:encoded><![CDATA[<p>Rapid orbital drift of macroscopic dust particles is one of the major obstacles against planetesimal formation in protoplanetary disks. We reexamine this problem by considering porosity evolution of dust aggregates. We apply a porosity model based on recent N-body simulations of aggregate collisions, which allows us to study the porosity change upon collision for a wide range of impact energies. As a first step, we neglect collisional fragmentation and instead focus on dust evolution outside the snow line, where the fragmentation has been suggested to be less significant than inside the snow line because of a high sticking efficiency of icy particles. We show that dust particles can evolve into highly porous aggregates (with internal densities of much less than 0.1 g/cm^3) even if collisional compression is taken into account. We also show that the high porosity triggers significant acceleration in collisional growth. This acceleration is a natural consequence of particles&#8217; aerodynamical property at low Knudsen numbers, i.e., at particle radii larger than the mean free path of the gas molecules. Thanks to this rapid growth, the highly porous aggregates are found to overcome the radial drift barrier at orbital radii less than 10 AU (assuming the minimum-mass solar nebula model). This suggests that, if collisional fragmentation is truly insignificant, formation of icy planetesimals is possible via direct collisional growth of submicron-sized icy particles.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/rapid-coagulation-of-porous-dust-aggregates-outside-the-snow-line-a-pathway-to-successful-icy-planetesimal-formation-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Particle Acceleration at a Flare Termination Shock: Effect of Large-scale Magnetic Turbulence [Replacement]</title>
		<link>http://voxcharta.org/2012/05/13/particle-acceleration-at-a-flare-termination-shock-effect-of-large-scale-magnetic-turbulence-replacement/</link>
		<comments>http://voxcharta.org/2012/05/13/particle-acceleration-at-a-flare-termination-shock-effect-of-large-scale-magnetic-turbulence-replacement/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:33:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[amplitude level]]></category>
		<category><![CDATA[collisionless shocks]]></category>
		<category><![CDATA[electron acceleration]]></category>
		<category><![CDATA[electrons and protons]]></category>
		<category><![CDATA[energy spectra]]></category>
		<category><![CDATA[flare loops]]></category>
		<category><![CDATA[flare plasma]]></category>
		<category><![CDATA[hybrid simulation]]></category>
		<category><![CDATA[magnetic fluctuations]]></category>
		<category><![CDATA[magnetic turbulence]]></category>
		<category><![CDATA[numerical simulation]]></category>
		<category><![CDATA[particle acceleration]]></category>
		<category><![CDATA[plasma environment]]></category>
		<category><![CDATA[plasma flow]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[shock effect]]></category>
		<category><![CDATA[solar flare]]></category>
		<category><![CDATA[termination shock]]></category>
		<category><![CDATA[test particle]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/particle-acceleration-at-a-flare-termination-shock-effect-of-large-scale-magnetic-turbulence-replacement/</guid>
		<description><![CDATA[We investigate the acceleration of charged particles (both electrons and protons) at collisionless shocks predicted to exist in the vicinity of solar flares. The existence of standing termination shocks has been examined by flare models and numerical simulations e.g., Shibata,Forbes. We study electron energization by numerically integrating the equations of motion of a large number [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate the acceleration of charged particles (both electrons and protons) at collisionless shocks predicted to exist in the vicinity of solar flares. The existence of standing termination shocks has been examined by flare models and numerical simulations e.g., Shibata,Forbes. We study electron energization by numerically integrating the equations of motion of a large number of test-particle electrons in the time-dependent two-dimensional electric and magnetic fields generated from hybrid simulations (kinetic ions and fluid electron) using parameters typical of the solar flare plasma environment. The shock is produced by injecting plasma flow toward a rigid piston. Large-scale magnetic fluctuations &#8212; known to exist in plasmas and known to have important effects on the nonthermal electron acceleration at shocks &#8212; are also included in our simulations. For the parameters characteristic of the flaring region, our calculations suggest that the termination shock formed in the reconnection outflow region (above post-flare loops) could accelerate electrons to a kinetic energy of a few MeV within 100 ion cyclotron periods, which is of the order of a millisecond. Given a sufficient turbulence amplitude level ($\delta B^2/B_0^2 \sim 0.3$), about 10% of thermal test-particle electrons are accelerated to more than 15 keV. We find that protons are also accelerated, but not to as high energy in the available time and the energy spectra are considerably steeper than that of the electrons for the parameters used in our simulations. Our results are qualitatively consistent with the observed hard X-ray emissions in solar flares.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/particle-acceleration-at-a-flare-termination-shock-effect-of-large-scale-magnetic-turbulence-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Chromospheric jets around the edges of sunspots [Replacement]</title>
		<link>http://voxcharta.org/2012/05/13/chromospheric-jets-around-the-edges-of-sunspots-replacement/</link>
		<comments>http://voxcharta.org/2012/05/13/chromospheric-jets-around-the-edges-of-sunspots-replacement/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:31:20 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[chromosphere]]></category>
		<category><![CDATA[continuous series]]></category>
		<category><![CDATA[corona]]></category>
		<category><![CDATA[disappearance]]></category>
		<category><![CDATA[evidence suggests that]]></category>
		<category><![CDATA[hinode]]></category>
		<category><![CDATA[jets]]></category>
		<category><![CDATA[leading edge]]></category>
		<category><![CDATA[region dynamics]]></category>
		<category><![CDATA[region features]]></category>
		<category><![CDATA[shock front]]></category>
		<category><![CDATA[sunspot]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/chromospheric-jets-around-the-edges-of-sunspots-replacement/</guid>
		<description><![CDATA[Evidence is beginning to be put forward that demonstrates the role of the chromosphere in supplying energy and mass to the corona. We aim to assess the role of chromospheric jets in active region dynamics. Using a combination of the Hinode/SOT Ca II H and TRACE 1550 {\AA} and 1600 {\AA} filters we examine chromospheric [...]]]></description>
			<content:encoded><![CDATA[<p>Evidence is beginning to be put forward that demonstrates the role of the chromosphere in supplying energy and mass to the corona. We aim to assess the role of chromospheric jets in active region dynamics. Using a combination of the Hinode/SOT Ca II H and TRACE 1550 {\AA} and 1600 {\AA} filters we examine chromospheric jets situated at the edge of a sunspot. Analysis reveals a near continuous series of jets, that raise chromospheric material into the low corona above a sunspot. The jets have average rise speeds of 30 km\,s^{-1} and a range of 10-100km\,s^{-1}. Enhanced emission observed at the jets leading edge suggests the formation of a shock front. Increased emission in TRACE bandpasses above the sunspot and the disappearance of the jets from the Ca II filter suggests that some of the chromospheric jet material is at least heated to \sim0.1MK. The evidence suggests that the jets could be a mechanism which provides a steady, low-level heating for active region features.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/chromospheric-jets-around-the-edges-of-sunspots-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Planets Around Low-Mass Stars (PALMS). I. A Substellar Companion to the Young M Dwarf 1RXS J235133.3+312720</title>
		<link>http://voxcharta.org/2012/05/10/planets-around-low-mass-stars-palms-i-a-substellar-companion-to-the-young-m-dwarf-1rxs-j235133-3312720/</link>
		<comments>http://voxcharta.org/2012/05/10/planets-around-low-mass-stars-palms-i-a-substellar-companion-to-the-young-m-dwarf-1rxs-j235133-3312720/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:46:41 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[brown dwarf companion]]></category>
		<category><![CDATA[brown dwarf lp]]></category>
		<category><![CDATA[companion cd]]></category>
		<category><![CDATA[epochs]]></category>
		<category><![CDATA[evolutionary model]]></category>
		<category><![CDATA[high resolution imaging]]></category>
		<category><![CDATA[infrared spectroscopy]]></category>
		<category><![CDATA[infrared spectrum]]></category>
		<category><![CDATA[irtf]]></category>
		<category><![CDATA[keck ii]]></category>
		<category><![CDATA[mass star]]></category>
		<category><![CDATA[moderate resolution]]></category>
		<category><![CDATA[photometric]]></category>
		<category><![CDATA[radial velocity]]></category>
		<category><![CDATA[spectral type]]></category>
		<category><![CDATA[spex]]></category>
		<category><![CDATA[substellar companion]]></category>
		<category><![CDATA[subtle hints]]></category>
		<category><![CDATA[surface gravity]]></category>
		<category><![CDATA[uvw]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/planets-around-low-mass-stars-palms-i-a-substellar-companion-to-the-young-m-dwarf-1rxs-j235133-3312720/</guid>
		<description><![CDATA[We report the discovery of a brown dwarf companion to the young M dwarf 1RXS J235133.3+312720 as part of a high contrast imaging search for planets around nearby young low-mass stars with Keck-II/NIRC2 and Subaru/HiCIAO. The 2.4&#8243; (~120 AU) pair is confirmed to be comoving from two epochs of high resolution imaging. Follow-up low- and [...]]]></description>
			<content:encoded><![CDATA[<p>We report the discovery of a brown dwarf companion to the young M dwarf 1RXS J235133.3+312720 as part of a high contrast imaging search for planets around nearby young low-mass stars with Keck-II/NIRC2 and Subaru/HiCIAO. The 2.4&#8243; (~120 AU) pair is confirmed to be comoving from two epochs of high resolution imaging. Follow-up low- and moderate-resolution near-infrared spectroscopy of 1RXS J2351+3127 B with IRTF/SpeX and Keck-II/OSIRIS reveals a spectral type of L0$^{+2}_{-1}$. The M2 primary star 1RXS J2351+3127 A exhibits X-ray and UV activity levels comparable to young moving group members with ages of ~10-100 Myr. UVW kinematics based the measured radial velocity of the primary and the system&#8217;s photometric distance (50 +/- 10 pc) indicate it is likely a member of the ~50-150 Myr AB Dor moving group. The near-infrared spectrum of 1RXS J2351+3127 B does not exhibit obvious signs of youth, but its H-band morphology shows subtle hints of intermediate surface gravity. The spectrum is also an excellent match to the ~200 Myr M9 brown dwarf LP 944-20. Assuming an age of 50-150 Myr, evolutionary models imply a mass of 32 +/- 6 Mjup for the companion, making 1RXS J2351+3127 B the second lowest-mass member of the AB Dor moving group after the L4 companion CD-35 2722 B and one of the few benchmark brown dwarfs known at young ages.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/planets-around-low-mass-stars-palms-i-a-substellar-companion-to-the-young-m-dwarf-1rxs-j235133-3312720/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Simulation of multiple supra&#8211;arcade downflows in solar flares</title>
		<link>http://voxcharta.org/2012/05/10/simulation-of-multiple-supra-arcade-downflows-in-solar-flares/</link>
		<comments>http://voxcharta.org/2012/05/10/simulation-of-multiple-supra-arcade-downflows-in-solar-flares/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:46:31 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[arcade]]></category>
		<category><![CDATA[deposition]]></category>
		<category><![CDATA[expansion waves]]></category>
		<category><![CDATA[flare]]></category>
		<category><![CDATA[interaction]]></category>
		<category><![CDATA[magnetic field direction]]></category>
		<category><![CDATA[plasma]]></category>
		<category><![CDATA[sads]]></category>
		<category><![CDATA[scenarios]]></category>
		<category><![CDATA[shock]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[solar flare]]></category>
		<category><![CDATA[stable features]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/simulation-of-multiple-supra-arcade-downflows-in-solar-flares/</guid>
		<description><![CDATA[In later papers we have shown that sunward, generally dark, plasma features originated above posteruption flare arcades are consistent with a scenario where plasma voids are generated by the bouncing and interfering of shocks and expansion waves upstream of an initial localized deposition of energy which is collimated in the magnetic field direction. In this [...]]]></description>
			<content:encoded><![CDATA[<p>In later papers we have shown that sunward, generally dark, plasma features originated above posteruption flare arcades are consistent with a scenario where plasma voids are generated by the bouncing and interfering of shocks and expansion waves upstream of an initial localized deposition of energy which is collimated in the magnetic field direction. In this paper we analyze the multiple production and interaction of supra&#8211;arcade downflows (SAD) and the structure of individual SADs that make them relatively stable features while moving. We compare our results with observations and with the scenarios proposed by other authors.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/simulation-of-multiple-supra-arcade-downflows-in-solar-flares/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Chandra/ACIS-I study of the X-ray properties of the NGC 6611 and M16 stellar population</title>
		<link>http://voxcharta.org/2012/05/10/chandraacis-i-study-of-the-x-ray-properties-of-the-ngc-6611-and-m16-stellar-population/</link>
		<comments>http://voxcharta.org/2012/05/10/chandraacis-i-study-of-the-x-ray-properties-of-the-ngc-6611-and-m16-stellar-population/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:45:33 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[central cluster]]></category>
		<category><![CDATA[Chandra]]></category>
		<category><![CDATA[cluster]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[eagle nebula m16]]></category>
		<category><![CDATA[evolutionary stage]]></category>
		<category><![CDATA[mass star]]></category>
		<category><![CDATA[mechanisms]]></category>
		<category><![CDATA[protostar]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[Sun]]></category>
		<category><![CDATA[target]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/chandraacis-i-study-of-the-x-ray-properties-of-the-ngc-6611-and-m16-stellar-population/</guid>
		<description><![CDATA[Mechanisms regulating the origin of X-rays in YSOs and the correlation with their evolutionary stage are under debate. Studies of the X-ray properties in young clusters allow to understand these mechanisms. One ideal target for this analysis is the Eagle Nebula (M16), with its central cluster NGC6611. At 1750 pc from the Sun, it harbors [...]]]></description>
			<content:encoded><![CDATA[<p>Mechanisms regulating the origin of X-rays in YSOs and the correlation with their evolutionary stage are under debate. Studies of the X-ray properties in young clusters allow to understand these mechanisms. One ideal target for this analysis is the Eagle Nebula (M16), with its central cluster NGC6611. At 1750 pc from the Sun, it harbors 93 OB stars, together with a population of low-mass stars from embedded protostars to disk-less Class III objects, with age &lt;= 3Myrs. We study an archival 78 ksec Chandra/ACIS-I observation of NGC6611, and two new 80ksec observations of the outer region of M16, one centered on the Column V, and one on a region of the molecular cloud with ongoing star-formation. We detect 1755 point sources, with 1183 candidate cluster members (219 disk-bearing and 964 disk-less). We study the global X-ray properties of M16 and compare them with those of the Orion Nebula Cluster. We also compare the level of X-ray emission of Class II and Class III stars, and analyze the X-ray spectral properties of OB stars. Our study supports the lower level of X-ray activity for the disk-bearing stars with respect to the disk-less members. The X-ray Luminosity Function (XLF) of M16 is similar to that of Orion, supporting the universality of the XLF in young clusters. 85% of the O stars of NGC6611 have been detected in X-rays. With only one possible exception, they show soft spectra with no hard component, indicating that mechanisms for the production of hard X-ray emission in O stars are not operating in NGC 6611.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/chandraacis-i-study-of-the-x-ray-properties-of-the-ngc-6611-and-m16-stellar-population/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The onset of Impulsive Bursty reconnection at a two-dimensional current layer</title>
		<link>http://voxcharta.org/2012/05/10/the-onset-of-impulsive-bursty-reconnection-at-a-two-dimensional-current-layer/</link>
		<comments>http://voxcharta.org/2012/05/10/the-onset-of-impulsive-bursty-reconnection-at-a-two-dimensional-current-layer/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:45:05 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[3d studies]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[beta]]></category>
		<category><![CDATA[critical level]]></category>
		<category><![CDATA[critical value]]></category>
		<category><![CDATA[current density]]></category>
		<category><![CDATA[dispersal]]></category>
		<category><![CDATA[internal energy]]></category>
		<category><![CDATA[kinetic energy]]></category>
		<category><![CDATA[launch]]></category>
		<category><![CDATA[lorentz]]></category>
		<category><![CDATA[magnetic energy]]></category>
		<category><![CDATA[perturbation]]></category>
		<category><![CDATA[plasma]]></category>
		<category><![CDATA[pulses]]></category>
		<category><![CDATA[reconnection]]></category>
		<category><![CDATA[regime]]></category>
		<category><![CDATA[resistivity]]></category>
		<category><![CDATA[solar flare]]></category>
		<category><![CDATA[stagnation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/the-onset-of-impulsive-bursty-reconnection-at-a-two-dimensional-current-layer/</guid>
		<description><![CDATA[The sudden reconnection of a non-force free 2D current layer, embedded in a low-beta plasma, triggered by the onset of an anomalous resistivity, is studied in detail. The resulting behaviour consists of two main phases. Firstly, a transient reconnection phase, in which the current in the layer is rapidly dispersed and some flux is reconnected. [...]]]></description>
			<content:encoded><![CDATA[<p>The sudden reconnection of a non-force free 2D current layer, embedded in a low-beta plasma, triggered by the onset of an anomalous resistivity, is studied in detail. The resulting behaviour consists of two main phases. Firstly, a transient reconnection phase, in which the current in the layer is rapidly dispersed and some flux is reconnected. This dispersal of current launches a family of small amplitude magnetic and plasma perturbations, which propagate away from the null at the local fast and slow magnetosonic speeds. The vast majority of the magnetic energy released in this phase goes into internal energy of the plasma, and only a tiny amount is converted into kinetic energy. In the wake of the outwards propagating pulses, an imbalance of Lorentz and pressure forces creates a stagnation flow which drives a regime of impulsive bursty reconnection, in which fast reconnection is turned on and off in a turbulent manner as the current density exceeds and falls below a critical value. During this phase, the null current density is continuously built up above a certain critical level, then dissipated very rapidly, and built up again, in a stochastic manner. Interestingly, the magnetic energy converted during this quasi-steady phase is greater than that converted during the initial transient reconnection phase. Again essentially all the energy converted during this phase goes directly to internal energy. These results are of potential importance for solar flares and coronal heating, and set a conceptually important reference for future 3D studies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/the-onset-of-impulsive-bursty-reconnection-at-a-two-dimensional-current-layer/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Further Defining Spectral Type &quot;Y&quot; and Exploring the Low-mass End of the Field Brown Dwarf Mass Function</title>
		<link>http://voxcharta.org/2012/05/10/further-defining-spectral-type-y-and-exploring-the-low-mass-end-of-the-field-brown-dwarf-mass-function/</link>
		<comments>http://voxcharta.org/2012/05/10/further-defining-spectral-type-y-and-exploring-the-low-mass-end-of-the-field-brown-dwarf-mass-function/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:44:50 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[brown dwarf]]></category>
		<category><![CDATA[burning stars]]></category>
		<category><![CDATA[characterization]]></category>
		<category><![CDATA[constituency]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[distance]]></category>
		<category><![CDATA[hydrogen]]></category>
		<category><![CDATA[infrared survey]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[mass function]]></category>
		<category><![CDATA[parallax measurement]]></category>
		<category><![CDATA[parsec]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[slope]]></category>
		<category><![CDATA[solar neighborhood]]></category>
		<category><![CDATA[space density]]></category>
		<category><![CDATA[spectral type]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/further-defining-spectral-type-y-and-exploring-the-low-mass-end-of-the-field-brown-dwarf-mass-function/</guid>
		<description><![CDATA[We present the discovery of another seven Y dwarfs from the Wide-field Infrared Survey Explorer (WISE). Using these objects, as well as the first six WISE Y dwarf discoveries from Cushing et al., we further explore the transition between spectral types T and Y. We find that the T/Y boundary roughly coincides with the spot [...]]]></description>
			<content:encoded><![CDATA[<p>We present the discovery of another seven Y dwarfs from the Wide-field Infrared Survey Explorer (WISE). Using these objects, as well as the first six WISE Y dwarf discoveries from Cushing et al., we further explore the transition between spectral types T and Y. We find that the T/Y boundary roughly coincides with the spot where the J-H colors of brown dwarfs, as predicted by models, turn back to the red. Moreover, we use preliminary trigonometric parallax measurements to show that the T/Y boundary may also correspond to the point at which the absolute H (1.6 um) and W2 (4.6 um) magnitudes plummet. We use these discoveries and their preliminary distances to place them in the larger context of the Solar Neighborhood. We present a table that updates the entire stellar and substellar constituency within 8 parsecs of the Sun, and we show that the current census has hydrogen-burning stars outnumbering brown dwarfs by roughly a factor of six. This factor will decrease with time as more brown dwarfs are identified within this volume, but unless there is a vast reservoir of cold brown dwarfs invisible to WISE, the final space density of brown dwarfs is still expected to fall well below that of stars. We also use these new Y dwarf discoveries, along with newly discovered T dwarfs from WISE, to investigate the field substellar mass function. We find that the overall space density of late-T and early-Y dwarfs matches that from simulations describing the mass function as a power law with slope -0.5 &lt; alpha &lt; 0.0; however, a power-law may provide a poor fit to the observed object counts as a function of spectral type because there are tantalizing hints that the number of brown dwarfs continues to rise from late-T to early-Y. More detailed monitoring and characterization of these Y dwarfs, along with dedicated searches aimed at identifying more examples, are certainly required.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/further-defining-spectral-type-y-and-exploring-the-low-mass-end-of-the-field-brown-dwarf-mass-function/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Stochastic Acceleration by Turbulence</title>
		<link>http://voxcharta.org/2012/05/10/stochastic-acceleration-by-turbulence/</link>
		<comments>http://voxcharta.org/2012/05/10/stochastic-acceleration-by-turbulence/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:44:25 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration mechanism]]></category>
		<category><![CDATA[astrophysical]]></category>
		<category><![CDATA[attractive feature]]></category>
		<category><![CDATA[electrons protons]]></category>
		<category><![CDATA[initial acceleration]]></category>
		<category><![CDATA[original model]]></category>
		<category><![CDATA[plasma particles]]></category>
		<category><![CDATA[plasma turbulence]]></category>
		<category><![CDATA[plasma wave]]></category>
		<category><![CDATA[radiation]]></category>
		<category><![CDATA[relative merits]]></category>
		<category><![CDATA[scenarios]]></category>
		<category><![CDATA[second stage]]></category>
		<category><![CDATA[shock]]></category>
		<category><![CDATA[signature]]></category>
		<category><![CDATA[solar energetic particle]]></category>
		<category><![CDATA[solar flare]]></category>
		<category><![CDATA[stochastic process]]></category>
		<category><![CDATA[thermal background]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/stochastic-acceleration-by-turbulence/</guid>
		<description><![CDATA[The subject of this paper is stochastic acceleration by plasma turbulence, a process akin to the original model proposed by Fermi. We review the relative merits of different acceleration models, in particular the so called first order Fermi acceleration by shocks and second order Fermi by stochastic processes, and point out that plasma waves or [...]]]></description>
			<content:encoded><![CDATA[<p>The subject of this paper is stochastic acceleration by plasma turbulence, a process akin to the original model proposed by Fermi. We review the relative merits of different acceleration models, in particular the so called first order Fermi acceleration by shocks and second order Fermi by stochastic processes, and point out that plasma waves or turbulence play an important role in all mechanisms of acceleration. Thus, stochastic acceleration by turbulence is active in most situations. We also show that it is the most efficient mechanism of acceleration of relatively cool non relativistic thermal background plasma particles. In addition, it can preferentially accelerate electrons relative to protons as is needed in many astrophysical radiating sources, where usually there are no indications of presence of shocks. We also point out that a hybrid acceleration mechanism consisting of initial acceleration by turbulence of background particles followed by a second stage acceleration by a shock has many attractive features. It is demonstrated that the above scenarios can account for many signatures of the accelerated electrons, protons and other ions, in particular $^3$He and $^4$He, seen directly as Solar Energetic Particles and through the radiation they produce in solar flares.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/stochastic-acceleration-by-turbulence/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Polar Field Reversal Observations with Hinode</title>
		<link>http://voxcharta.org/2012/05/10/polar-field-reversal-observations-with-hinode/</link>
		<comments>http://voxcharta.org/2012/05/10/polar-field-reversal-observations-with-hinode/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:43:00 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[hinode]]></category>
		<category><![CDATA[latitude]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetic flux density]]></category>
		<category><![CDATA[map]]></category>
		<category><![CDATA[number density]]></category>
		<category><![CDATA[optical telescope]]></category>
		<category><![CDATA[order of magnitude]]></category>
		<category><![CDATA[orders of magnitude]]></category>
		<category><![CDATA[patches]]></category>
		<category><![CDATA[polar field]]></category>
		<category><![CDATA[polar region]]></category>
		<category><![CDATA[polarity]]></category>
		<category><![CDATA[pore]]></category>
		<category><![CDATA[quiet sun]]></category>
		<category><![CDATA[solar cycle]]></category>
		<category><![CDATA[solar maximum]]></category>
		<category><![CDATA[temporal change]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/polar-field-reversal-observations-with-hinode/</guid>
		<description><![CDATA[We have been monitoring yearly variation in the Sun&#8217;s polar magnetic fields with the Solar Optical Telescope aboard {\it Hinode} to record their evolution and expected reversal near the solar maximum. All magnetic patches in the magnetic flux maps are automatically identified to obtain the number density and magnetic flux density as a function of [...]]]></description>
			<content:encoded><![CDATA[<p>We have been monitoring yearly variation in the Sun&#8217;s polar magnetic fields with the Solar Optical Telescope aboard {\it Hinode} to record their evolution and expected reversal near the solar maximum. All magnetic patches in the magnetic flux maps are automatically identified to obtain the number density and magnetic flux density as a function of th total magnetic flux per patch. The detected magnetic flux per patch ranges over four orders of magnitude ($10^{15}$ &#8212; $10^{20}$ Mx). The higher end of the magnetic flux in the polar regions is about one order of magnitude larger than that of the quiet Sun, and nearly that of pores. Almost all large patches ($ \geq 10^{18}$ Mx) have the same polarity, while smaller patches have a fair balance of both polarities. The polarity of the polar region as a whole is consequently determined only by the large magnetic concentrations. A clear decrease in the net flux of the polar region is detected in the slow rising phase of the current solar cycle. The decrease is more rapid in the north polar region than in the south. The decrease in the net flux is caused by a decrease in the number and size of the large flux concentrations as well as the appearance of patches with opposite polarity at lower latitudes. In contrast, we do not see temporal change in the magnetic flux associated with the smaller patches ($ &lt; 10^{18}$ Mx) and that of the horizontal magnetic fields during the years 2008&#8211;2012.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/polar-field-reversal-observations-with-hinode/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Stellar Polarimetry: Where Are We and Where Are We Going?</title>
		<link>http://voxcharta.org/2012/05/10/stellar-polarimetry-where-are-we-and-where-are-we-going/</link>
		<comments>http://voxcharta.org/2012/05/10/stellar-polarimetry-where-are-we-and-where-are-we-going/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:42:43 +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[breakout session]]></category>
		<category><![CDATA[community priorities]]></category>
		<category><![CDATA[conference participants]]></category>
		<category><![CDATA[instrumentation]]></category>
		<category><![CDATA[polarimetry]]></category>
		<category><![CDATA[vitality]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/stellar-polarimetry-where-are-we-and-where-are-we-going/</guid>
		<description><![CDATA[On the final day of the Stellar Polarimetry conference, participants split up into three &#8220;breakout sessions&#8221; to discuss the future of the field in the areas of instrumentation, upcoming opportunities, and community priorities. This contribution compiles the major recommendations arising from each breakout session. We hope that the polarimetric community will find these ideas useful [...]]]></description>
			<content:encoded><![CDATA[<p>On the final day of the Stellar Polarimetry conference, participants split up into three &#8220;breakout sessions&#8221; to discuss the future of the field in the areas of instrumentation, upcoming opportunities, and community priorities. This contribution compiles the major recommendations arising from each breakout session. We hope that the polarimetric community will find these ideas useful as we consider how to maintain the vitality of polarimetry in the coming years.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/stellar-polarimetry-where-are-we-and-where-are-we-going/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>On the origin of [Ne II] emission in young stars: mid-infrared and optical observations with the Very Large Telescope</title>
		<link>http://voxcharta.org/2012/05/10/on-the-origin-of-ne-ii-emission-in-young-stars-mid-infrared-and-optical-observations-with-the-very-large-telescope/</link>
		<comments>http://voxcharta.org/2012/05/10/on-the-origin-of-ne-ii-emission-in-young-stars-mid-infrared-and-optical-observations-with-the-very-large-telescope/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:41:50 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bipolar]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[dispersion]]></category>
		<category><![CDATA[forbidden lines]]></category>
		<category><![CDATA[herbig]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[line profile]]></category>
		<category><![CDATA[optical observation]]></category>
		<category><![CDATA[peak velocity]]></category>
		<category><![CDATA[resolution observations]]></category>
		<category><![CDATA[spectral resolution]]></category>
		<category><![CDATA[Spitzer]]></category>
		<category><![CDATA[three star]]></category>
		<category><![CDATA[two stars]]></category>
		<category><![CDATA[visir]]></category>
		<category><![CDATA[vlt]]></category>
		<category><![CDATA[wavelength]]></category>
		<category><![CDATA[young stars]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/on-the-origin-of-ne-ii-emission-in-young-stars-mid-infrared-and-optical-observations-with-the-very-large-telescope/</guid>
		<description><![CDATA[{Abridged version for ArXiv}. We provide direct constraints on the origin of the [Ne II] emission in 15 young stars using high-spatial and spectral resolution observations with VISIR at the VLT that allow us to study the kinematics of the emitting gas. In addition we compare the [Ne II] line with optical forbidden lines observed [...]]]></description>
			<content:encoded><![CDATA[<p>{Abridged version for ArXiv}. We provide direct constraints on the origin of the [Ne II] emission in 15 young stars using high-spatial and spectral resolution observations with VISIR at the VLT that allow us to study the kinematics of the emitting gas. In addition we compare the [Ne II] line with optical forbidden lines observed for three stars with UVES. The [Ne II] line was detected in 7 stars, among them the first confirmed detection of [Ne II] in a Herbig Be star, V892 Tau. In four cases, the large blueshifted lines indicate an origin in a jet. In two stars, the small shifts and asymmetric profiles indicate an origin in a photo-evaporative wind. CoKu Tau 1, seen close to edge-on, shows a spatially unresolved line centered at the stellar rest velocity, although cross-dispersion centroids move within 10 AU from one side of the star to the other as a function of wavelength. The line profile is symmetric with wings extending up to about +-80 km/s. The origin of the [Ne II] line could either be due to the bipolar jet or to the disk. For the stars with VLT-UVES observations, in several cases, the optical forbidden line profiles and shifts are very similar to the profile of the [Ne II] line, suggesting that the lines are emitted in the same region. A general trend observed with VISIR is a lower line flux when compared with the fluxes obtained with Spitzer. We found no correlation between the line full-width at half maximum and the line peak velocity. The [Ne II] line remains undetected in a large part of the sample, an indication that the emission detected with Spitzer in those stars is likely extended.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/on-the-origin-of-ne-ii-emission-in-young-stars-mid-infrared-and-optical-observations-with-the-very-large-telescope/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Integral-field spectroscopy of the young high-mass star IRAS13481-6124</title>
		<link>http://voxcharta.org/2012/05/10/integral-field-spectroscopy-of-the-young-high-mass-star-iras13481-6124/</link>
		<comments>http://voxcharta.org/2012/05/10/integral-field-spectroscopy-of-the-young-high-mass-star-iras13481-6124/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:41:36 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[axis]]></category>
		<category><![CDATA[continuum]]></category>
		<category><![CDATA[field spectroscopy]]></category>
		<category><![CDATA[gamma]]></category>
		<category><![CDATA[high mass]]></category>
		<category><![CDATA[innermost disk]]></category>
		<category><![CDATA[integral field]]></category>
		<category><![CDATA[k band]]></category>
		<category><![CDATA[mass star]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[outflow]]></category>
		<category><![CDATA[photo center]]></category>
		<category><![CDATA[position angle]]></category>
		<category><![CDATA[rigid rotation]]></category>
		<category><![CDATA[sinfoni]]></category>
		<category><![CDATA[surroundings]]></category>
		<category><![CDATA[velocity gradient]]></category>
		<category><![CDATA[vlt]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/integral-field-spectroscopy-of-the-young-high-mass-star-iras13481-6124/</guid>
		<description><![CDATA[We present results of AO-assisted K-band IFU spectroscopy of the massive young star IRAS13481-6124 performed with ESO&#8217;s VLT/SINFONI instrument. Our spectro-astrometric analysis of the Br{\gamma} line revealed a photo-center shift with respect to the adjacent continuum of \sim1 AU at a distance of 3.1 kpc. The position angle of this shift matches with that of [...]]]></description>
			<content:encoded><![CDATA[<p>We present results of AO-assisted K-band IFU spectroscopy of the massive young star IRAS13481-6124 performed with ESO&#8217;s VLT/SINFONI instrument. Our spectro-astrometric analysis of the Br{\gamma} line revealed a photo-center shift with respect to the adjacent continuum of \sim1 AU at a distance of 3.1 kpc. The position angle of this shift matches with that of the outflow which confirms that the massive star is indeed the driving source. Furthermore, a velocity gradient along the major disk axis was found which hints at the rotational sense of the ionized region, and thus of the disk as well. The gradient is not consistent with Keplerian motion but points to rigid rotation of the innermost disk. Notably, emission of H_2 is absent from source while both shocked and fluorescent H_2 emission are observed in its immediate surroundings.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/integral-field-spectroscopy-of-the-young-high-mass-star-iras13481-6124/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Broadband ESO/VISIR-Spitzer infrared spectroscopy of the obscured supergiant X-ray Binary IGR J16318-4848</title>
		<link>http://voxcharta.org/2012/05/10/broadband-esovisir-spitzer-infrared-spectroscopy-of-the-obscured-supergiant-x-ray-binary-igr-j16318-4848/</link>
		<comments>http://voxcharta.org/2012/05/10/broadband-esovisir-spitzer-infrared-spectroscopy-of-the-obscured-supergiant-x-ray-binary-igr-j16318-4848/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:40:21 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[binary system]]></category>
		<category><![CDATA[celestial source]]></category>
		<category><![CDATA[cold gas]]></category>
		<category><![CDATA[compact object]]></category>
		<category><![CDATA[dust component]]></category>
		<category><![CDATA[eso ntt]]></category>
		<category><![CDATA[fundamental question]]></category>
		<category><![CDATA[high mass]]></category>
		<category><![CDATA[infrared observation]]></category>
		<category><![CDATA[infrared spectroscopy]]></category>
		<category><![CDATA[mass x]]></category>
		<category><![CDATA[phenomenological model]]></category>
		<category><![CDATA[photometric]]></category>
		<category><![CDATA[ray binaries]]></category>
		<category><![CDATA[sofi]]></category>
		<category><![CDATA[spectral energy distribution]]></category>
		<category><![CDATA[spectroscopic observation]]></category>
		<category><![CDATA[spherical geometry]]></category>
		<category><![CDATA[supergiant]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/broadband-esovisir-spitzer-infrared-spectroscopy-of-the-obscured-supergiant-x-ray-binary-igr-j16318-4848/</guid>
		<description><![CDATA[A new class of X-ray binaries has been recently discovered by the high energy observatory, INTEGRAL. It is composed of intrinsically obscured supergiant high mass X-ray binaries, unveiled by means of multi-wavelength X-ray, optical, near- and mid-infrared observations, in particular photometric and spectroscopic observations using ESO facilities. However the fundamental questions about these intriguing sources, [...]]]></description>
			<content:encoded><![CDATA[<p>A new class of X-ray binaries has been recently discovered by the high energy observatory, INTEGRAL. It is composed of intrinsically obscured supergiant high mass X-ray binaries, unveiled by means of multi-wavelength X-ray, optical, near- and mid-infrared observations, in particular photometric and spectroscopic observations using ESO facilities. However the fundamental questions about these intriguing sources, namely their formation, evolution, and the nature of their environment, are still unsolved. Among them, IGR J16318-4848 &#8211; a compact object orbiting around a supergiant B[e] star &#8211; seems to be one of the most extraordinary celestial sources of our Galaxy. We present here new ESO/VLT VISIR mid-infrared (MIR) spectroscopic observations of this source. First, line diagnostics allow us to confirm the presence of absorbing material (dust and cold gas) enshrouding the whole binary system, and to characterise the nature of this material. Second, by fitting broadband near to mid-infrared Spectral Energy Distribution &#8211; including ESO NTT/SofI, VLT/VISIR and Spitzer data &#8211; with a phenomenological model for sgB[e] stars, we show that the star is surrounded by an irradiated rim heated to a temperature of 3800-5500 K, along with a viscous disk component at an inner temperature of 750 K. VISIR data allow us to exclude the spherical geometry for the dust component. This detailed study will allow us in the future to get better constraints on the formation and evolution of such rare and short-living high mass X-ray binary systems in our Galaxy.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/broadband-esovisir-spitzer-infrared-spectroscopy-of-the-obscured-supergiant-x-ray-binary-igr-j16318-4848/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Wavelet Analysis on Solar Wind Parameters and Geomagnetic Indices</title>
		<link>http://voxcharta.org/2012/05/10/wavelet-analysis-on-solar-wind-parameters-and-geomagnetic-indices/</link>
		<comments>http://voxcharta.org/2012/05/10/wavelet-analysis-on-solar-wind-parameters-and-geomagnetic-indices/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:40:06 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[beta]]></category>
		<category><![CDATA[earth]]></category>
		<category><![CDATA[geomagnetic indices]]></category>
		<category><![CDATA[heliosphere]]></category>
		<category><![CDATA[interplanetary magnetic field]]></category>
		<category><![CDATA[oscillator]]></category>
		<category><![CDATA[plasma density]]></category>
		<category><![CDATA[plasma pressure]]></category>
		<category><![CDATA[plasma temperature]]></category>
		<category><![CDATA[solar cycle]]></category>
		<category><![CDATA[solar plasma]]></category>
		<category><![CDATA[solar wind parameters]]></category>
		<category><![CDATA[solar wind speed]]></category>
		<category><![CDATA[Sun]]></category>
		<category><![CDATA[temperature plasma]]></category>
		<category><![CDATA[terrestrial magnetosphere]]></category>
		<category><![CDATA[wind exhibit]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/wavelet-analysis-on-solar-wind-parameters-and-geomagnetic-indices/</guid>
		<description><![CDATA[The sun as an oscillator produces frequencies which propagate in the heliosphere, via solar wind, to the terrestrial magnetosphere. We searched for those frequencies in the parameters of the near Earth solar plasma and the geomagnetic indices for the past four solar cycles. The solar wind parameters used in this work are the interplanetary magnetic [...]]]></description>
			<content:encoded><![CDATA[<p>The sun as an oscillator produces frequencies which propagate in the heliosphere, via solar wind, to the terrestrial magnetosphere. We searched for those frequencies in the parameters of the near Earth solar plasma and the geomagnetic indices for the past four solar cycles. The solar wind parameters used in this work are the interplanetary magnetic field, plasma beta, Alfven Mach number, solar wind speed, plasma temperature, plasma pressure, plasma density and the geomagnetic indices DST, AE, Ap and Kp. We found out that each parameter of the solar wind exhibit certain periodicities which di?erentiate in each cycle. Our results indicate intermittent periodicities in our data, some of them shared between the solar wind parameters and geomagnetic indices.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/wavelet-analysis-on-solar-wind-parameters-and-geomagnetic-indices/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Calcium Emission in Interacting Binary Be Stars</title>
		<link>http://voxcharta.org/2012/05/10/calcium-emission-in-interacting-binary-be-stars/</link>
		<comments>http://voxcharta.org/2012/05/10/calcium-emission-in-interacting-binary-be-stars/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:39:13 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[advent]]></category>
		<category><![CDATA[binaries]]></category>
		<category><![CDATA[calcium]]></category>
		<category><![CDATA[satellite]]></category>
		<category><![CDATA[signature]]></category>
		<category><![CDATA[spectrometer]]></category>
		<category><![CDATA[spectroscopic survey]]></category>
		<category><![CDATA[star disc]]></category>
		<category><![CDATA[triplet]]></category>
		<category><![CDATA[visible emission]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/calcium-emission-in-interacting-binary-be-stars/</guid>
		<description><![CDATA[Polidan (1976) suggested that Be stars showing the CaII IR triplet in emission are interacting binaries. With the advent of the Gaia satellite, which will host a spectrometer to observe stars in the range 8470&#8211;8750 \AA, we carried out a spectroscopic survey of 150 Be stars, including Be binaries. We show that the Ca II [...]]]></description>
			<content:encoded><![CDATA[<p>Polidan (1976) suggested that Be stars showing the CaII IR triplet in emission are interacting binaries. With the advent of the Gaia satellite, which will host a spectrometer to observe stars in the range 8470&#8211;8750 \AA, we carried out a spectroscopic survey of 150 Be stars, including Be binaries. We show that the Ca II triplet in emission, often connected with emission in Paschen lines, is an indicator of a peculiar environment in a Be star disc rather than a signature of an interacting binary Be star. However, Ca II emission without visible emission in Paschen lines is observed in interacting binary stars, as well as in peculiar objects. During the survey, a new interacting Be binary &#8211; HD 81357 &#8211; was discovered.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/calcium-emission-in-interacting-binary-be-stars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The AMBRE project: A new synthetic grid of high-resolution FGKM stellar spectra</title>
		<link>http://voxcharta.org/2012/05/10/the-ambre-project-a-new-synthetic-grid-of-high-resolution-fgkm-stellar-spectra/</link>
		<comments>http://voxcharta.org/2012/05/10/the-ambre-project-a-new-synthetic-grid-of-high-resolution-fgkm-stellar-spectra/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:38:54 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[atmospheric parameters]]></category>
		<category><![CDATA[chemical content]]></category>
		<category><![CDATA[dex]]></category>
		<category><![CDATA[grids]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[leq]]></category>
		<category><![CDATA[main goal]]></category>
		<category><![CDATA[model atmosphere]]></category>
		<category><![CDATA[new generation]]></category>
		<category><![CDATA[optical domain]]></category>
		<category><![CDATA[resolution spectra]]></category>
		<category><![CDATA[solar metallicity]]></category>
		<category><![CDATA[spectral resolution]]></category>
		<category><![CDATA[spectral type]]></category>
		<category><![CDATA[spectrograph]]></category>
		<category><![CDATA[stellar parameters]]></category>
		<category><![CDATA[stellar spectra]]></category>
		<category><![CDATA[synthetic spectra]]></category>
		<category><![CDATA[wavelength range]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/the-ambre-project-a-new-synthetic-grid-of-high-resolution-fgkm-stellar-spectra/</guid>
		<description><![CDATA[Large grids of synthetic spectra covering a widespread range of stellar parameters are mandatory for different stellar and (extra-)Galactic physics applications. Such large grids can be used for the automatic parametrisation of stellar spectra such as that performed within the AMBRE project for which the main goal is the stellar atmospheric parameters determination for the [...]]]></description>
			<content:encoded><![CDATA[<p>Large grids of synthetic spectra covering a widespread range of stellar parameters are mandatory for different stellar and (extra-)Galactic physics applications. Such large grids can be used for the automatic parametrisation of stellar spectra such as that performed within the AMBRE project for which the main goal is the stellar atmospheric parameters determination for the few hundreds of thousands of archived spectra of four ESO spectrographs. To fulfil the needs of AMBRE and future similar projects, we have computed a grid of synthetic spectra over the whole optical domain for cool to very cool stars of any luminosity with metallicities varying from 10-5 to 10 times the solar metallicity, and considering large variations in the chemical content of the {\alpha}-elements. New generation MARCS model atmospheres and the Turbospectrum code for radiative transfer have been used. We have also taken into account as complete as possible atomic and molecular linelists. A new grid of 16783 high resolution spectra over the wavelength range 3000 to 12000 {\AA} has been computed with a spectral resolution always larger than 150000. Normalised and absolute flux versions are available over a wide range of stellar atmospheric parameters for stars of FGKM spectral types. The covered parameters are 2500K\leqTeff\leq8000K, -0.5\leqlog(g)\leq5.5dex, -5.0\leq[M/H]\leq+1.0 dex and five different values of the enrichment in {\alpha}-elements have been considered (0.0, \pm0.2 dex and \pm0.4 dex around the standard values). This grid is made publicly available through the POLLUX database (about 50% of the spectra are already included in this database) and in FITS format upon request to the authors.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/the-ambre-project-a-new-synthetic-grid-of-high-resolution-fgkm-stellar-spectra/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Frequency of Hot Jupiters Orbiting Nearby Solar-Type Stars</title>
		<link>http://voxcharta.org/2012/05/10/the-frequency-of-hot-jupiters-orbiting-nearby-solar-type-stars/</link>
		<comments>http://voxcharta.org/2012/05/10/the-frequency-of-hot-jupiters-orbiting-nearby-solar-type-stars/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:38:34 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[gould]]></category>
		<category><![CDATA[harp]]></category>
		<category><![CDATA[hot jupiters]]></category>
		<category><![CDATA[keck]]></category>
		<category><![CDATA[kepler]]></category>
		<category><![CDATA[number statistics]]></category>
		<category><![CDATA[ogle]]></category>
		<category><![CDATA[radial velocity]]></category>
		<category><![CDATA[solar neighborhood]]></category>
		<category><![CDATA[solar type stars]]></category>
		<category><![CDATA[statistical significance]]></category>
		<category><![CDATA[velocity data]]></category>
		<category><![CDATA[velocity surveys]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/the-frequency-of-hot-jupiters-orbiting-nearby-solar-type-stars/</guid>
		<description><![CDATA[We determine the fraction of F, G, and K dwarfs in the Solar Neighborhood hosting hot jupiters as measured by the California Planet Survey from the Lick and Keck planet searches. We find the rate to be 1.2\pm0.38%, which is consistent with the rate reported by Mayor et al. (2011) from the HARPS and CORALIE [...]]]></description>
			<content:encoded><![CDATA[<p>We determine the fraction of F, G, and K dwarfs in the Solar Neighborhood hosting hot jupiters as measured by the California Planet Survey from the Lick and Keck planet searches. We find the rate to be 1.2\pm0.38%, which is consistent with the rate reported by Mayor et al. (2011) from the HARPS and CORALIE radial velocity surveys. These numbers are more than double the rate reported by Howard et al. (2011) for Kepler stars and the rate of Gould et al. (2006) from the OGLE-III transit search, however due to small number statistics these differences are of only marginal statistical significance. We explore some of the difficulties in estimating this rate from the existing radial velocity data sets and comparing radial velocity rates to rates from other techniques.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/the-frequency-of-hot-jupiters-orbiting-nearby-solar-type-stars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Interactions between brown-dwarf binaries and Sun-like stars</title>
		<link>http://voxcharta.org/2012/05/10/interactions-between-brown-dwarf-binaries-and-sun-like-stars/</link>
		<comments>http://voxcharta.org/2012/05/10/interactions-between-brown-dwarf-binaries-and-sun-like-stars/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:38:12 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[binary system]]></category>
		<category><![CDATA[brown dwarf]]></category>
		<category><![CDATA[conclusion]]></category>
		<category><![CDATA[consensus]]></category>
		<category><![CDATA[desert]]></category>
		<category><![CDATA[dissipation]]></category>
		<category><![CDATA[dwarf binaries]]></category>
		<category><![CDATA[favour]]></category>
		<category><![CDATA[fragmentation]]></category>
		<category><![CDATA[gravitational interaction]]></category>
		<category><![CDATA[hydrodynamic effects]]></category>
		<category><![CDATA[inference]]></category>
		<category><![CDATA[mechanisms]]></category>
		<category><![CDATA[numerical simulation]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[protostar]]></category>
		<category><![CDATA[selection effect]]></category>
		<category><![CDATA[statistic]]></category>
		<category><![CDATA[Sun]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/interactions-between-brown-dwarf-binaries-and-sun-like-stars/</guid>
		<description><![CDATA[Several mechanisms have been proposed for the formation of brown dwarfs, but there is as yet no consensus as to which &#8212; if any &#8212; are operative in nature. Any theory of brown dwarf formation must explain the observed statistics of brown dwarfs. These statistics are limited by selection effects, but they are becoming increasingly [...]]]></description>
			<content:encoded><![CDATA[<p>Several mechanisms have been proposed for the formation of brown dwarfs, but there is as yet no consensus as to which &#8212; if any &#8212; are operative in nature. Any theory of brown dwarf formation must explain the observed statistics of brown dwarfs. These statistics are limited by selection effects, but they are becoming increasingly discriminating. In particular, it appears (a) that brown dwarfs that are secondaries to Sun-like stars tend to be on wide orbits, $a\ga 100\,{\rm AU}$ (the Brown Dwarf Desert), and (b) that these brown dwarfs have a significantly higher chance of being in a close ($a\la 10\,{\rm AU}$) binary system with another brown dwarf than do brown dwarfs in the field. This then raises the issue of whether these brown dwarfs have formed {\it in situ}, i.e. by fragmentation of a circumstellar disc; or have formed elsewhere and subsequently been captured. We present numerical simulations of the purely gravitational interaction between a close brown-dwarf binary and a Sun-like star. These simulations demonstrate that such interactions have a negligible chance ($&lt;0.001$) of leading to the close brown-dwarf binary being captured by the Sun-like star. Making the interactions dissipative by invoking the hydrodynamic effects of attendant discs might alter this conclusion. However, in order to explain the above statistics, this dissipation would have to favour the capture of brown-dwarf binaries over single brown-dwarfs, and we present arguments why this is unlikely. The simplest inference is that most brown-dwarf binaries &#8212; and therefore possibly also most single brown dwarfs &#8212; form by fragmentation of circumstellar discs around Sun-like protostars, with some of them subsequently being ejected into the field.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/interactions-between-brown-dwarf-binaries-and-sun-like-stars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Tracers of Discs and Winds around Intermediate and High Mass Young Stellar Objects</title>
		<link>http://voxcharta.org/2012/05/10/tracers-of-discs-and-winds-around-intermediate-and-high-mass-young-stellar-objects/</link>
		<comments>http://voxcharta.org/2012/05/10/tracers-of-discs-and-winds-around-intermediate-and-high-mass-young-stellar-objects/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:37:37 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorption]]></category>
		<category><![CDATA[accretion disc]]></category>
		<category><![CDATA[circumstellar environment]]></category>
		<category><![CDATA[dense material]]></category>
		<category><![CDATA[disc model]]></category>
		<category><![CDATA[doppler]]></category>
		<category><![CDATA[electron]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[high speed]]></category>
		<category><![CDATA[inner regions]]></category>
		<category><![CDATA[mass range]]></category>
		<category><![CDATA[mass star]]></category>
		<category><![CDATA[outflow]]></category>
		<category><![CDATA[similarity]]></category>
		<category><![CDATA[speed motion]]></category>
		<category><![CDATA[stellar object]]></category>
		<category><![CDATA[stellar wind]]></category>
		<category><![CDATA[tracers]]></category>
		<category><![CDATA[transition]]></category>
		<category><![CDATA[wings]]></category>

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

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/chromospheric-jets-around-the-edges-of-sunspots/</guid>
		<description><![CDATA[Evidence is beginning to be put forward that demonstrates the role of the chromosphere in supplying energy and mass to the corona. We aim to asses the role of chromospheric jets in active region dynamics}{Using a combination of the {Hinode/SOT} Ca II H and TRACE 1550 {\AA} and 1600 {\AA} filters we examine chromospheric jets [...]]]></description>
			<content:encoded><![CDATA[<p>Evidence is beginning to be put forward that demonstrates the role of the chromosphere in supplying energy and mass to the corona. We aim to asses the role of chromospheric jets in active region dynamics}{Using a combination of the {Hinode/SOT} Ca II H and TRACE 1550 {\AA} and 1600 {\AA} filters we examine chromospheric jets situated at the edge of a sunspot.}{Analysis reveals a near continuous series of jets, that raise chromospheric material into the low corona above a sunspot. The jets have average rise speeds of 30 km\,s^{-1} and a range of 10-100km\,s^{-1}. Enhanced emission observed at the jets leading edge suggests the formation of a shock front. Increased emission in TRACE bandpasses above the sunspot and the disappearance of the jets from the Ca II filter suggests that some of the chromospheric jet material is at least heated to \sim0.1MK. The evidence suggests that the jets could be a mechanism which provides a steady, low-level heating for active region features.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/chromospheric-jets-around-the-edges-of-sunspots/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Subsurface Flows in and Around Active Regions with Rotating and Non-rotating Sunspots</title>
		<link>http://voxcharta.org/2012/05/10/subsurface-flows-in-and-around-active-regions-with-rotating-and-non-rotating-sunspots/</link>
		<comments>http://voxcharta.org/2012/05/10/subsurface-flows-in-and-around-active-regions-with-rotating-and-non-rotating-sunspots/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:35:34 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[carrington rotation]]></category>
		<category><![CDATA[depth profile]]></category>
		<category><![CDATA[flow component]]></category>
		<category><![CDATA[horizontal velocity]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[meridional flow]]></category>
		<category><![CDATA[neighborhood]]></category>
		<category><![CDATA[plasma]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[significant influence]]></category>
		<category><![CDATA[solar disk]]></category>
		<category><![CDATA[subsurface flow]]></category>
		<category><![CDATA[sunspot]]></category>
		<category><![CDATA[systematic effects]]></category>
		<category><![CDATA[temporal variation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/subsurface-flows-in-and-around-active-regions-with-rotating-and-non-rotating-sunspots/</guid>
		<description><![CDATA[The temporal variation of the horizontal velocity in subsurface layers beneath three different types of active regions is studied using the technique of ring diagrams. In this study, we select active regions (ARs) 10923, 10930, 10935 from three consecutive Carrington rotations: AR 10930 contains a fast-rotating sunspot in a strong emerging active region while other [...]]]></description>
			<content:encoded><![CDATA[<p>The temporal variation of the horizontal velocity in subsurface layers beneath three different types of active regions is studied using the technique of ring diagrams. In this study, we select active regions (ARs) 10923, 10930, 10935 from three consecutive Carrington rotations: AR 10930 contains a fast-rotating sunspot in a strong emerging active region while other two have non-rotating sunspots with emerging flux in AR 10923 and decaying flux in AR 10935. The depth range covered is from the surface to about 12 Mm. In order to minimize the influence of systematic effects, the selection of active and quiet regions is made so that these were observed at the same heliographic locations on the solar disk. We find a significant variation in both components of the horizontal velocity in active regions as compared to quiet regions. The magnitude is higher in emerging-flux regions than in the decaying-flux region, in agreement with earlier findings. Further, we clearly see a significant temporal variation in depth profiles of both zonal and meridional flow components in AR 10930, with the variation in the zonal component being more pronounced. We also notice a significant influence of the plasma motion in areas closest to the rotating sunspot in AR 10930 while areas surrounding the non-rotating sunspots in all three cases are least affected by the presence of the active region in their neighborhood.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/subsurface-flows-in-and-around-active-regions-with-rotating-and-non-rotating-sunspots/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Oscillation mode frequencies of 61 main sequence and subgiant stars observed by Kepler [Replacement]</title>
		<link>http://voxcharta.org/2012/05/10/oscillation-mode-frequencies-of-61-main-sequence-and-subgiant-stars-observed-by-kepler-replacement-2/</link>
		<comments>http://voxcharta.org/2012/05/10/oscillation-mode-frequencies-of-61-main-sequence-and-subgiant-stars-observed-by-kepler-replacement-2/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:32:25 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[corot]]></category>
		<category><![CDATA[echelle]]></category>
		<category><![CDATA[kepler]]></category>
		<category><![CDATA[likelihood ratio test]]></category>
		<category><![CDATA[main sequence]]></category>
		<category><![CDATA[maximum likelihood estimator]]></category>
		<category><![CDATA[methodology]]></category>
		<category><![CDATA[mode frequency]]></category>
		<category><![CDATA[modes]]></category>
		<category><![CDATA[nine months]]></category>
		<category><![CDATA[oscillation]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[power spectra]]></category>
		<category><![CDATA[probability]]></category>
		<category><![CDATA[scientist]]></category>
		<category><![CDATA[series of nine]]></category>
		<category><![CDATA[sigma]]></category>
		<category><![CDATA[solar type stars]]></category>
		<category><![CDATA[time series]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/oscillation-mode-frequencies-of-61-main-sequence-and-subgiant-stars-observed-by-kepler-replacement-2/</guid>
		<description><![CDATA[Solar-like oscillations have been observed by Kepler and CoRoT in several solar-type stars, thereby providing a way to probe the stars using asteroseismology.   We provide the mode frequencies of the oscillations of various stars required to perform a comparison with those obtained from stellar modelling.   We used a time series of [...]]]></description>
			<content:encoded><![CDATA[<p>Solar-like oscillations have been observed by Kepler and CoRoT in several solar-type stars, thereby providing a way to probe the stars using asteroseismology.   We provide the mode frequencies of the oscillations of various stars required to perform a comparison with those obtained from stellar modelling.   We used a time series of nine months of data for each star. The 61 stars observed were categorised in three groups: simple, F-like and mixed-mode. The simple group includes stars for which the identification of the mode degree is obvious. The F-like group includes stars for which the identification of the degree is ambiguous. The mixed-mode group includes evolved stars for which the modes do not follow the asymptotic relation of low-degree frequencies. Following this categorisation, the power spectra of the 61 main sequence and subgiant stars were analysed using both maximum likelihood estimators and Bayesian estimators, providing individual mode characteristics such as frequencies, linewidths, and mode heights. We developed and describe a methodology for extracting a single set of mode frequencies from multiple sets derived by different methods and individual scientists. We report on how one can assess the quality of the fitted parameters using the likelihood ratio test and the posterior probabilities.   We provide the mode frequencies of 61 stars (with their 1-sigma error bars), as well as their associated echelle diagrams.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/oscillation-mode-frequencies-of-61-main-sequence-and-subgiant-stars-observed-by-kepler-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Improved Variable Star Search in Large Photometric Data Sets &#8212; New Variables in CoRoT Field LRa02 Detected by BEST II [Replacement]</title>
		<link>http://voxcharta.org/2012/05/10/improved-variable-star-search-in-large-photometric-data-sets-new-variables-in-corot-field-lra02-detected-by-best-ii-replacement/</link>
		<comments>http://voxcharta.org/2012/05/10/improved-variable-star-search-in-large-photometric-data-sets-new-variables-in-corot-field-lra02-detected-by-best-ii-replacement/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:31:15 +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[analysis of variance]]></category>
		<category><![CDATA[berlin]]></category>
		<category><![CDATA[empirical approach]]></category>
		<category><![CDATA[ephemerides]]></category>
		<category><![CDATA[exoplanet]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[periodic variables]]></category>
		<category><![CDATA[photometric data]]></category>
		<category><![CDATA[reanalysis]]></category>
		<category><![CDATA[search procedure]]></category>
		<category><![CDATA[selection process]]></category>
		<category><![CDATA[star search]]></category>
		<category><![CDATA[statistic]]></category>
		<category><![CDATA[stellar variability]]></category>
		<category><![CDATA[supplementary catalog]]></category>
		<category><![CDATA[Telescope]]></category>
		<category><![CDATA[variable star]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/improved-variable-star-search-in-large-photometric-data-sets-new-variables-in-corot-field-lra02-detected-by-best-ii-replacement/</guid>
		<description><![CDATA[The CoRoT field LRa02 has been observed with the Berlin Exoplanet Search Telescope II (BEST II) during the southern summer 2007/2008. A first analysis of stellar variability led to the publication of 345 newly discovered variable stars. Now, a deeper analysis of this data set was used to optimize the variability search procedure. Several methods [...]]]></description>
			<content:encoded><![CDATA[<p>The CoRoT field LRa02 has been observed with the Berlin Exoplanet Search Telescope II (BEST II) during the southern summer 2007/2008. A first analysis of stellar variability led to the publication of 345 newly discovered variable stars. Now, a deeper analysis of this data set was used to optimize the variability search procedure. Several methods and parameters have been tested in order to improve the selection process compared to the widely used J index for variability ranking. This paper describes an empirical approach to treat systematic trends in photometric data based upon the analysis of variance statistics that can significantly decrease the rate of false detections.   Finally, the process of reanalysis and method improvement has virtually doubled the number of variable stars compared to the first analysis by Kabath et al. A supplementary catalog of 272 previously unknown periodic variables plus 52 stars with suspected variability is presented. Improved ephemerides are given for 19 known variables in the field. In addition, the BEST II results are compared with CoRoT data and its automatic variability classification.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/improved-variable-star-search-in-large-photometric-data-sets-new-variables-in-corot-field-lra02-detected-by-best-ii-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Constraining Tidal Dissipation in Stars from The Destruction Rates of Exoplanets</title>
		<link>http://voxcharta.org/2012/05/09/constraining-tidal-dissipation-in-stars-from-the-destruction-rates-of-exoplanets/</link>
		<comments>http://voxcharta.org/2012/05/09/constraining-tidal-dissipation-in-stars-from-the-destruction-rates-of-exoplanets/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:47:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[circular orbit]]></category>
		<category><![CDATA[efficiency]]></category>
		<category><![CDATA[exoplanet]]></category>
		<category><![CDATA[extrasolar planet]]></category>
		<category><![CDATA[parent star]]></category>
		<category><![CDATA[population]]></category>
		<category><![CDATA[quality factor]]></category>
		<category><![CDATA[tidal dissipation]]></category>
		<category><![CDATA[tide]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/constraining-tidal-dissipation-in-stars-from-the-destruction-rates-of-exoplanets/</guid>
		<description><![CDATA[We use the distribution of extrasolar planets in circular orbits around stars with surface convective zones detected by ground based transit searches to constrain how efficiently tides raised by the planet are dissipated on the parent star. We parameterize this efficiency as a tidal quality factor (Q*). We conclude that the population of currently known [...]]]></description>
			<content:encoded><![CDATA[<p>We use the distribution of extrasolar planets in circular orbits around stars with surface convective zones detected by ground based transit searches to constrain how efficiently tides raised by the planet are dissipated on the parent star. We parameterize this efficiency as a tidal quality factor (Q*). We conclude that the population of currently known planets is inconsistent with Q*&lt;10^7 at the 99% level. Previous studies show that values of Q* between 10^5 and 10^7 are required in order to explain the orbital circularization of main sequence low mass binary stars in clusters, suggesting that different dissipation mechanisms might be acting in the two cases, most likely due to the very different tidal forcing frequencies relative to the stellar rotation frequency occurring for star&#8211;star versus planet&#8211;star systems.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/constraining-tidal-dissipation-in-stars-from-the-destruction-rates-of-exoplanets/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Scaling of the growth rate of magnetic islands in the heliosheath</title>
		<link>http://voxcharta.org/2012/05/09/scaling-of-the-growth-rate-of-magnetic-islands-in-the-heliosheath/</link>
		<comments>http://voxcharta.org/2012/05/09/scaling-of-the-growth-rate-of-magnetic-islands-in-the-heliosheath/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:45:59 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[aspect ratio]]></category>
		<category><![CDATA[current sheet]]></category>
		<category><![CDATA[heliosheath]]></category>
		<category><![CDATA[high aspect ratio]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetic island]]></category>
		<category><![CDATA[magnetic reconnection]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[tension]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/scaling-of-the-growth-rate-of-magnetic-islands-in-the-heliosheath/</guid>
		<description><![CDATA[Current sheets thinner than the ion inertial length are unstable to the tearing instability and will develop magnetic islands that grow due to magnetic reconnection. We investigate whether the growth of magnetic islands in a current sheet can continue indefinitely, or in the case of the heliosheath until reaching a neighboring current sheet, and at [...]]]></description>
			<content:encoded><![CDATA[<p>Current sheets thinner than the ion inertial length are unstable to the tearing instability and will develop magnetic islands that grow due to magnetic reconnection. We investigate whether the growth of magnetic islands in a current sheet can continue indefinitely, or in the case of the heliosheath until reaching a neighboring current sheet, and at what rate the islands grow. We investigate the development and growth of magnetic islands using a particle-in-cell code, starting from particle noise. Performing a scaling of the growth of magnetic islands versus the system size, we find that the growth rate is independent of the system size up to the largest simulation we were able to complete. The islands are able to continue growing as long as they merge with each other and maintain a high aspect ratio. Otherwise there is not enough magnetic tension to sustain reconnection. When applied to the sectored magnetic fields in the heliosheath, we show that the islands can continue growing until they reach the sector width and do so in much less time than it takes for the islands to convect through the heliosheath.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/scaling-of-the-growth-rate-of-magnetic-islands-in-the-heliosheath/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Stream Overflow in Z Cha and OY Car during Quiescence</title>
		<link>http://voxcharta.org/2012/05/09/stream-overflow-in-z-cha-and-oy-car-during-quiescence/</link>
		<comments>http://voxcharta.org/2012/05/09/stream-overflow-in-z-cha-and-oy-car-during-quiescence/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:41:56 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[distance]]></category>
		<category><![CDATA[eclipse]]></category>
		<category><![CDATA[hot spot]]></category>
		<category><![CDATA[ingress and egress]]></category>
		<category><![CDATA[outburst]]></category>
		<category><![CDATA[overflow]]></category>
		<category><![CDATA[quiescence]]></category>
		<category><![CDATA[radius]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/stream-overflow-in-z-cha-and-oy-car-during-quiescence/</guid>
		<description><![CDATA[Eclipses of the hot spot in Z Cha and OY Car observed by many authors during their quiescence are re-analyzed. Distances of the spot from the center of the disk r_s are determined from phases of ingress and egress. In the case of several eclipses of Z Cha and nearly all eclipses of OY Car [...]]]></description>
			<content:encoded><![CDATA[<p>Eclipses of the hot spot in Z Cha and OY Car observed by many authors during their quiescence are re-analyzed. Distances of the spot from the center of the disk r_s are determined from phases of ingress and egress. In the case of several eclipses of Z Cha and nearly all eclipses of OY Car it is found that r_s(egress) &lt; r_s(ingress). This implies that they are not representative for the radius of the disk r_d and is interpreted as being due to the stream overflow. The r_s(ingress) &#8211; dt relations (where dt is the time since last outburst) are improved when points affected by the stream overflow are omitted.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/stream-overflow-in-z-cha-and-oy-car-during-quiescence/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Improved Variable Star Search in Large Photometric Data Sets &#8212; New Variables in CoRoT Field LRa02 Detected ba BEST II</title>
		<link>http://voxcharta.org/2012/05/09/improved-variable-star-search-in-large-photometric-data-sets-new-variables-in-corot-field-lra02-detected-ba-best-ii/</link>
		<comments>http://voxcharta.org/2012/05/09/improved-variable-star-search-in-large-photometric-data-sets-new-variables-in-corot-field-lra02-detected-ba-best-ii/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:41:19 +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[analysis of variance]]></category>
		<category><![CDATA[berlin]]></category>
		<category><![CDATA[empirical approach]]></category>
		<category><![CDATA[ephemerides]]></category>
		<category><![CDATA[exoplanet]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[periodic variables]]></category>
		<category><![CDATA[photometric data]]></category>
		<category><![CDATA[reanalysis]]></category>
		<category><![CDATA[search procedure]]></category>
		<category><![CDATA[selection process]]></category>
		<category><![CDATA[star search]]></category>
		<category><![CDATA[statistic]]></category>
		<category><![CDATA[stellar variability]]></category>
		<category><![CDATA[supplementary catalog]]></category>
		<category><![CDATA[Telescope]]></category>
		<category><![CDATA[variable star]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/improved-variable-star-search-in-large-photometric-data-sets-new-variables-in-corot-field-lra02-detected-ba-best-ii/</guid>
		<description><![CDATA[The CoRoT field LRa02 has been observed with the Berlin Exoplanet Search Telescope II (BEST II) during the southern summer 2007/2008. A first analysis of stellar variability led to the publication of 345 newly discovered variable stars. Now, a deeper analysis of this data set was used to optimize the variability search procedure. Several methods [...]]]></description>
			<content:encoded><![CDATA[<p>The CoRoT field LRa02 has been observed with the Berlin Exoplanet Search Telescope II (BEST II) during the southern summer 2007/2008. A first analysis of stellar variability led to the publication of 345 newly discovered variable stars. Now, a deeper analysis of this data set was used to optimize the variability search procedure. Several methods and parameters have been tested in order to improve the selection process compared to the widely used J index for variability ranking. This paper describes an empirical approach to treat systematic trends in photometric data based upon the analysis of variance statistics that can significantly decrease the rate of false detections.   Finally, the process of reanalysis and method improvement has virtually doubled the number of variable stars compared to the first analysis by Kabath et al. A supplementary catalog of 272 previously unknown periodic variables plus 52 stars with suspected variability is presented. Improved ephemerides are given for 19 known variables in the field. In addition, the BEST II results are compared with CoRoT data and its automatic variability classification.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/improved-variable-star-search-in-large-photometric-data-sets-new-variables-in-corot-field-lra02-detected-ba-best-ii/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Great Eruption of Eta Carinae</title>
		<link>http://voxcharta.org/2012/05/09/the-great-eruption-of-eta-carinae/</link>
		<comments>http://voxcharta.org/2012/05/09/the-great-eruption-of-eta-carinae/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:40:09 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[contradiction]]></category>
		<category><![CDATA[impostor]]></category>
		<category><![CDATA[light echo]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[outflow]]></category>
		<category><![CDATA[physical mechanism]]></category>
		<category><![CDATA[physics]]></category>
		<category><![CDATA[prototype]]></category>
		<category><![CDATA[spectrum]]></category>
		<category><![CDATA[star eta carinae]]></category>
		<category><![CDATA[supernova explosion]]></category>
		<category><![CDATA[theoretical expectations]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/the-great-eruption-of-eta-carinae/</guid>
		<description><![CDATA[During the years 1838-1858, the very massive star {\eta} Carinae became the prototype supernova impostor: it released nearly as much light as a supernova explosion and shed an impressive amount of mass, but survived as a star.1 Based on a light-echo spectrum of that event, Rest et al.2 conclude that &#8220;a new physical mechanism&#8221; is [...]]]></description>
			<content:encoded><![CDATA[<p>During the years 1838-1858, the very massive star {\eta} Carinae became the prototype supernova impostor: it released nearly as much light as a supernova explosion and shed an impressive amount of mass, but survived as a star.1 Based on a light-echo spectrum of that event, Rest et al.2 conclude that &#8220;a new physical mechanism&#8221; is required to explain it, because the gas outflow appears cooler than theoretical expectations. Here we note that (1) theory predicted a substantially lower temperature than they quoted, and (2) their inferred observational value is quite uncertain. Therefore, analyses so far do not reveal any significant contradiction between the observed spectrum and most previous discussions of the Great Eruption and its physics.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/the-great-eruption-of-eta-carinae/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Really focused stellar winds in X-ray binaries</title>
		<link>http://voxcharta.org/2012/05/09/really-focused-stellar-winds-in-x-ray-binaries/</link>
		<comments>http://voxcharta.org/2012/05/09/really-focused-stellar-winds-in-x-ray-binaries/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:39:41 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[anisotropy]]></category>
		<category><![CDATA[approximation]]></category>
		<category><![CDATA[compact companion]]></category>
		<category><![CDATA[continuum]]></category>
		<category><![CDATA[coriolis force]]></category>
		<category><![CDATA[gravitational field]]></category>
		<category><![CDATA[high mass]]></category>
		<category><![CDATA[mass loss]]></category>
		<category><![CDATA[mass x]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[radiation]]></category>
		<category><![CDATA[roche]]></category>
		<category><![CDATA[spectral line]]></category>
		<category><![CDATA[stellar wind]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/really-focused-stellar-winds-in-x-ray-binaries/</guid>
		<description><![CDATA[We investigate the anisotropy of stellar winds in binaries to improve the models of accretion in high-mass X-ray binaries. We model numerically the stellar wind from a supergiant component of a binary in radial and three-dimensional radiation hydrodynamic approximation taking into account the Roche potential, Coriolis force, and radiative pressure in the continuum and spectral [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate the anisotropy of stellar winds in binaries to improve the models of accretion in high-mass X-ray binaries. We model numerically the stellar wind from a supergiant component of a binary in radial and three-dimensional radiation hydrodynamic approximation taking into account the Roche potential, Coriolis force, and radiative pressure in the continuum and spectral lines. The Coriolis force influences substantially the mass loss and thus also the accretion rate. The focusing of the stellar wind by the gravitational field of the compact companion leads to the formation of a gaseous tail behind the companion.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/really-focused-stellar-winds-in-x-ray-binaries/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Short Gas Dissipation Timescales: Diskless Stars in Taurus and Chamaeleon I</title>
		<link>http://voxcharta.org/2012/05/09/short-gas-dissipation-timescales-diskless-stars-in-taurus-and-chamaeleon-i/</link>
		<comments>http://voxcharta.org/2012/05/09/short-gas-dissipation-timescales-diskless-stars-in-taurus-and-chamaeleon-i/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:39:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[advanced camera]]></category>
		<category><![CDATA[angular momentum]]></category>
		<category><![CDATA[blind channel]]></category>
		<category><![CDATA[cloud core]]></category>
		<category><![CDATA[disk mass]]></category>
		<category><![CDATA[evolution planet]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[fuv]]></category>
		<category><![CDATA[initial condition]]></category>
		<category><![CDATA[mechanisms]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[myr]]></category>
		<category><![CDATA[nearby star]]></category>
		<category><![CDATA[planet formation]]></category>
		<category><![CDATA[radiation field]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[survey]]></category>
		<category><![CDATA[taurus]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/short-gas-dissipation-timescales-diskless-stars-in-taurus-and-chamaeleon-i/</guid>
		<description><![CDATA[We present an Advanced Camera for Surveys/ Solar Blind Channel far-ultraviolet (FUV) study of \h2 gas in 12 weak T Tauri stars in nearby star-forming regions. The sample consists of sources which have no evidence of inner disk dust. Our new FUV spectra show that in addition to the dust, the gas is depleted from [...]]]></description>
			<content:encoded><![CDATA[<p>We present an Advanced Camera for Surveys/ Solar Blind Channel far-ultraviolet (FUV) study of \h2 gas in 12 weak T Tauri stars in nearby star-forming regions. The sample consists of sources which have no evidence of inner disk dust. Our new FUV spectra show that in addition to the dust, the gas is depleted from the inner disk. This sample is combined with a larger FUV sample of accretors and non-accretors with ages between 1 and 100 Myr, showing that as early as 1&#8211;3 Myr, systems both with and without gas are found. Possible mechanisms for depleting gas quickly include viscous evolution, planet formation and photoevaporation by stellar radiation fields. Since these mechanisms alone cannot account for the lack of gas at 1&#8211;3 Myr, it is likely that the initial conditions (e.g. initial disk mass or core angular momentum) contribute to the variety of disks observed at any age. We estimate the angular momentum of a cloud needed for most of the mass to fall very close to the central object and compare this to models of the expected distribution of angular momenta. Up to 20% of cloud cores have low enough angular momenta to form disks with the mass close to the star, which would then accrete quickly; this percentage is similar to the fraction of diskless stars in the youngest star forming regions. With our sample, we characterize the chromospheric contribution to the FUV luminosity and find that $L_{FUV}/L_{bol}$ saturates at $\sim10^{-4.1}$.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/short-gas-dissipation-timescales-diskless-stars-in-taurus-and-chamaeleon-i/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Magnetic Fields in Astrophysical Jets: From Launch to Termination</title>
		<link>http://voxcharta.org/2012/05/09/magnetic-fields-in-astrophysical-jets-from-launch-to-termination/</link>
		<comments>http://voxcharta.org/2012/05/09/magnetic-fields-in-astrophysical-jets-from-launch-to-termination/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:38:31 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion disc]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[AGN]]></category>
		<category><![CDATA[astrophysical jets]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[galactic compact objects]]></category>
		<category><![CDATA[launch]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[mechanical energy]]></category>
		<category><![CDATA[molecular cloud]]></category>
		<category><![CDATA[momentum]]></category>
		<category><![CDATA[numerical simulation]]></category>
		<category><![CDATA[observational constraints]]></category>
		<category><![CDATA[protostar]]></category>
		<category><![CDATA[radiation processes]]></category>
		<category><![CDATA[relativistic jet]]></category>
		<category><![CDATA[scales]]></category>
		<category><![CDATA[similarities and differences]]></category>
		<category><![CDATA[young stars]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/magnetic-fields-in-astrophysical-jets-from-launch-to-termination/</guid>
		<description><![CDATA[Long-lived, stable jets are observed in a wide variety of systems, from protostars, through Galactic compact objects to active galactic nuclei (AGN). Magnetic fields play a central role in launching, accelerating, and collimating the jets through various media. The termination of jets in molecular clouds or the interstellar medium deposits enormous amounts of mechanical energy [...]]]></description>
			<content:encoded><![CDATA[<p>Long-lived, stable jets are observed in a wide variety of systems, from protostars, through Galactic compact objects to active galactic nuclei (AGN). Magnetic fields play a central role in launching, accelerating, and collimating the jets through various media. The termination of jets in molecular clouds or the interstellar medium deposits enormous amounts of mechanical energy and momentum, and their interactions with the external medium, as well, in many cases, as the radiation processes by which they are observed, are intimately connected with the magnetic fields they carry. This review focuses on the properties and structures of magnetic fields in long-lived jets, from their launch from rotating magnetized young stars, black holes, and their accretion discs, to termination and beyond. We compare the results of theory, numerical simulations, and observations of these diverse systems and address similarities and differences between relativistic and non-relativistic jets in protostellar versus AGN systems. On the observational side, we focus primarily on jets driven by AGN because of the strong observational constraints on their magnetic field properties, and we discuss the links between the physics of these jets on all scales.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/magnetic-fields-in-astrophysical-jets-from-launch-to-termination/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The effects of plasma beta and anisotropy instabilities on the dynamics of reconnecting magnetic fields in the heliosheath [Replacement]</title>
		<link>http://voxcharta.org/2012/05/09/the-effects-of-plasma-beta-and-anisotropy-instabilities-on-the-dynamics-of-reconnecting-magnetic-fields-in-the-heliosheath-replacement/</link>
		<comments>http://voxcharta.org/2012/05/09/the-effects-of-plasma-beta-and-anisotropy-instabilities-on-the-dynamics-of-reconnecting-magnetic-fields-in-the-heliosheath-replacement/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:36:32 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[anisotropy]]></category>
		<category><![CDATA[beta]]></category>
		<category><![CDATA[contraction]]></category>
		<category><![CDATA[core]]></category>
		<category><![CDATA[finite size]]></category>
		<category><![CDATA[firehose]]></category>
		<category><![CDATA[heliosheath]]></category>
		<category><![CDATA[instabilities]]></category>
		<category><![CDATA[magnetic energy]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetic island]]></category>
		<category><![CDATA[magnetic pressure]]></category>
		<category><![CDATA[magnetic reconnection]]></category>
		<category><![CDATA[mechanisms]]></category>
		<category><![CDATA[plasma pressure]]></category>
		<category><![CDATA[saturation]]></category>
		<category><![CDATA[stress]]></category>
		<category><![CDATA[weibel]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/the-effects-of-plasma-beta-and-anisotropy-instabilities-on-the-dynamics-of-reconnecting-magnetic-fields-in-the-heliosheath-replacement/</guid>
		<description><![CDATA[The plasma {\beta} (the ratio of the plasma pressure to the magnetic pressure) of a system can have a large effect on its dynamics as high {\beta} enhances the effects of pressure anisotropies. We investigate the effects of {\beta} in a system of stacked current sheets that break up into magnetic islands due to magnetic [...]]]></description>
			<content:encoded><![CDATA[<p>The plasma {\beta} (the ratio of the plasma pressure to the magnetic pressure) of a system can have a large effect on its dynamics as high {\beta} enhances the effects of pressure anisotropies. We investigate the effects of {\beta} in a system of stacked current sheets that break up into magnetic islands due to magnetic reconnection. We find significant differences between {\beta}  1. At low {\beta} growing magnetic islands are modestly elongated and become round as contraction releases magnetic stress and reduces magnetic energy. At high {\beta} the increase of the parallel pressure in contracting islands causes saturation of modestly elongated islands as island cores approach the marginal firehose condition. Only highly elongated islands reach finite size. The kinking associated with the Weibel and firehose instabilities prevents full contraction of these islands, leading to a final state of highly elongated islands in which further reconnection is suppressed. The results are directly relevant to reconnection in the sectored region of the heliosheath and possibly to saturation mechanisms of the magnetorotational instability in accretion flows.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/the-effects-of-plasma-beta-and-anisotropy-instabilities-on-the-dynamics-of-reconnecting-magnetic-fields-in-the-heliosheath-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Oscillation mode frequencies of 61 main sequence and subgiant stars observed by Kepler [Replacement]</title>
		<link>http://voxcharta.org/2012/05/09/oscillation-mode-frequencies-of-61-main-sequence-and-subgiant-stars-observed-by-kepler-replacement/</link>
		<comments>http://voxcharta.org/2012/05/09/oscillation-mode-frequencies-of-61-main-sequence-and-subgiant-stars-observed-by-kepler-replacement/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:32:11 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[corot]]></category>
		<category><![CDATA[echelle]]></category>
		<category><![CDATA[kepler]]></category>
		<category><![CDATA[likelihood ratio test]]></category>
		<category><![CDATA[main sequence]]></category>
		<category><![CDATA[maximum likelihood estimator]]></category>
		<category><![CDATA[methodology]]></category>
		<category><![CDATA[mode frequency]]></category>
		<category><![CDATA[modes]]></category>
		<category><![CDATA[nine months]]></category>
		<category><![CDATA[oscillation]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[power spectra]]></category>
		<category><![CDATA[probability]]></category>
		<category><![CDATA[scientist]]></category>
		<category><![CDATA[series of nine]]></category>
		<category><![CDATA[sigma]]></category>
		<category><![CDATA[solar type stars]]></category>
		<category><![CDATA[time series]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/oscillation-mode-frequencies-of-61-main-sequence-and-subgiant-stars-observed-by-kepler-replacement/</guid>
		<description><![CDATA[Solar-like oscillations have been observed by Kepler and CoRoT in several solar-type stars, thereby providing a way to probe the stars using asteroseismology   We provide the mode frequencies of the oscillations of various stars required to perform a comparison with those obtained from stellar modelling.   We used a time series of [...]]]></description>
			<content:encoded><![CDATA[<p>Solar-like oscillations have been observed by Kepler and CoRoT in several solar-type stars, thereby providing a way to probe the stars using asteroseismology   We provide the mode frequencies of the oscillations of various stars required to perform a comparison with those obtained from stellar modelling.   We used a time series of nine months of data for each star. The 61 stars observed were categorised in three groups: simple, F-like and mixed-mode. The simple group includes stars for which the identification of the mode degree is obvious. The F-like group includes stars for which the identification of the degree is ambiguous. The mixed-mode group includes evolved stars for which the modes do not follow the asymptotic relation of low-degree frequencies. Following this categorisation, the power spectra of the 61 main sequence and subgiant stars were analysed using both maximum likelihood estimators and Bayesian estimators, providing individual mode characteristics such as frequencies, linewidths, and mode heights. We developed and describe a methodology for extracting a single set of mode frequencies from multiple sets derived by different methods and individual scientists. We report on how one can assess the quality of the fitted parameters using the likelihood ratio test and the posterior probabilities.   We provide the mode frequencies of 61 stars (with their 1-sigma error bars), as well as their associated echelle diagrams.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/oscillation-mode-frequencies-of-61-main-sequence-and-subgiant-stars-observed-by-kepler-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Properties of Umbral Dots from Stray Light Corrected Hinode Filtergrams [Replacement]</title>
		<link>http://voxcharta.org/2012/05/09/properties-of-umbral-dots-from-stray-light-corrected-hinode-filtergrams-replacement/</link>
		<comments>http://voxcharta.org/2012/05/09/properties-of-umbral-dots-from-stray-light-corrected-hinode-filtergrams-replacement/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:31:55 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[continuum]]></category>
		<category><![CDATA[dots]]></category>
		<category><![CDATA[filament]]></category>
		<category><![CDATA[filamentary structure]]></category>
		<category><![CDATA[geometric properties]]></category>
		<category><![CDATA[grains]]></category>
		<category><![CDATA[horizontal speed]]></category>
		<category><![CDATA[image contrast]]></category>
		<category><![CDATA[kinematic properties]]></category>
		<category><![CDATA[numerical simulation]]></category>
		<category><![CDATA[peak intensity]]></category>
		<category><![CDATA[rms]]></category>
		<category><![CDATA[scattered light]]></category>
		<category><![CDATA[stray light]]></category>
		<category><![CDATA[sunspot]]></category>
		<category><![CDATA[telescopes]]></category>
		<category><![CDATA[time interval]]></category>
		<category><![CDATA[time sequence]]></category>
		<category><![CDATA[trajectory]]></category>
		<category><![CDATA[umbra penumbra]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/properties-of-umbral-dots-from-stray-light-corrected-hinode-filtergrams-replacement/</guid>
		<description><![CDATA[High resolution blue continuum filtergrams from Hinode are employed to study the umbral fine structure of a regular unipolar sunspot. The removal of scattered light from the images increases the rms contrast by a factor of 1.45 on average. Improvement in image contrast renders identification of short filamentary structures resembling penumbrae that are well separated [...]]]></description>
			<content:encoded><![CDATA[<p>High resolution blue continuum filtergrams from Hinode are employed to study the umbral fine structure of a regular unipolar sunspot. The removal of scattered light from the images increases the rms contrast by a factor of 1.45 on average. Improvement in image contrast renders identification of short filamentary structures resembling penumbrae that are well separated from the umbra-penumbra boundary and comprise bright filaments/grains flanking dark filaments. Such fine structures were recently detected from ground based telescopes and have now been observed with Hinode. A multi-level tracking algorithm was used to identify umbral dots in both the uncorrected and corrected images and to track them in time. The distribution of the values describing the photometric and geometric properties of umbral dots are more easily affected by the presence of stray light while it is less severe in the case of kinematic properties. Statistically, umbral dots exhibit a peak intensity, effective diameter, lifetime, horizontal speed and a trajectory length of 0.29 I_QS, 272 km, 8.4 min, 0.45 km/s and 221 km respectively. The 2 hr 20 min time sequence depicts several locations where umbral dots tend to appear and disappear repeatedly with various time intervals. The correction for scattered light in the Hinode filtergrams facilitates photometry of umbral fine structure which can be related to results obtained from larger telescopes and numerical simulations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/properties-of-umbral-dots-from-stray-light-corrected-hinode-filtergrams-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>RX J0942.7-7726AB: an isolated pre-main sequence wide binary</title>
		<link>http://voxcharta.org/2012/05/08/rx-j0942-7-7726ab-an-isolated-pre-main-sequence-wide-binary/</link>
		<comments>http://voxcharta.org/2012/05/08/rx-j0942-7-7726ab-an-isolated-pre-main-sequence-wide-binary/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:47:06 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[2mass]]></category>
		<category><![CDATA[arcsec]]></category>
		<category><![CDATA[binaries]]></category>
		<category><![CDATA[cen]]></category>
		<category><![CDATA[eta]]></category>
		<category><![CDATA[fragile systems]]></category>
		<category><![CDATA[main sequence star]]></category>
		<category><![CDATA[medium resolution]]></category>
		<category><![CDATA[molecular cloud]]></category>
		<category><![CDATA[open cluster]]></category>
		<category><![CDATA[proper motion]]></category>
		<category><![CDATA[radial velocity]]></category>
		<category><![CDATA[resolution spectroscopy]]></category>
		<category><![CDATA[scorpius]]></category>
		<category><![CDATA[turbulent environment]]></category>
		<category><![CDATA[velocities]]></category>
		<category><![CDATA[velocity difference]]></category>
		<category><![CDATA[velocity vector]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/rx-j0942-7-7726ab-an-isolated-pre-main-sequence-wide-binary/</guid>
		<description><![CDATA[We report the discovery of two young M-dwarfs, RX J0942.7-7726 (M1) and 2MASS J09424157-7727130 (M4.5), that were found only 42 arcsec apart in a survey for pre-main sequence stars surrounding the open cluster eta Chamaeleontis. Both stars have congruent proper motions and near-infrared photometry. Medium-resolution spectroscopy reveals that they are coeval (age 8-12 Myr), codistant [...]]]></description>
			<content:encoded><![CDATA[<p>We report the discovery of two young M-dwarfs, RX J0942.7-7726 (M1) and 2MASS J09424157-7727130 (M4.5), that were found only 42 arcsec apart in a survey for pre-main sequence stars surrounding the open cluster eta Chamaeleontis. Both stars have congruent proper motions and near-infrared photometry. Medium-resolution spectroscopy reveals that they are coeval (age 8-12 Myr), codistant (100-150 pc) and thus almost certainly form a true wide binary with a projected separation of 4000-6000 AU. The system appears too old and dynamically fragile to have originated in eta Cha and a traceback analysis argues for its birth in or near the Scorpius-Centaurus OB Association. RX J0942.7-7726AB joins a growing group of wide binaries kinematically linked to Sco-Cen, suggesting that such fragile systems can survive the turbulent environment of their natal molecular clouds while still being dispersed with large velocities. Conversely, the small radial velocity difference between the stars (2.7 \pm 1.0 km/s) could mean the system is unbound, a result of the coincidental ejection of two single stars with similar velocity vectors from the OB association early in its evolution.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/rx-j0942-7-7726ab-an-isolated-pre-main-sequence-wide-binary/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The star formation history of RCW 36</title>
		<link>http://voxcharta.org/2012/05/08/the-star-formation-history-of-rcw-36/</link>
		<comments>http://voxcharta.org/2012/05/08/the-star-formation-history-of-rcw-36/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:46:07 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[bipolar]]></category>
		<category><![CDATA[generations]]></category>
		<category><![CDATA[insight]]></category>
		<category><![CDATA[jet structure]]></category>
		<category><![CDATA[jets]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[molecular cloud]]></category>
		<category><![CDATA[periphery]]></category>
		<category><![CDATA[photometric]]></category>
		<category><![CDATA[plasma]]></category>
		<category><![CDATA[shooter]]></category>
		<category><![CDATA[spectroscopic observation]]></category>
		<category><![CDATA[spectrum]]></category>
		<category><![CDATA[star formation history]]></category>
		<category><![CDATA[stellar object]]></category>
		<category><![CDATA[young stars]]></category>
		<category><![CDATA[yso]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/the-star-formation-history-of-rcw-36/</guid>
		<description><![CDATA[Recent studies of massive-star forming regions indicate that they can contain multiple generations of young stars. These observations suggest that star formation in these regions is sequential and/or triggered by a previous generation of (massive) stars. Here we present new observations of the star forming region RCW 36 in the Vela Molecular Ridge, hosting a [...]]]></description>
			<content:encoded><![CDATA[<p>Recent studies of massive-star forming regions indicate that they can contain multiple generations of young stars. These observations suggest that star formation in these regions is sequential and/or triggered by a previous generation of (massive) stars. Here we present new observations of the star forming region RCW 36 in the Vela Molecular Ridge, hosting a young cluster of massive stars embedded in a molecular cloud complex. In the periphery of the cluster several young stellar objects (YSOs) are detected which produce bipolar jets (HH 1042 and HH 1043) demonstrating that these objects are still actively accreting. The VLT/X-shooter spectrum of the jet structure of HH 1042 provides detailed information on the physical conditions and kinematical properties of the jet plasma. From this information the YSO&#8217;s accretion history can be derived. Combining the photometric and spectroscopic observations of RCW 36 gives insight into the formation process of individual stars and the star formation history of this young massive-star forming region.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/the-star-formation-history-of-rcw-36/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Circumbinary Gas Accretion onto a Central Binary: Infrared Molecular Hydrogen Emission from GG Tau A</title>
		<link>http://voxcharta.org/2012/05/08/circumbinary-gas-accretion-onto-a-central-binary-infrared-molecular-hydrogen-emission-from-gg-tau-a/</link>
		<comments>http://voxcharta.org/2012/05/08/circumbinary-gas-accretion-onto-a-central-binary-infrared-molecular-hydrogen-emission-from-gg-tau-a/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:45:12 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[binaries]]></category>
		<category><![CDATA[central star]]></category>
		<category><![CDATA[circumstellar environment]]></category>
		<category><![CDATA[excitation mechanism]]></category>
		<category><![CDATA[gap]]></category>
		<category><![CDATA[gas emission]]></category>
		<category><![CDATA[high spatial resolution]]></category>
		<category><![CDATA[hydrogen emission]]></category>
		<category><![CDATA[line ratio]]></category>
		<category><![CDATA[micron]]></category>
		<category><![CDATA[molecular hydrogen]]></category>
		<category><![CDATA[resolution maps]]></category>
		<category><![CDATA[spatial location]]></category>
		<category><![CDATA[streamer]]></category>
		<category><![CDATA[tau]]></category>
		<category><![CDATA[uv emission]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[young stars]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/circumbinary-gas-accretion-onto-a-central-binary-infrared-molecular-hydrogen-emission-from-gg-tau-a/</guid>
		<description><![CDATA[We present high spatial resolution maps of ro-vibrational molecular hydrogen emission from the environment of the GG Tau A binary component in the GG Tau quadruple system. The H2 v= 1-0 S(1) emission is spatially resolved and encompasses the inner binary, with emission detected at locations that should be dynamically cleared on several hundred-year timescales. [...]]]></description>
			<content:encoded><![CDATA[<p>We present high spatial resolution maps of ro-vibrational molecular hydrogen emission from the environment of the GG Tau A binary component in the GG Tau quadruple system. The H2 v= 1-0 S(1) emission is spatially resolved and encompasses the inner binary, with emission detected at locations that should be dynamically cleared on several hundred-year timescales. Extensions of H2 gas emission are seen to ~100 AU distances from the central stars. The v = 2-1 S(1) emission at 2.24 microns is also detected at ~30 AU from the central stars, with a line ratio of 0.05 +/- 0.01 with respect to the v = 1-0 S(1) emission. Assuming gas in LTE, this ratio corresponds to an emission environment at ~1700 K. We estimate that this temperature is too high for quiescent gas heated by X-ray or UV emission from the central stars. Surprisingly, we find that the brightest region of H2 emission arises from a spatial location that is exactly coincident with a recently revealed dust &#8220;streamer&#8221; which seems to be transferring material from the outer circumbinary ring around GG Tau A into the inner region. As a result, we identify a new excitation mechanism for ro-vibrational H2 stimulation in the environment of young stars. The H2 in the GG Tau A system appears to be stimulated by mass accretion infall as material in the circumbinary ring accretes onto the system to replenish the inner circumstellar disks. We postulate that H2 stimulated by accretion infall could be present in other systems, particularly binaries and &#8220;transition disk&#8221; systems which have dust cleared gaps in their circumstellar environments.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/circumbinary-gas-accretion-onto-a-central-binary-infrared-molecular-hydrogen-emission-from-gg-tau-a/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>On the Amplitude of Convective Velocities in the Deep Solar Interior</title>
		<link>http://voxcharta.org/2012/05/08/on-the-amplitude-of-convective-velocities-in-the-deep-solar-interior/</link>
		<comments>http://voxcharta.org/2012/05/08/on-the-amplitude-of-convective-velocities-in-the-deep-solar-interior/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:44:51 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[angular momentum transport]]></category>
		<category><![CDATA[characteristic length]]></category>
		<category><![CDATA[circulation]]></category>
		<category><![CDATA[convective motion]]></category>
		<category><![CDATA[differential]]></category>
		<category><![CDATA[differential rotation]]></category>
		<category><![CDATA[dynamo models]]></category>
		<category><![CDATA[efficiency]]></category>
		<category><![CDATA[gyroscopic]]></category>
		<category><![CDATA[linchpin]]></category>
		<category><![CDATA[mhd equations]]></category>
		<category><![CDATA[reynolds stress]]></category>
		<category><![CDATA[shear layer]]></category>
		<category><![CDATA[solar convection zone]]></category>
		<category><![CDATA[solar interior]]></category>
		<category><![CDATA[turbulent transport]]></category>
		<category><![CDATA[velocities]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/on-the-amplitude-of-convective-velocities-in-the-deep-solar-interior/</guid>
		<description><![CDATA[We obtain lower limits on the amplitude of convective velocities in the deep solar convection zone based only on the observed properties of the differential rotation and meridional circulation together with simple and robust dynamical balances obtained from the fundamental MHD equations. The linchpin of the approach is the concept of gyroscopic pumping whereby the [...]]]></description>
			<content:encoded><![CDATA[<p>We obtain lower limits on the amplitude of convective velocities in the deep solar convection zone based only on the observed properties of the differential rotation and meridional circulation together with simple and robust dynamical balances obtained from the fundamental MHD equations. The linchpin of the approach is the concept of gyroscopic pumping whereby the meridional circulation across isosurfaces of specific angular momentum is linked to the angular momentum transport by the convective Reynolds stress. We find that the amplitude of the convective velocity must be at least 30 m s$^{-1}$ in the upper CZ ($r \sim 0.95 R$) and at least 8 m s$^{-1}$ in the lower CZ ($r \sim 0.75 R$) in order to be consistent with the observed mean flows. Using the base of the near-surface shear layer as a probe of the rotational influence, we are further able to show that the characteristic length scale of deep convective motions must be no smaller than 5.5&#8211;30 Mm. These results are compatible with convection models but suggest that the efficiency of the turbulent transport assumed in advection-dominated flux-transport dynamo models is generally not consistent with the mean flows they employ.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/on-the-amplitude-of-convective-velocities-in-the-deep-solar-interior/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Direct modeling of neutral helium in the heliosphere</title>
		<link>http://voxcharta.org/2012/05/08/direct-modeling-of-neutral-helium-in-the-heliosphere/</link>
		<comments>http://voxcharta.org/2012/05/08/direct-modeling-of-neutral-helium-in-the-heliosphere/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:43:37 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accounting]]></category>
		<category><![CDATA[charge exchange]]></category>
		<category><![CDATA[distribution function]]></category>
		<category><![CDATA[distributions]]></category>
		<category><![CDATA[heliosphere]]></category>
		<category><![CDATA[helium distribution]]></category>
		<category><![CDATA[ibex]]></category>
		<category><![CDATA[inference]]></category>
		<category><![CDATA[interstellar medium]]></category>
		<category><![CDATA[nasa]]></category>
		<category><![CDATA[neutral atom]]></category>
		<category><![CDATA[neutral helium]]></category>
		<category><![CDATA[neutral particle]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[oxygen ions]]></category>
		<category><![CDATA[particle measurements]]></category>
		<category><![CDATA[plasma]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[spacecraft]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/direct-modeling-of-neutral-helium-in-the-heliosphere/</guid>
		<description><![CDATA[Several years of neutral particle measurements by the NASA/IBEX mission have yielded direct observations of interstellar neutral helium and oxygen. The data indicate the presence of secondary neutral helium and oxygen, which are created within the heliosphere by charge exchange involving helium or oxygen ions. This contribution describes a detailed conserving calculation method based on [...]]]></description>
			<content:encoded><![CDATA[<p>Several years of neutral particle measurements by the NASA/IBEX mission have yielded direct observations of interstellar neutral helium and oxygen. The data indicate the presence of secondary neutral helium and oxygen, which are created within the heliosphere by charge exchange involving helium or oxygen ions. This contribution describes a detailed conserving calculation method based on Keplerian orbits that has been developed to characterize helium distribution functions throughout the heliosphere, in particular in the innermost heliosphere, while accounting for loss and production of neutral particles along their path. Coupled with global heliosphere models of plasma distributions, this code is useful for predicting the fluxes of heavy neutral atoms at spacecraft detectors, so enabling inferences on the characteristics of the interstellar medium.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/direct-modeling-of-neutral-helium-in-the-heliosphere/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Long-term Variations of Solar Differential Rotation and Sunspot Activity: Revisited</title>
		<link>http://voxcharta.org/2012/05/08/long-term-variations-of-solar-differential-rotation-and-sunspot-activity-revisited/</link>
		<comments>http://voxcharta.org/2012/05/08/long-term-variations-of-solar-differential-rotation-and-sunspot-activity-revisited/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:40:57 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[callebaut]]></category>
		<category><![CDATA[differential]]></category>
		<category><![CDATA[differential rotation]]></category>
		<category><![CDATA[equator]]></category>
		<category><![CDATA[latitude]]></category>
		<category><![CDATA[makarov]]></category>
		<category><![CDATA[negative correlation]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[rotation rate]]></category>
		<category><![CDATA[secular trend]]></category>
		<category><![CDATA[solar rotation]]></category>
		<category><![CDATA[solar surface]]></category>
		<category><![CDATA[statistical significance]]></category>
		<category><![CDATA[sunspot activity]]></category>
		<category><![CDATA[sunspot area]]></category>
		<category><![CDATA[term variation]]></category>
		<category><![CDATA[ulrich]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/long-term-variations-of-solar-differential-rotation-and-sunspot-activity-revisited/</guid>
		<description><![CDATA[Long-term variations of solar differential rotation and sunspot activity are investigated through re-analyzing the data on parameters of the differential rotation law obtained by Makarov, Tlatov, and Callebaut (1997), Javaraiah, Bertello, and Ulrich (2005a, b), and Javaraiah et al. (2009). Our results indicate that the solar surface rotation rate at the Equator (indicated by the [...]]]></description>
			<content:encoded><![CDATA[<p>Long-term variations of solar differential rotation and sunspot activity are investigated through re-analyzing the data on parameters of the differential rotation law obtained by Makarov, Tlatov, and Callebaut (1997), Javaraiah, Bertello, and Ulrich (2005a, b), and Javaraiah et al. (2009). Our results indicate that the solar surface rotation rate at the Equator (indicated by the A parameter of the standard solar rotation law) shows a secular decrease since cycle 12 onwards, given by about $1\,-\,1.5\times10^{-3}$($deg\ day^{-1} year^{-1}$). The B parameter of the standard differential rotation law seems to also show a secular decrease since cycle 12 onwards, but of weak statistical significance. The rotation rate averaged on latitudes ($0^{o}\,&#8211;\,40^{o}$) does not show a secular trend of statistical significance. Moreover, the average sunspot area shows a secular increase of statistical significance since cycle 12 onwards, while a negative correlation is found between the level of sunspot activity (indicated by the average sunspot area) and the solar equatorial rotation in the long run.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/long-term-variations-of-solar-differential-rotation-and-sunspot-activity-revisited/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Infant mortality without gas expulsion? The rapid dispersal of virialised low mass clusters</title>
		<link>http://voxcharta.org/2012/05/08/infant-mortality-without-gas-expulsion-the-rapid-dispersal-of-virialised-low-mass-clusters/</link>
		<comments>http://voxcharta.org/2012/05/08/infant-mortality-without-gas-expulsion-the-rapid-dispersal-of-virialised-low-mass-clusters/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:37:00 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[10s]]></category>
		<category><![CDATA[body simulation]]></category>
		<category><![CDATA[cluster mass]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[dispersal]]></category>
		<category><![CDATA[disruption]]></category>
		<category><![CDATA[dynamical evolution]]></category>
		<category><![CDATA[efficiency]]></category>
		<category><![CDATA[expulsion]]></category>
		<category><![CDATA[gravitational collapse]]></category>
		<category><![CDATA[infant mortality]]></category>
		<category><![CDATA[initial condition]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[mass spectrum]]></category>
		<category><![CDATA[massive cluster]]></category>
		<category><![CDATA[solar neighborhood]]></category>
		<category><![CDATA[star cluster]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[stellar dynamics]]></category>
		<category><![CDATA[timescale]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/infant-mortality-without-gas-expulsion-the-rapid-dispersal-of-virialised-low-mass-clusters/</guid>
		<description><![CDATA[Infant mortality brought about by the expulsion of a star cluster&#8217;s natal gas is widely invoked to explain cluster statistics at different ages. While a well studied problem, most recent studies of gas expulsion&#8217;s effect on a cluster have focused on massive clusters, with stellar counts of order $10^4$. Here we argue that the evolutionary [...]]]></description>
			<content:encoded><![CDATA[<p>Infant mortality brought about by the expulsion of a star cluster&#8217;s natal gas is widely invoked to explain cluster statistics at different ages. While a well studied problem, most recent studies of gas expulsion&#8217;s effect on a cluster have focused on massive clusters, with stellar counts of order $10^4$. Here we argue that the evolutionary timescales associated with the compact low-mass clusters typical of the median cluster in the Solar neighborhood are short enough that significant dynamical evolution can take place over the ages usually associated with gas expulsion. To test this we perform {\it N}-body simulations of the dynamics of a very young star forming region, with initial conditions drawn from a large-scale hydrodynamic simulation of gravitational collapse and fragmentation. The subclusters we analyse have high local star formation efficiencies and are roughly virialised, and have populations of a few hundred stars. Over 10 Myr they expand to a similar degree as would be expected from gas expulsion if they were initially gas-rich, but the expansion is purely due to the internal stellar dynamics of the young clusters. The expansion is such that the stellar densities at 2 Myr match those of YSOs in the Solar neighborhood. We argue that at the low-mass end of the cluster mass spectrum, a deficit of clusters at 10s of Myr does not necessarily imply gas expulsion as a disruption mechanism.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/infant-mortality-without-gas-expulsion-the-rapid-dispersal-of-virialised-low-mass-clusters/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Period decrease in three SuperWASP eclipsing binary candidates near the short-period limit</title>
		<link>http://voxcharta.org/2012/05/08/period-decrease-in-three-superwasp-eclipsing-binary-candidates-near-the-short-period-limit/</link>
		<comments>http://voxcharta.org/2012/05/08/period-decrease-in-three-superwasp-eclipsing-binary-candidates-near-the-short-period-limit/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:36:51 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[angular momentum]]></category>
		<category><![CDATA[gravitational radiation]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[mass transfer]]></category>
		<category><![CDATA[momentum loss]]></category>
		<category><![CDATA[orbital period]]></category>
		<category><![CDATA[period change]]></category>
		<category><![CDATA[radiation effects]]></category>
		<category><![CDATA[short period]]></category>
		<category><![CDATA[sigma]]></category>
		<category><![CDATA[uma]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/period-decrease-in-three-superwasp-eclipsing-binary-candidates-near-the-short-period-limit/</guid>
		<description><![CDATA[SuperWASP light curves for 53 W UMa-type eclipsing binary (EB) candidates, identified in previous work as being close to the contact binary short-period limit, were studied for evidence of period change. The orbital periods of most of the stars were confirmed, and period decrease, significant at more than 5 sigma, was observed in three objects: [...]]]></description>
			<content:encoded><![CDATA[<p>SuperWASP light curves for 53 W UMa-type eclipsing binary (EB) candidates, identified in previous work as being close to the contact binary short-period limit, were studied for evidence of period change. The orbital periods of most of the stars were confirmed, and period decrease, significant at more than 5 sigma, was observed in three objects: 1SWASP J174310.98+432709.6 (-0.055 \pm0.003 s/yr), 1SWASP J133105.91+121538.0 (-0.075 \pm0.013 s/yr) and 1SWASP J234401.81-212229.1 (-0.313 \pm0.019 s/yr). The magnitudes of the observed period changes cannot be explained by magnetic braking or gravitational radiation effects, and are most likely primarily due to unstable mass transfer from primary to secondary components, possibly accompanied by unstable mass and angular momentum loss from the systems. If these period decreases persist, the systems could merge on a relatively short timescale.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/period-decrease-in-three-superwasp-eclipsing-binary-candidates-near-the-short-period-limit/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>A new soft X-ray spectral model for polars with an application to AM Herculis</title>
		<link>http://voxcharta.org/2012/05/08/a-new-soft-x-ray-spectral-model-for-polars-with-an-application-to-am-herculis/</link>
		<comments>http://voxcharta.org/2012/05/08/a-new-soft-x-ray-spectral-model-for-polars-with-an-application-to-am-herculis/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:36:32 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[Chandra]]></category>
		<category><![CDATA[exponential distribution]]></category>
		<category><![CDATA[free parameter]]></category>
		<category><![CDATA[heuristic model]]></category>
		<category><![CDATA[normalization]]></category>
		<category><![CDATA[polars]]></category>
		<category><![CDATA[prototype]]></category>
		<category><![CDATA[soft x]]></category>
		<category><![CDATA[spectral model]]></category>
		<category><![CDATA[spectrum]]></category>
		<category><![CDATA[temperature distribution]]></category>
		<category><![CDATA[wavelength]]></category>
		<category><![CDATA[white dwarf]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/a-new-soft-x-ray-spectral-model-for-polars-with-an-application-to-am-herculis/</guid>
		<description><![CDATA[We present a simple heuristic model for the time-averaged soft X-ray temperature distribution in the accretion spot on the white dwarf in polars. The model is based on the analysis of the Chandra LETG spectrum of the prototype polar AM Her and involves an exponential distribution of the emitting area vs. blackbody temperature a(T) = [...]]]></description>
			<content:encoded><![CDATA[<p>We present a simple heuristic model for the time-averaged soft X-ray temperature distribution in the accretion spot on the white dwarf in polars. The model is based on the analysis of the Chandra LETG spectrum of the prototype polar AM Her and involves an exponential distribution of the emitting area vs. blackbody temperature a(T) = a0 exp(-T/T0). With one free parameter besides the normalization, it is mathematically as simple as the single blackbody, but is physically more plausible and fits the soft X-ray and far-ultraviolet spectral fluxes much better. The model yields more reliable values of the wavelength-integrated flux of the soft X-ray component and the implied accretion rate than reported previously.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/a-new-soft-x-ray-spectral-model-for-polars-with-an-application-to-am-herculis/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Time series of high resolution photospheric spectra in a quiet region of the Sun. I. Analysis of global and spatial variations of line parameters</title>
		<link>http://voxcharta.org/2012/05/08/time-series-of-high-resolution-photospheric-spectra-in-a-quiet-region-of-the-sun-i-analysis-of-global-and-spatial-variations-of-line-parameters/</link>
		<comments>http://voxcharta.org/2012/05/08/time-series-of-high-resolution-photospheric-spectra-in-a-quiet-region-of-the-sun-i-analysis-of-global-and-spatial-variations-of-line-parameters/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:35:22 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[coherence]]></category>
		<category><![CDATA[continuum]]></category>
		<category><![CDATA[convective motion]]></category>
		<category><![CDATA[correlation coefficient]]></category>
		<category><![CDATA[equivalent width]]></category>
		<category><![CDATA[gravity wave]]></category>
		<category><![CDATA[intensity pattern]]></category>
		<category><![CDATA[line parameters]]></category>
		<category><![CDATA[observatorio del teide]]></category>
		<category><![CDATA[phase shift]]></category>
		<category><![CDATA[quiet region]]></category>
		<category><![CDATA[quiet sun]]></category>
		<category><![CDATA[slit]]></category>
		<category><![CDATA[spatial variation]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[time series]]></category>
		<category><![CDATA[vacuum tower telescope]]></category>
		<category><![CDATA[velocity gradient]]></category>
		<category><![CDATA[velocity pattern]]></category>
		<category><![CDATA[vertical structure]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/time-series-of-high-resolution-photospheric-spectra-in-a-quiet-region-of-the-sun-i-analysis-of-global-and-spatial-variations-of-line-parameters/</guid>
		<description><![CDATA[A 50 min time series of one-dimensional slit-spectrograms, taken in quiet sun at disk center, observed at the German Vacuum Tower Telescope (Observatorio del Teide), was used to study the global and spatial variations of different line parameters. In order to determine the vertical structure of the photosphere two lines with well separated formation heights [...]]]></description>
			<content:encoded><![CDATA[<p>A 50 min time series of one-dimensional slit-spectrograms, taken in quiet sun at disk center, observed at the German Vacuum Tower Telescope (Observatorio del Teide), was used to study the global and spatial variations of different line parameters. In order to determine the vertical structure of the photosphere two lines with well separated formation heights have been considered. The data have been filtered of p-modes to isolate the pure convective phenomenon. From our studies of global correlation coefficients and coherence and phase shift analyzes between the several line parameters, the following results can be reported. The convective velocity pattern preserves structures larger than 1.0&#8243; up to the highest layers of the photosphere (~ 435 km). However, at these layers, in the intensity pattern only structures larger than 2.0&#8243; are still connected with those at the continuum level although showing inverted brightness contrast. This confirms an inversion of temperature that we have found at a height of ~140 km. A possible evidence of gravity waves superimposed to the convective motions is derived from the phase shift analysis. We interpret the behavior of the full width at half maximum and the equivalent width as a function of the distance to the granular borders, as a consequence of enhanced turbulence and/or strong velocity gradients in the intergranular lanes.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/time-series-of-high-resolution-photospheric-spectra-in-a-quiet-region-of-the-sun-i-analysis-of-global-and-spatial-variations-of-line-parameters/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Time series of high resolution photospheric spectra in a quiet region of the Sun. II. Analysis of the variation of physical quantities of granular structures</title>
		<link>http://voxcharta.org/2012/05/08/time-series-of-high-resolution-photospheric-spectra-in-a-quiet-region-of-the-sun-ii-analysis-of-the-variation-of-physical-quantities-of-granular-structures/</link>
		<comments>http://voxcharta.org/2012/05/08/time-series-of-high-resolution-photospheric-spectra-in-a-quiet-region-of-the-sun-ii-analysis-of-the-variation-of-physical-quantities-of-granular-structures/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:35:11 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cell model]]></category>
		<category><![CDATA[flow velocity]]></category>
		<category><![CDATA[granular scales]]></category>
		<category><![CDATA[granule]]></category>
		<category><![CDATA[height variation]]></category>
		<category><![CDATA[increasing height]]></category>
		<category><![CDATA[optical depth]]></category>
		<category><![CDATA[phase shift]]></category>
		<category><![CDATA[photosphere]]></category>
		<category><![CDATA[physical quantity]]></category>
		<category><![CDATA[quiet region]]></category>
		<category><![CDATA[quiet sun]]></category>
		<category><![CDATA[spatial coherence]]></category>
		<category><![CDATA[stratification]]></category>
		<category><![CDATA[temperature contrast]]></category>
		<category><![CDATA[temperature fluctuation]]></category>
		<category><![CDATA[temporal distribution]]></category>
		<category><![CDATA[vertical flow]]></category>
		<category><![CDATA[vertical velocity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/time-series-of-high-resolution-photospheric-spectra-in-a-quiet-region-of-the-sun-ii-analysis-of-the-variation-of-physical-quantities-of-granular-structures/</guid>
		<description><![CDATA[From the inversion of a time series of high resolution slit spectrograms obtained from the quiet sun, the spatial and temporal distribution of the thermodynamical quantities and the vertical flow velocity is derived as a function of logarithmic optical depth and geometrical height. Spatial coherence and phase shift analyzes between temperature and vertical velocity depict [...]]]></description>
			<content:encoded><![CDATA[<p>From the inversion of a time series of high resolution slit spectrograms obtained from the quiet sun, the spatial and temporal distribution of the thermodynamical quantities and the vertical flow velocity is derived as a function of logarithmic optical depth and geometrical height. Spatial coherence and phase shift analyzes between temperature and vertical velocity depict the height variation of these physical quantities for structures of different size. An average granular cell model is presented, showing the granule-intergranular lane stratification of temperature, vertical velocity, gas pressure and density as a function of logarithmic optical depth and geometrical height. Studies of a specific small and a specific large granular cell complement these results. A strong decay of the temperature fluctuations with increasing height together with a less efficient penetration of smaller cells is revealed. The T -T coherence at all granular scales is broken already at log tau =-1 or z~170 km. At the layers beyond, an inversion of the temperature contrast is revealed. Vertical velocities are in phase throughout the photosphere and penetrate into the highest layers under study.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/time-series-of-high-resolution-photospheric-spectra-in-a-quiet-region-of-the-sun-ii-analysis-of-the-variation-of-physical-quantities-of-granular-structures/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Heating of Flare Loops With Observationally Constrained Heating Functions [Replacement]</title>
		<link>http://voxcharta.org/2012/05/08/heating-of-flare-loops-with-observationally-constrained-heating-functions-replacement-3/</link>
		<comments>http://voxcharta.org/2012/05/08/heating-of-flare-loops-with-observationally-constrained-heating-functions-replacement-3/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:33:02 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[30 minutes]]></category>
		<category><![CDATA[aia]]></category>
		<category><![CDATA[august 1]]></category>
		<category><![CDATA[cadence]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[duration]]></category>
		<category><![CDATA[few minutes]]></category>
		<category><![CDATA[flare loops]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[magnetic reconnection]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[plasma]]></category>
		<category><![CDATA[radiation]]></category>
		<category><![CDATA[resolution observations]]></category>
		<category><![CDATA[sdo]]></category>
		<category><![CDATA[soft x]]></category>
		<category><![CDATA[timescale]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/heating-of-flare-loops-with-observationally-constrained-heating-functions-replacement-3/</guid>
		<description><![CDATA[We analyze high cadence high resolution observations of a C3.2 flare obtained by AIA/SDO on August 1, 2010. The flare is a long duration event with soft X-ray and EUV radiation lasting for over four hours. Analysis suggests that magnetic reconnection and formation of new loops continue for more than two hours. Furthermore, the UV [...]]]></description>
			<content:encoded><![CDATA[<p>We analyze high cadence high resolution observations of a C3.2 flare obtained by AIA/SDO on August 1, 2010. The flare is a long duration event with soft X-ray and EUV radiation lasting for over four hours. Analysis suggests that magnetic reconnection and formation of new loops continue for more than two hours. Furthermore, the UV 1600\AA\ observations show that each of the individual pixels at the feet of flare loops is brightened instantaneously with a timescale of a few minutes, and decays over a much longer timescale of more than 30 minutes. We use these spatially resolved UV light curves during the rise phase to construct empirical heating functions for individual flare loops, and model heating of coronal plasmas in these loops. The total coronal radiation of these flare loops are compared with soft X-ray and EUV radiation fluxes measured by GOES and AIA. This study presents a method to observationally infer heating functions in numerous flare loops that are formed and heated sequentially by reconnection throughout the flare, and provides a very useful constraint to coronal heating models.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/heating-of-flare-loops-with-observationally-constrained-heating-functions-replacement-3/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Discovery of Super-Li Rich Red Giants in Dwarf Spheroidal Galaxies [Replacement]</title>
		<link>http://voxcharta.org/2012/05/08/discovery-of-super-li-rich-red-giants-in-dwarf-spheroidal-galaxies-replacement/</link>
		<comments>http://voxcharta.org/2012/05/08/discovery-of-super-li-rich-red-giants-in-dwarf-spheroidal-galaxies-replacement/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:31:25 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bump]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[envelopes]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[first ascent]]></category>
		<category><![CDATA[giant branch]]></category>
		<category><![CDATA[Lithium]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[luminosity function]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[new discovery]]></category>
		<category><![CDATA[red giant]]></category>
		<category><![CDATA[satellite galaxy]]></category>
		<category><![CDATA[spheroidal galaxy]]></category>
		<category><![CDATA[temperature]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/discovery-of-super-li-rich-red-giants-in-dwarf-spheroidal-galaxies-replacement/</guid>
		<description><![CDATA[Stars destroy lithium (Li) in their normal evolution. The convective envelopes of evolved red giants reach temperatures of millions of K, hot enough for the 7Li(p,alpha)4He reaction to burn Li efficiently. Only about 1% of first-ascent red giants more luminous than the luminosity function bump in the red giant branch exhibit A(Li) &#62; 1.5. Nonetheless, [...]]]></description>
			<content:encoded><![CDATA[<p>Stars destroy lithium (Li) in their normal evolution. The convective envelopes of evolved red giants reach temperatures of millions of K, hot enough for the 7Li(p,alpha)4He reaction to burn Li efficiently. Only about 1% of first-ascent red giants more luminous than the luminosity function bump in the red giant branch exhibit A(Li) &gt; 1.5. Nonetheless, Li-rich red giants do exist. We present 15 Li-rich red giants&#8211;14 of which are new discoveries&#8211;among a sample of 2054 red giants in Milky Way dwarf satellite galaxies. Our sample more than doubles the number of low-mass, metal-poor ([Fe/H] &lt;~ -0.7) Li-rich red giants, and it includes the most-metal poor Li-enhanced star known ([Fe/H] = -2.82, A(Li)_NLTE = 3.15). Because most of these stars have Li abundances larger than the universe&#039;s primordial value, the Li in these stars must have been created rather than saved from destruction. These Li-rich stars appear like other stars in the same galaxies in every measurable regard other than Li abundance. We consider the possibility that Li enrichment is a universal phase of evolution that affects all stars, and it seems rare only because it is brief.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/discovery-of-super-li-rich-red-giants-in-dwarf-spheroidal-galaxies-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Discovery of Super-Li Rich Red Giants in Dwarf Spheroidal Galaxies</title>
		<link>http://voxcharta.org/2012/05/07/discovery-of-super-li-rich-red-giants-in-dwarf-spheroidal-galaxies/</link>
		<comments>http://voxcharta.org/2012/05/07/discovery-of-super-li-rich-red-giants-in-dwarf-spheroidal-galaxies/#comments</comments>
		<pubDate>Tue, 08 May 2012 01:07:45 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bump]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[envelopes]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[first ascent]]></category>
		<category><![CDATA[giant branch]]></category>
		<category><![CDATA[Lithium]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[luminosity function]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[new discovery]]></category>
		<category><![CDATA[red giant]]></category>
		<category><![CDATA[satellite galaxy]]></category>
		<category><![CDATA[spheroidal galaxy]]></category>
		<category><![CDATA[temperature]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/discovery-of-super-li-rich-red-giants-in-dwarf-spheroidal-galaxies/</guid>
		<description><![CDATA[Stars destroy lithium (Li) in their normal evolution. The convective envelopes of evolved red giants reach temperatures of millions of K, hot enough for the 7Li(p,alpha)4He reaction to burn Li efficiently. Only about 1% of first-ascent red giants more luminous than the luminosity function bump in the red giant branch exhibit A(Li) &#62; 1.5. Nonetheless, [...]]]></description>
			<content:encoded><![CDATA[<p>Stars destroy lithium (Li) in their normal evolution. The convective envelopes of evolved red giants reach temperatures of millions of K, hot enough for the 7Li(p,alpha)4He reaction to burn Li efficiently. Only about 1% of first-ascent red giants more luminous than the luminosity function bump in the red giant branch exhibit A(Li) &gt; 1.5. Nonetheless, Li-rich red giants do exist. We present 15 Li-rich red giants&#8211;14 of which are new discoveries&#8211;among a sample of 2054 red giants in Milky Way dwarf satellite galaxies. Our sample more than doubles the number of low-mass, metal-poor ([Fe/H] &lt;~ -0.7) Li-rich red giants, and it includes the most-metal poor Li-enhanced star known ([Fe/H] = -2.82, A(Li)_NLTE = 3.15). Because most of these stars have Li abundances larger than the universe&#039;s primordial value, the Li in these stars must have been created rather than saved from destruction. These Li-rich stars appear like other stars in the same galaxies in every measurable regard other than Li abundance. We consider the possibility that Li enrichment is a universal phase of evolution that affects all stars, and it seems rare only because it is brief.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/discovery-of-super-li-rich-red-giants-in-dwarf-spheroidal-galaxies/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Free-free Emission and Radio Recombination Lines from Photoevaporating Disks</title>
		<link>http://voxcharta.org/2012/05/07/free-free-emission-and-radio-recombination-lines-from-photoevaporating-disks/</link>
		<comments>http://voxcharta.org/2012/05/07/free-free-emission-and-radio-recombination-lines-from-photoevaporating-disks/#comments</comments>
		<pubDate>Tue, 08 May 2012 01:04:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[centimeter wavelength]]></category>
		<category><![CDATA[central star]]></category>
		<category><![CDATA[continuum emission]]></category>
		<category><![CDATA[dispersal]]></category>
		<category><![CDATA[electron density]]></category>
		<category><![CDATA[energy photons]]></category>
		<category><![CDATA[flow rate]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[inference]]></category>
		<category><![CDATA[infrared observation]]></category>
		<category><![CDATA[instrumentation]]></category>
		<category><![CDATA[intensity]]></category>
		<category><![CDATA[mass flow rate]]></category>
		<category><![CDATA[millimeter]]></category>
		<category><![CDATA[profile]]></category>
		<category><![CDATA[radio recombination lines]]></category>
		<category><![CDATA[Sun]]></category>
		<category><![CDATA[vla observation]]></category>
		<category><![CDATA[wind parameters]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/free-free-emission-and-radio-recombination-lines-from-photoevaporating-disks/</guid>
		<description><![CDATA[Recent infrared observations have demonstrated that photoevaporation driven by high-energy photons from the central star contributes to the dispersal of protoplanetary disks. Here, we show that photoevaporative winds should produce a detectable free-free continuum emission given the range of stellar ionizing photons and X-ray luminosities inferred for young sun-like stars. We point out that VLA [...]]]></description>
			<content:encoded><![CDATA[<p>Recent infrared observations have demonstrated that photoevaporation driven by high-energy photons from the central star contributes to the dispersal of protoplanetary disks. Here, we show that photoevaporative winds should produce a detectable free-free continuum emission given the range of stellar ionizing photons and X-ray luminosities inferred for young sun-like stars. We point out that VLA observations of the nearby disk around TWHya might have already detected this emission at centimeter wavelengths and calculate the wind electron density and mass flow rate. We also estimate the intensities of H radio recombination lines tracing the wind and discuss which ones could be detected with current instrumentation. The detection and profiles of these recombination lines would unambiguously prove our inference of free-free emission from photoevaporating disks like TWHya. In addition, radio/millimeter data can help constraining wind parameters such as temperature and electron density that are fundamental in measuring mass flow rates.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/free-free-emission-and-radio-recombination-lines-from-photoevaporating-disks/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Surface flux evolution constraints for flux transport dynamos</title>
		<link>http://voxcharta.org/2012/05/07/surface-flux-evolution-constraints-for-flux-transport-dynamos/</link>
		<comments>http://voxcharta.org/2012/05/07/surface-flux-evolution-constraints-for-flux-transport-dynamos/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:58:47 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[boundary condition]]></category>
		<category><![CDATA[dynamo]]></category>
		<category><![CDATA[evolution of the sun]]></category>
		<category><![CDATA[ftd]]></category>
		<category><![CDATA[gradient]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetic flux]]></category>
		<category><![CDATA[radial transport]]></category>
		<category><![CDATA[reynolds number]]></category>
		<category><![CDATA[solar magnetic field]]></category>
		<category><![CDATA[solar surface]]></category>
		<category><![CDATA[surface boundary layer]]></category>
		<category><![CDATA[surface evolution]]></category>
		<category><![CDATA[surface flux]]></category>
		<category><![CDATA[surface properties]]></category>
		<category><![CDATA[upper boundary]]></category>
		<category><![CDATA[velocities]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/surface-flux-evolution-constraints-for-flux-transport-dynamos/</guid>
		<description><![CDATA[The surface flux transport (SFT) model of solar magnetic fields involves empirically well-constrained velocity and magnetic fields. The basic evolution of the Sun&#8217;s large-scale surface magnetic field is well described by this model. The azimuthally averaged evolution of the SFT model can be compared to the surface evolution of the flux transport dynamo (FTD), and [...]]]></description>
			<content:encoded><![CDATA[<p>The surface flux transport (SFT) model of solar magnetic fields involves empirically well-constrained velocity and magnetic fields. The basic evolution of the Sun&#8217;s large-scale surface magnetic field is well described by this model. The azimuthally averaged evolution of the SFT model can be compared to the surface evolution of the flux transport dynamo (FTD), and the evolution of the SFT model can be used to constrain several near-surface properties of the FTD model.   We compared the results of the FTD model with different upper boundary conditions and diffusivity profiles against the results of the SFT model. Among the ingredients of the FTD model, downward pumping of magnetic flux, related to a positive diffusivity gradient, has a significant effect in slowing down the diffusive radial transport of magnetic flux through the solar surface. Provided the pumping was strong enough to give rise to a downflow of a magnetic Reynolds number of 5 in the near-surface boundary layer, the FTD using a vertical boundary condition matches the SFT model based on the average velocities above the boundary layer. The FTD model with a potential field were unable to match the SFT results.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/surface-flux-evolution-constraints-for-flux-transport-dynamos/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Period-Luminosity Relation of Red Supergiant Stars in the Small Magellanic Cloud</title>
		<link>http://voxcharta.org/2012/05/07/the-period-luminosity-relation-of-red-supergiant-stars-in-the-small-magellanic-cloud/</link>
		<comments>http://voxcharta.org/2012/05/07/the-period-luminosity-relation-of-red-supergiant-stars-in-the-small-magellanic-cloud/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:52:14 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[2mass]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[infrared band]]></category>
		<category><![CDATA[irac]]></category>
		<category><![CDATA[lmc]]></category>
		<category><![CDATA[lsp]]></category>
		<category><![CDATA[mip]]></category>
		<category><![CDATA[photometry]]></category>
		<category><![CDATA[pulsation]]></category>
		<category><![CDATA[short period]]></category>
		<category><![CDATA[small magellanic cloud]]></category>
		<category><![CDATA[smc]]></category>
		<category><![CDATA[Spitzer]]></category>
		<category><![CDATA[supergiant star]]></category>
		<category><![CDATA[theoretical calculation]]></category>
		<category><![CDATA[variables]]></category>
		<category><![CDATA[variation 15]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/the-period-luminosity-relation-of-red-supergiant-stars-in-the-small-magellanic-cloud/</guid>
		<description><![CDATA[The characteristics of light variation of RSGs in SMC are analyzed based on the nearly 8-10 year long data collected by the ASAS and MACHO projects. The identified 126 RSGs are classified into five categories accordingly: 20 with poor photometry, 55 with no reliable period, 6 with semi-regular variation, 15 with Long Secondary Period (LSP) [...]]]></description>
			<content:encoded><![CDATA[<p>The characteristics of light variation of RSGs in SMC are analyzed based on the nearly 8-10 year long data collected by the ASAS and MACHO projects. The identified 126 RSGs are classified into five categories accordingly: 20 with poor photometry, 55 with no reliable period, 6 with semi-regular variation, 15 with Long Secondary Period (LSP) and distinguishable short period and 30 with only LSP. For the semi-regular variables and the LSP variables with distinguishable short period, the Ks band period-luminosity (P-L) relation is analyzed and compared with that of the Galaxy, LMC and M33. It is found that the RSGs in these galaxies obey similar P-L relation except the Galaxy. In addition, the P-L relations in the infrared bands, namely the 2MASS JHKs, Spitzer/IRAC and Spitzer/MIPS 24 {\mu}m bands, are derived with high reliability. The best P-L relation occurs in the Spitzer/IRAC [3.6] and [4.5] bands. Based on the comparison with the theoretical calculation of the P-L relation, the mode of pulsation of RSGs in SMC is suggested to be the first overtone radial mode.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/the-period-luminosity-relation-of-red-supergiant-stars-in-the-small-magellanic-cloud/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Prominence-cavity regions observed using SWAP 174A filtergrams and simultaneous eclipse flash spectra</title>
		<link>http://voxcharta.org/2012/05/07/prominence-cavity-regions-observed-using-swap-174a-filtergrams-and-simultaneous-eclipse-flash-spectra/</link>
		<comments>http://voxcharta.org/2012/05/07/prominence-cavity-regions-observed-using-swap-174a-filtergrams-and-simultaneous-eclipse-flash-spectra/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:50:00 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cavity]]></category>
		<category><![CDATA[continuum]]></category>
		<category><![CDATA[corona]]></category>
		<category><![CDATA[depression]]></category>
		<category><![CDATA[excitation emission lines]]></category>
		<category><![CDATA[flash spectrum]]></category>
		<category><![CDATA[heii]]></category>
		<category><![CDATA[intensity]]></category>
		<category><![CDATA[interval]]></category>
		<category><![CDATA[modulation]]></category>
		<category><![CDATA[paschen]]></category>
		<category><![CDATA[photometric measurements]]></category>
		<category><![CDATA[plasma density]]></category>
		<category><![CDATA[prominence]]></category>
		<category><![CDATA[scales]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[swap images]]></category>
		<category><![CDATA[total eclipse]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/prominence-cavity-regions-observed-using-swap-174a-filtergrams-and-simultaneous-eclipse-flash-spectra/</guid>
		<description><![CDATA[Images from the SWAP (Proba 2 mission) taken at 174A in the Fe IX/X lines are compared to simultaneous slitless flash spectra taken during the last solar total eclipse of July, 11th 2010. Many faint low excitation emission lines together with the HeI and HeII Paschen Alpha chromospheric lines are recorded on eclipse spectra where [...]]]></description>
			<content:encoded><![CDATA[<p>Images from the SWAP (Proba 2 mission) taken at 174A in the Fe IX/X lines are compared to simultaneous slitless flash spectra taken during the last solar total eclipse of July, 11th 2010. Many faint low excitation emission lines together with the HeI and HeII Paschen Alpha chromospheric lines are recorded on eclipse spectra where regions of limb prominences are obtained with space-borne imagers. We consider a deep flash spectrum obtained by summing 80 individual spectra to show the intensity modulations of the continuum. Intensity depressions are observed around the prominences in both eclipse and SWAP images. The prominence cavities are interpreted as a relative depression of plasma density, produced inside the corona surrounding the prominences. Photometric measurements are shown at different scales and different, spectrally narrow, intervals for both the prominences and the coronal background.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/prominence-cavity-regions-observed-using-swap-174a-filtergrams-and-simultaneous-eclipse-flash-spectra/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Thermohaline instabilities inside stars: a synthetic study including external turbulence and radiative levitation</title>
		<link>http://voxcharta.org/2012/05/07/thermohaline-instabilities-inside-stars-a-synthetic-study-including-external-turbulence-and-radiative-levitation/</link>
		<comments>http://voxcharta.org/2012/05/07/thermohaline-instabilities-inside-stars-a-synthetic-study-including-external-turbulence-and-radiative-levitation/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:49:29 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accumulation]]></category>
		<category><![CDATA[atomic diffusion]]></category>
		<category><![CDATA[boussinesq equations]]></category>
		<category><![CDATA[computations]]></category>
		<category><![CDATA[consequence]]></category>
		<category><![CDATA[convection]]></category>
		<category><![CDATA[element]]></category>
		<category><![CDATA[expression]]></category>
		<category><![CDATA[gradient]]></category>
		<category><![CDATA[incompressible fluid]]></category>
		<category><![CDATA[instabilities]]></category>
		<category><![CDATA[levitation]]></category>
		<category><![CDATA[linear approximation]]></category>
		<category><![CDATA[mutual interaction]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[radiative accelerations]]></category>
		<category><![CDATA[stellar structure]]></category>
		<category><![CDATA[synthetic study]]></category>
		<category><![CDATA[Turbulence]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/thermohaline-instabilities-inside-stars-a-synthetic-study-including-external-turbulence-and-radiative-levitation/</guid>
		<description><![CDATA[We have derived a new expression for the thermohaline mixing coefficient in stars, including the effects of radiative levitation and external turbulence, by solving Boussinesq equations in a quasi-incompressible fluid with a linear approximation. It is well known that radiative levitation of individual elements can lead to their accumulation in specific stellar layers. In some [...]]]></description>
			<content:encoded><![CDATA[<p>We have derived a new expression for the thermohaline mixing coefficient in stars, including the effects of radiative levitation and external turbulence, by solving Boussinesq equations in a quasi-incompressible fluid with a linear approximation. It is well known that radiative levitation of individual elements can lead to their accumulation in specific stellar layers. In some cases, it can induce important effects on the stellar structure. Here we confirm that this accumulation is moderated by thermohaline convection due to the resulting inverse $\mu$-gradient. The new coefficient that we have derived shows that the effect of radiative accelerations on the thermohaline instability itself is small. This effect must however be checked in all computations. We also confirm that the presence of large horizontal turbulence can reduce or even suppress the thermohaline convection. These results are important as they concern all the cases of heavy element accumulation in stars. The computations of radiative diffusion have to be revisited including thermohaline convection and its consequences. It may be one of the basic reasons for the fact that the observed abundances are always smaller than those predicted by pure atomic diffusion. In any case, these processes have to compete with rotation-induced mixing, but this competition is more complex than previously thought due to their mutual interaction.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/thermohaline-instabilities-inside-stars-a-synthetic-study-including-external-turbulence-and-radiative-levitation/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The complex case of V445 Lyr observed with Kepler: Two Blazhko modulations, a non-radial mode, possible triple mode RR Lyrae pulsation, and more</title>
		<link>http://voxcharta.org/2012/05/07/the-complex-case-of-v445-lyr-observed-with-kepler-two-blazhko-modulations-a-non-radial-mode-possible-triple-mode-rr-lyrae-pulsation-and-more/</link>
		<comments>http://voxcharta.org/2012/05/07/the-complex-case-of-v445-lyr-observed-with-kepler-two-blazhko-modulations-a-non-radial-mode-possible-triple-mode-rr-lyrae-pulsation-and-more/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:48:26 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[dex]]></category>
		<category><![CDATA[extreme case]]></category>
		<category><![CDATA[fourier analysis]]></category>
		<category><![CDATA[frequency range]]></category>
		<category><![CDATA[kepler]]></category>
		<category><![CDATA[lyr]]></category>
		<category><![CDATA[modulation]]></category>
		<category><![CDATA[overtone]]></category>
		<category><![CDATA[period change]]></category>
		<category><![CDATA[precision satellite]]></category>
		<category><![CDATA[pulsation]]></category>
		<category><![CDATA[rich spectrum]]></category>
		<category><![CDATA[rr lyrae stars]]></category>
		<category><![CDATA[satellite data]]></category>
		<category><![CDATA[space mission]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[term period]]></category>
		<category><![CDATA[triple mode]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/the-complex-case-of-v445-lyr-observed-with-kepler-two-blazhko-modulations-a-non-radial-mode-possible-triple-mode-rr-lyrae-pulsation-and-more/</guid>
		<description><![CDATA[Rapid and strong changes in the Blazhko modulation of RR Lyrae stars, as they have recently been detected in high precision satellite data, have become a crucial topic in finding an explanation of the long-standing mystery of the Blazhko effect. We present here an analysis of the most extreme case detected so far, the RRab [...]]]></description>
			<content:encoded><![CDATA[<p>Rapid and strong changes in the Blazhko modulation of RR Lyrae stars, as they have recently been detected in high precision satellite data, have become a crucial topic in finding an explanation of the long-standing mystery of the Blazhko effect. We present here an analysis of the most extreme case detected so far, the RRab star V445 Lyr (KIC 6186029) which was observed with the Kepler space mission. V445 Lyr shows very strong cycle-to-cycle changes in its Blazhko modulation, which are caused both by a secondary long-term modulation period as well as irregular variations. In addition to the complex Blazhko modulation, V445 Lyr also shows a rich spectrum of additional peaks in the frequency range between the fundamental pulsation and the first harmonic. Among those peaks, the second radial overtone could be identified, which, combined with a metallicity estimate of [Fe/H]=-2.0 dex from spectroscopy, allowed to constrain the mass (0.55-0.65 M_sun) and luminosity (40-50 L_sun) of V445 Lyr through theoretical Petersen diagrams. A non-radial mode as well as possibly the first overtone are also excited. Furthermore, V445 Lyr shows signs of the period doubling phenomenon and a long term period change. A detailed Fourier analysis along with a study of the O-C variation of V445 Lyr is presented, and the origin of the additional peaks and possible causes of the changes in the Blazhko modulation are discussed. The results are then put into context with those of the only other star with a variable Blazhko effect for which a long enough set of high precision continuous satellite data has been published so far, the CoRoT star 105288363.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/the-complex-case-of-v445-lyr-observed-with-kepler-two-blazhko-modulations-a-non-radial-mode-possible-triple-mode-rr-lyrae-pulsation-and-more/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Fundamental Parameters of Four Massive Eclipsing Binaries in Westerlund 1</title>
		<link>http://voxcharta.org/2012/05/07/the-fundamental-parameters-of-four-massive-eclipsing-binaries-in-westerlund-1/</link>
		<comments>http://voxcharta.org/2012/05/07/the-fundamental-parameters-of-four-massive-eclipsing-binaries-in-westerlund-1/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:46:56 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accuracy]]></category>
		<category><![CDATA[companion]]></category>
		<category><![CDATA[component stars]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[eclipsing binary]]></category>
		<category><![CDATA[evolutionary model]]></category>
		<category><![CDATA[fundamental parameters]]></category>
		<category><![CDATA[magnetar]]></category>
		<category><![CDATA[mass star]]></category>
		<category><![CDATA[massive cluster]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[progenitor]]></category>
		<category><![CDATA[radial velocity]]></category>
		<category><![CDATA[radii]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[velocity curves]]></category>
		<category><![CDATA[westerlund 1]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/the-fundamental-parameters-of-four-massive-eclipsing-binaries-in-westerlund-1/</guid>
		<description><![CDATA[Only a small number of high mass stars (&#62; 30 Mo) have fundamental parameters measured with high enough accuracy from eclipsing binaries to constrain formation and evolutionary models of massive stars. This work aims to increase this limited sample, by studying the 4 massive eclipsing binary candidates discovered by Bonanos in the young massive cluster [...]]]></description>
			<content:encoded><![CDATA[<p>Only a small number of high mass stars (&gt; 30 Mo) have fundamental parameters measured with high enough accuracy from eclipsing binaries to constrain formation and evolutionary models of massive stars. This work aims to increase this limited sample, by studying the 4 massive eclipsing binary candidates discovered by Bonanos in the young massive cluster Westerlund 1. We present new follow-up echelle spectroscopy of these binaries and models of their light and radial velocity curves. We obtain fundamental parameters (i.e. masses, radii) for the 8 component stars, finding masses that span a range of 10-40 Mo, and contributing accurate fundamental parameters for 1 additional very massive star, the 33 Mo component of W13. WR77o is found to have a ~40 Mo companion, which provides a second dynamical constraint on the mass of the progenitor of the magnetar known in the cluster. We also use W13 to estimate the first, direct, eclipsing binary distance to Westerlund 1 and therefore the magnetar, and find it to be at 4.0 +/- 0.6 kpc. Our results confirm previous evidence for a high mass for the progenitor of the magnetar. In addition, the availability of eclipsing binaries with accurate parameters opens the way for direct, independent, high precision eclipsing binary distance measurements to Westerlund 1.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/the-fundamental-parameters-of-four-massive-eclipsing-binaries-in-westerlund-1/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>DRAFTS: A Deep, Rapid Archival Flare Transient Search in the Galactic Bulge</title>
		<link>http://voxcharta.org/2012/05/07/drafts-a-deep-rapid-archival-flare-transient-search-in-the-galactic-bulge/</link>
		<comments>http://voxcharta.org/2012/05/07/drafts-a-deep-rapid-archival-flare-transient-search-in-the-galactic-bulge/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:40:05 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[25m]]></category>
		<category><![CDATA[acs]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[dataset]]></category>
		<category><![CDATA[dwarf]]></category>
		<category><![CDATA[energy loss]]></category>
		<category><![CDATA[flare energy]]></category>
		<category><![CDATA[flare rate]]></category>
		<category><![CDATA[flare star]]></category>
		<category><![CDATA[galactic bulge]]></category>
		<category><![CDATA[hst]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[modulation]]></category>
		<category><![CDATA[planet search]]></category>
		<category><![CDATA[proper motion]]></category>
		<category><![CDATA[scale variability]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[stellar variability]]></category>
		<category><![CDATA[variable star]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/drafts-a-deep-rapid-archival-flare-transient-search-in-the-galactic-bulge/</guid>
		<description><![CDATA[We utilize the Sagittarius Window Eclipsing Extrasolar Planet Search (SWEEPS) HST/ACS dataset for a Deep Rapid Archival Flare Transient Search (DRAFTS) to constrain the flare rate toward the older stellar population in the Galactic bulge. During 7 days of monitoring 229,293 stars brighter than V=29.5, we find evidence for flaring activity in 105 stars between [...]]]></description>
			<content:encoded><![CDATA[<p>We utilize the Sagittarius Window Eclipsing Extrasolar Planet Search (SWEEPS) HST/ACS dataset for a Deep Rapid Archival Flare Transient Search (DRAFTS) to constrain the flare rate toward the older stellar population in the Galactic bulge. During 7 days of monitoring 229,293 stars brighter than V=29.5, we find evidence for flaring activity in 105 stars between V=20 and V=28. We divided the sample into non-variable stars and variable stars whose light curves contain large-scale variability. The flare rate on variable stars is \sim 700 times that of non-variable stars, with a significant correlation between the amount of underlying stellar variability and peak flare amplitude. The flare energy loss rates are generally higher than those of nearby well-studied single dMe flare stars. The distribution of proper motions is consistent with the flaring stars being at the distance and age of the Galactic bulge. If they are single dwarfs, they span a range of \approx 1.0 &#8211; 0.25M\odot. A majority of the flaring stars exhibit periodic photometric modulations with P &lt;3d. If these are tidally locked magnetically active binary systems, their fraction in the bulge is enhanced by a factor of \sim20 compared to the local value. These stars may be useful for placing constraints on the angular momentum evolution of cool close binary stars. Our results expand the type of stars studied for flares in the optical band, and suggest that future sensitive optical time-domain studies will have to contend with a larger sample of flaring stars than the M dwarf flare stars usually considered.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/drafts-a-deep-rapid-archival-flare-transient-search-in-the-galactic-bulge/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Coupled polar-axial magnetar oscillations [Replacement]</title>
		<link>http://voxcharta.org/2012/05/07/coupled-polar-axial-magnetar-oscillations-replacement/</link>
		<comments>http://voxcharta.org/2012/05/07/coupled-polar-axial-magnetar-oscillations-replacement/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:36:23 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[consequence]]></category>
		<category><![CDATA[continuum]]></category>
		<category><![CDATA[coupling]]></category>
		<category><![CDATA[discrete spectrum]]></category>
		<category><![CDATA[dramatic change]]></category>
		<category><![CDATA[fluid core]]></category>
		<category><![CDATA[magnetar]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[relativistic simulation]]></category>
		<category><![CDATA[resonance]]></category>
		<category><![CDATA[toroidal components]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/coupled-polar-axial-magnetar-oscillations-replacement/</guid>
		<description><![CDATA[We study coupled axial and polar axisymmetric oscillations of a neutron star endowed with a strong magnetic field, having both poloidal and toroidal components. The toroidal component of the magnetic field is driving the coupling between the polar and axial oscillations. The star is composed of a fluid core as well as a solid crust. [...]]]></description>
			<content:encoded><![CDATA[<p>We study coupled axial and polar axisymmetric oscillations of a neutron star endowed with a strong magnetic field, having both poloidal and toroidal components. The toroidal component of the magnetic field is driving the coupling between the polar and axial oscillations. The star is composed of a fluid core as well as a solid crust. Using a two dimensional general relativistic simulation and a magnetic field B = 10^16 G, we study the change in the polar and axial spectrum caused by the coupling. We find that the axial spectrum suffers a dramatic change in its nature, losing its continuum character. In fact, we find that only the &#8216;edges&#8217; of the continua survive, generating a discrete spectrum. As a consequence the crustal frequencies, that in our previous simulation could be absorbed by the continua, if they were embedded inside it, are now long living oscillations. They may lose their energy only in the very special case that they are in resonance with the &#8216;edges&#8217; of the continua.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/coupled-polar-axial-magnetar-oscillations-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>They might be giants: luminosity class, planet frequency, and planet-metallicity relation of the coolest Kepler target stars [Replacement]</title>
		<link>http://voxcharta.org/2012/05/07/they-might-be-giants-luminosity-class-planet-frequency-and-planet-metallicity-relation-of-the-coolest-kepler-target-stars-replacement/</link>
		<comments>http://voxcharta.org/2012/05/07/they-might-be-giants-luminosity-class-planet-frequency-and-planet-metallicity-relation-of-the-coolest-kepler-target-stars-replacement/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:33:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[artifact]]></category>
		<category><![CDATA[class planet]]></category>
		<category><![CDATA[criterion]]></category>
		<category><![CDATA[dwarf star]]></category>
		<category><![CDATA[exoplanet]]></category>
		<category><![CDATA[giant star]]></category>
		<category><![CDATA[kepler]]></category>
		<category><![CDATA[luminosity class]]></category>
		<category><![CDATA[medium resolution]]></category>
		<category><![CDATA[monte carlo simulation]]></category>
		<category><![CDATA[neptune]]></category>
		<category><![CDATA[spectral type]]></category>
		<category><![CDATA[stellar model]]></category>
		<category><![CDATA[stellar parameters]]></category>
		<category><![CDATA[target star]]></category>
		<category><![CDATA[they might be giants]]></category>
		<category><![CDATA[transits]]></category>
		<category><![CDATA[visible spectra]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/they-might-be-giants-luminosity-class-planet-frequency-and-planet-metallicity-relation-of-the-coolest-kepler-target-stars-replacement/</guid>
		<description><![CDATA[We estimate the stellar parameters of late K and early M type Kepler target stars. We obtain medium resolution visible spectra of 382 stars with Kp-J&#62;2 (~K5 and later spectral type). We determine luminosity class by comparing the strength of gravity-sensitive indices (CaH, K I, Ca II, and Na I) to their strength in a [...]]]></description>
			<content:encoded><![CDATA[<p>We estimate the stellar parameters of late K and early M type Kepler target stars. We obtain medium resolution visible spectra of 382 stars with Kp-J&gt;2 (~K5 and later spectral type). We determine luminosity class by comparing the strength of gravity-sensitive indices (CaH, K I, Ca II, and Na I) to their strength in a sample of stars of known luminosity class. We find that giants constitute 96+-% of the bright (Kp14) stars, significantly higher than fractions based on the stellar parameters quoted in the Kepler Input Catalog (KIC). The KIC effective temperatures are systematically (110 +15 -35} K) higher than temperatures we determine from fitting our spectra to PHOENIX stellar models. Through Monte Carlo simulations of the Kepler exoplanet candidate population, we find a planet occurrence of 0.36+-0.08 when giant stars are properly removed, somewhat higher than when a KIC log(g)&gt;4 criterion is used (0.27+-0.05). Lastly, we show that there is no significant difference in g-r color (a probe of metallicity) between late-type Kepler stars with transiting Earth-to-Neptune sized exoplanet candidates and dwarf stars with no detected transits. We show that a previous claimed offset between these two populations is most likely an artifact of including a large number of misidentified giants.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/they-might-be-giants-luminosity-class-planet-frequency-and-planet-metallicity-relation-of-the-coolest-kepler-target-stars-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Merger by Migration at the Final Phase of Common Envelope Evolution [Replacement]</title>
		<link>http://voxcharta.org/2012/05/07/merger-by-migration-at-the-final-phase-of-common-envelope-evolution-replacement/</link>
		<comments>http://voxcharta.org/2012/05/07/merger-by-migration-at-the-final-phase-of-common-envelope-evolution-replacement/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:32:28 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[angular momentum]]></category>
		<category><![CDATA[basic assumption]]></category>
		<category><![CDATA[binary system]]></category>
		<category><![CDATA[companion]]></category>
		<category><![CDATA[convection]]></category>
		<category><![CDATA[envelopes]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[final phase]]></category>
		<category><![CDATA[formalism]]></category>
		<category><![CDATA[giant]]></category>
		<category><![CDATA[gravitational energy]]></category>
		<category><![CDATA[mass ratio]]></category>
		<category><![CDATA[merger]]></category>
		<category><![CDATA[orbital separation]]></category>
		<category><![CDATA[planet migration]]></category>
		<category><![CDATA[vicinity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/merger-by-migration-at-the-final-phase-of-common-envelope-evolution-replacement/</guid>
		<description><![CDATA[I find the common envelope (CE) energy formalism, the CE \alpha-prescription, to be inadequate to predict the final orbital separation of the CE evolution in massive envelopes. I find that when the orbital separation decreases to ~10 times the final orbital separation predicted by the CE \alpha-prescription, the companion has not enough mass in its [...]]]></description>
			<content:encoded><![CDATA[<p>I find the common envelope (CE) energy formalism, the CE \alpha-prescription, to be inadequate to predict the final orbital separation of the CE evolution in massive envelopes. I find that when the orbital separation decreases to ~10 times the final orbital separation predicted by the CE \alpha-prescription, the companion has not enough mass in its vicinity to carry away its angular momentum. The core-secondary binary system must get rid of its angular momentum by interacting with mass further out. The binary system interacts gravitationally with a rapidly-rotating flat envelope, in a situation that resembles planet-migration in protoplanetary disks. The envelope convection of the giant carries energy and angular momentum outward. The basic assumption of the CE \alpha-prescription, that the binary system&#8217;s gravitational energy goes to unbind the envelope, breaks down. Based on that, I claim that merger is a common outcome of the CE evolution of AGB and red super-giants stars with an envelope to secondary mass ratio of (M_env/M_2)&gt;~5. I discuss some other puzzling observations that might be explained by the migration and merger processes.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/merger-by-migration-at-the-final-phase-of-common-envelope-evolution-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Precision Astrometry of the Exoplanet Host Candidate GD 66</title>
		<link>http://voxcharta.org/2012/05/06/precision-astrometry-of-the-exoplanet-host-candidate-gd-66/</link>
		<comments>http://voxcharta.org/2012/05/06/precision-astrometry-of-the-exoplanet-host-candidate-gd-66/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:53:45 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Earth and Planetary]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[arrival time]]></category>
		<category><![CDATA[companion]]></category>
		<category><![CDATA[giant planet]]></category>
		<category><![CDATA[guidance sensor]]></category>
		<category><![CDATA[hubble space telescope]]></category>
		<category><![CDATA[infrared data]]></category>
		<category><![CDATA[main sequence]]></category>
		<category><![CDATA[orbital motion]]></category>
		<category><![CDATA[planets]]></category>
		<category><![CDATA[precision astrometry]]></category>
		<category><![CDATA[precision measurement]]></category>
		<category><![CDATA[profound implications]]></category>
		<category><![CDATA[regeneration]]></category>
		<category><![CDATA[stellar evolution]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[stellar pulsation]]></category>
		<category><![CDATA[stellar remnant]]></category>
		<category><![CDATA[u s naval observatory]]></category>
		<category><![CDATA[variation]]></category>
		<category><![CDATA[white dwarf]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/precision-astrometry-of-the-exoplanet-host-candidate-gd-66/</guid>
		<description><![CDATA[The potential existence of a giant planet orbiting within a few AU of a stellar remnant has profound implications for both the survival and possible regeneration of planets during post-main sequence stellar evolution. This paper reports Hubble Space Telescope Fine Guidance Sensor and U.S. Naval Observatory relative astrometry of GD 66, a white dwarf thought [...]]]></description>
			<content:encoded><![CDATA[<p>The potential existence of a giant planet orbiting within a few AU of a stellar remnant has profound implications for both the survival and possible regeneration of planets during post-main sequence stellar evolution. This paper reports Hubble Space Telescope Fine Guidance Sensor and U.S. Naval Observatory relative astrometry of GD 66, a white dwarf thought to harbor a giant planet between 2 and 3 AU based on stellar pulsation arrival times. Combined with existing infrared data, the precision measurements here rule out all stellar-mass and brown dwarf companions, implying that only a planet remains plausible, if orbital motion is indeed the cause of the variations in pulsation timing.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/precision-astrometry-of-the-exoplanet-host-candidate-gd-66/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A Physical Model for SN 2001ay, a normal, bright, extremely slowly declining Type Ia supernova</title>
		<link>http://voxcharta.org/2012/05/06/a-physical-model-for-sn-2001ay-a-normal-bright-extremely-slowly-declining-type-ia-supernova/</link>
		<comments>http://voxcharta.org/2012/05/06/a-physical-model-for-sn-2001ay-a-normal-bright-extremely-slowly-declining-type-ia-supernova/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:51:20 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[chandrasekhar mass]]></category>
		<category><![CDATA[decay energy]]></category>
		<category><![CDATA[detonation]]></category>
		<category><![CDATA[energy generation]]></category>
		<category><![CDATA[high velocity]]></category>
		<category><![CDATA[instantaneous rate]]></category>
		<category><![CDATA[light curve]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[m15]]></category>
		<category><![CDATA[opacity]]></category>
		<category><![CDATA[peak luminosity]]></category>
		<category><![CDATA[peculiar type]]></category>
		<category><![CDATA[peculiarity]]></category>
		<category><![CDATA[physical model]]></category>
		<category><![CDATA[slow decline]]></category>
		<category><![CDATA[sne ia]]></category>
		<category><![CDATA[spectral feature]]></category>
		<category><![CDATA[stellar evolution]]></category>
		<category><![CDATA[temperature dependence]]></category>
		<category><![CDATA[white dwarf]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/a-physical-model-for-sn-2001ay-a-normal-bright-extremely-slowly-declining-type-ia-supernova/</guid>
		<description><![CDATA[We present a study of the peculiar Type Ia supernova 2001ay (SN 2001ay). The defining features of its peculiarity are: high velocity, broad lines, and a fast rising light curve, combined with the slowest known rate of decline. It is one magnitude dimmer than would be predicted from its observed value of Delta-m15, and shows [...]]]></description>
			<content:encoded><![CDATA[<p>We present a study of the peculiar Type Ia supernova 2001ay (SN 2001ay). The defining features of its peculiarity are: high velocity, broad lines, and a fast rising light curve, combined with the slowest known rate of decline. It is one magnitude dimmer than would be predicted from its observed value of Delta-m15, and shows broad spectral features. We base our analysis on detailed calculations for the explosion, light curves, and spectra. We demonstrate that consistency is key for both validating the models and probing the underlying physics. We show that this SN can be understood within the physics underlying the Delta-m15 relation, and in the framework of pulsating delayed detonation models originating from a Chandrasekhar mass, white dwarf, but with a progenitor core composed of 80% carbon. We suggest a possible scenario for stellar evolution which leads to such a progenitor. We show that the unusual light curve decline can be understood with the same physics as has been used to understand the Delta-m15 relation for normal SNe Ia. The decline relation can be explained by a combination of the temperature dependence of the opacity and excess or deficit of the peak luminosity, alpha, measured relative to the instantaneous rate of radiative decay energy generation. What differentiates SN 2001ay from normal SNe Ia is a higher explosion energy which leads to a shift of the Ni56 distribution towards higher velocity and alpha &lt; 1. This result is responsible for the fast rise and slow decline. We define a class of SN 2001ay-like SNe Ia, which will show an anti-Phillips relation.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/a-physical-model-for-sn-2001ay-a-normal-bright-extremely-slowly-declining-type-ia-supernova/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Discovery of Two Very Wide Binaries with Ultracool Companions and a New Brown Dwarf at the L/T Transition</title>
		<link>http://voxcharta.org/2012/05/06/discovery-of-two-very-wide-binaries-with-ultracool-companions-and-a-new-brown-dwarf-at-the-lt-transition/</link>
		<comments>http://voxcharta.org/2012/05/06/discovery-of-two-very-wide-binaries-with-ultracool-companions-and-a-new-brown-dwarf-at-the-lt-transition/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:50:22 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[2mass]]></category>
		<category><![CDATA[angular separation]]></category>
		<category><![CDATA[binaries]]></category>
		<category><![CDATA[brown dwarf]]></category>
		<category><![CDATA[catalog]]></category>
		<category><![CDATA[companion]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[infrared spectra]]></category>
		<category><![CDATA[infrared spectrum]]></category>
		<category><![CDATA[infrared survey]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[micron]]></category>
		<category><![CDATA[optical spectrum]]></category>
		<category><![CDATA[pair]]></category>
		<category><![CDATA[proper motion]]></category>
		<category><![CDATA[sky survey]]></category>
		<category><![CDATA[spectral type]]></category>
		<category><![CDATA[transition]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/discovery-of-two-very-wide-binaries-with-ultracool-companions-and-a-new-brown-dwarf-at-the-lt-transition/</guid>
		<description><![CDATA[We present the discovery and spectroscopic follow-up of a nearby late-type L dwarf (2M0614+3950), and two extremely wide very-low-mass binary systems (2M0525-7425AB and 2M1348-1344AB), resulting from our search for common proper motion pairs containing ultracool components in the Two Micron All Sky Survey (2MASS) and the Wide-field Infrared Survey Explorer (WISE) catalogs. The near-infrared spectrum [...]]]></description>
			<content:encoded><![CDATA[<p>We present the discovery and spectroscopic follow-up of a nearby late-type L dwarf (2M0614+3950), and two extremely wide very-low-mass binary systems (2M0525-7425AB and 2M1348-1344AB), resulting from our search for common proper motion pairs containing ultracool components in the Two Micron All Sky Survey (2MASS) and the Wide-field Infrared Survey Explorer (WISE) catalogs. The near-infrared spectrum of 2M0614+3950 indicates a spectral type L9 \pm 1 object residing at a distance of 26.1 \pm 1.3 pc. The optical spectrum of the 2M0525-7425 primary reveals an M3.0 \pm 0.5 dwarf, accompanied by a secondary previously classified as L2. The system has an angular separation of ~44&#8243;, equivalent to ~2000 AU at the 45.7 \pm 2.5 pc distance. Using optical and infrared spectra, respectively, we classify the components of 2M1348-1344AB as M4.5 \pm 0.5 and T6 \pm 1. The angular separation of ~68&#8243; is equivalent to ~1300 AU at the distance of 19.2 \pm 0.9 pc. 2M1348-1344AB is one of only five very wide (separation &gt; 1000 AU) systems containing late T dwarfs known to date.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/discovery-of-two-very-wide-binaries-with-ultracool-companions-and-a-new-brown-dwarf-at-the-lt-transition/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Data Analysis of Gravitational Waves Signals from Millisecond Pulsars [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/06/data-analysis-of-gravitational-waves-signals-from-millisecond-pulsars-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/06/data-analysis-of-gravitational-waves-signals-from-millisecond-pulsars-cross-listing/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:49:20 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[47 tucanae]]></category>
		<category><![CDATA[allegro]]></category>
		<category><![CDATA[doppler]]></category>
		<category><![CDATA[estimates]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[millisecond pulsar]]></category>
		<category><![CDATA[power spectrum]]></category>
		<category><![CDATA[signal]]></category>
		<category><![CDATA[variation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/data-analysis-of-gravitational-waves-signals-from-millisecond-pulsars-cross-listing/</guid>
		<description><![CDATA[The present work is devoted to the detection of monochromatic gravitational waves signals from pulsars using the ALLEGRO&#8217;s data detector. In this work we will present the region (in frequency) of millisecond pulsars of the 47 Tucanae (NGC 104) in the band of detector. According with this result was possible to analyse the frequency of [...]]]></description>
			<content:encoded><![CDATA[<p>The present work is devoted to the detection of monochromatic gravitational waves signals from pulsars using the ALLEGRO&#8217;s data detector. In this work we will present the region (in frequency) of millisecond pulsars of the 47 Tucanae (NGC 104) in the band of detector. According with this result was possible to analyse the frequency of the pulsar J1748-2446L and J1342+2822c, searching annual Doppler variations using power spectrum estimates for the year 1999. We tested this method injecting a simulated signal in real data and we were able to detect it.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/data-analysis-of-gravitational-waves-signals-from-millisecond-pulsars-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Pure Neutron Matter Constraints on the Relativistic Mean-Field and Skyrme-Hartree-Fock Models [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/06/pure-neutron-matter-constraints-on-the-relativistic-mean-field-and-skyrme-hartree-fock-models-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/06/pure-neutron-matter-constraints-on-the-relativistic-mean-field-and-skyrme-hartree-fock-models-cross-listing/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:47:55 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[ab initio]]></category>
		<category><![CDATA[binding energy]]></category>
		<category><![CDATA[confidence ellipse]]></category>
		<category><![CDATA[curvature]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[density functionals]]></category>
		<category><![CDATA[emph]]></category>
		<category><![CDATA[energy density]]></category>
		<category><![CDATA[equation of state]]></category>
		<category><![CDATA[initio calculations]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[nuclear energy]]></category>
		<category><![CDATA[nuclear matter]]></category>
		<category><![CDATA[nuclei]]></category>
		<category><![CDATA[radii]]></category>
		<category><![CDATA[rmf]]></category>
		<category><![CDATA[saturation properties]]></category>
		<category><![CDATA[slope parameter]]></category>
		<category><![CDATA[thicknesses]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/pure-neutron-matter-constraints-on-the-relativistic-mean-field-and-skyrme-hartree-fock-models-cross-listing/</guid>
		<description><![CDATA[Using constraints on the pure neutron matter (PNM) equation of state (EoS) from recent \emph{ab initio} calculations, we present a general optimization of the pure isovector parameters of the popular relativistic mean-field (RMF) and Skyrme-Hartree-Fock (SHF) nuclear energy-density functionals (EDFs) while maintaining the broad quality of the predictions for binding energies and charge radii of [...]]]></description>
			<content:encoded><![CDATA[<p>Using constraints on the pure neutron matter (PNM) equation of state (EoS) from recent \emph{ab initio} calculations, we present a general optimization of the pure isovector parameters of the popular relativistic mean-field (RMF) and Skyrme-Hartree-Fock (SHF) nuclear energy-density functionals (EDFs) while maintaining the broad quality of the predictions for binding energies and charge radii of nuclei. Such optimization leads to broadly consistent and tight predictions of the symmetry energy $J$ and its slope parameter $L$ at saturation density with associated joint 1$\sigma$ confidence ellipses in the $J-L$ plane. We demonstrate that given this optimization, the resulting neutron skin thicknesses are consistent with the experimental data so far, but clear model dependence shows up in (a) the slope of the correlation between $J$ and $L$ from the confidence ellipse, (b) the curvature parameter of the symmetry energy $K_{\rm sym}$, (c) the symmetry energy at supra-saturation densities, and (d) the neutron star radius. Notably, the RMF and SHF models are shown to be only marginally consistent at best with constraints on the isospin-dependent part of the incompressibility of neutron-rich nuclear matter $K_{\tau}$, and that the model dependence can lead to about 1 km difference of the neutron star radius given the same values of $J$, $L$ and symmetric nuclear matter (SNM) saturation properties.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/pure-neutron-matter-constraints-on-the-relativistic-mean-field-and-skyrme-hartree-fock-models-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Propagating Disturbances in Coronal Loops: A Detailed Analysis of Propagation Speeds</title>
		<link>http://voxcharta.org/2012/05/06/propagating-disturbances-in-coronal-loops-a-detailed-analysis-of-propagation-speeds/</link>
		<comments>http://voxcharta.org/2012/05/06/propagating-disturbances-in-coronal-loops-a-detailed-analysis-of-propagation-speeds/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:46:28 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[aia]]></category>
		<category><![CDATA[asymmetry]]></category>
		<category><![CDATA[coronal]]></category>
		<category><![CDATA[doppler velocity]]></category>
		<category><![CDATA[intensity]]></category>
		<category><![CDATA[observatory]]></category>
		<category><![CDATA[outer solar atmosphere]]></category>
		<category><![CDATA[periodic disturbances]]></category>
		<category><![CDATA[propagation]]></category>
		<category><![CDATA[regions of the sun]]></category>
		<category><![CDATA[schrijver]]></category>
		<category><![CDATA[sunspot]]></category>
		<category><![CDATA[sunspot region]]></category>
		<category><![CDATA[temperature dependence]]></category>
		<category><![CDATA[velocities]]></category>
		<category><![CDATA[wave]]></category>
		<category><![CDATA[wavelength]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/propagating-disturbances-in-coronal-loops-a-detailed-analysis-of-propagation-speeds/</guid>
		<description><![CDATA[Quasi-periodic disturbances have been observed in the outer solar atmosphere for many years now. Although first interpreted as upflows (Schrijver et al. (1999)), they have been widely regarded as slow magnetoacoustic waves, due to observed velocities and periods. However, recent observations have questioned this interpretation, as periodic disturbances in Doppler velocity, line width and profile [...]]]></description>
			<content:encoded><![CDATA[<p>Quasi-periodic disturbances have been observed in the outer solar atmosphere for many years now. Although first interpreted as upflows (Schrijver et al. (1999)), they have been widely regarded as slow magnetoacoustic waves, due to observed velocities and periods. However, recent observations have questioned this interpretation, as periodic disturbances in Doppler velocity, line width and profile asymmetry were found to be in phase with the intensity oscillations (De Pontieu et al. (2010),Tian1 et al. (2011))}, suggesting the disturbances could be quasi-periodic upflows. Here we conduct a detailed analysis of the velocities of these disturbances across several wavelengths using the Atmospheric Imaging Assembly (AIA) on board the Solar Dynamics Observatory (SDO). We analysed 41 examples, including both sunspot and non sunspot regions of the Sun. We found that the velocities of propagating disturbances (PDs) located at sunspots are more likely to be temperature dependent, whereas the velocities of PDs at non sunspot locations do not show a clear temperature dependence. We also considered on what scale the underlying driver is affecting the properties of the PDs. Finally, we found that removing the contribution due to the cooler ions in the 193 A wavelength suggests that a substantial part of the 193 emission of sunspot PDs can be contributed to the cool component of 193\AA.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/propagating-disturbances-in-coronal-loops-a-detailed-analysis-of-propagation-speeds/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Thomas Hinsley Astbury: from an English market town schoolroom to the internal constitution of the stars [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/06/thomas-hinsley-astbury-from-an-english-market-town-schoolroom-to-the-internal-constitution-of-the-stars-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/06/thomas-hinsley-astbury-from-an-english-market-town-schoolroom-to-the-internal-constitution-of-the-stars-cross-listing/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:46:11 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[amateur astronomer]]></category>
		<category><![CDATA[arthur eddington]]></category>
		<category><![CDATA[astbury]]></category>
		<category><![CDATA[cepheid]]></category>
		<category><![CDATA[constitution]]></category>
		<category><![CDATA[english market town]]></category>
		<category><![CDATA[first discovery]]></category>
		<category><![CDATA[frank dyson]]></category>
		<category><![CDATA[headmaster]]></category>
		<category><![CDATA[herbert hall]]></category>
		<category><![CDATA[hinsley]]></category>
		<category><![CDATA[meteor]]></category>
		<category><![CDATA[professional astronomers]]></category>
		<category><![CDATA[schoolroom]]></category>
		<category><![CDATA[town of wallingford]]></category>
		<category><![CDATA[variable star]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/thomas-hinsley-astbury-from-an-english-market-town-schoolroom-to-the-internal-constitution-of-the-stars-cross-listing/</guid>
		<description><![CDATA[T. H. Astbury (1858-1922) was for many years the much-respected headmaster of a boys&#8217; junior school in the English market town of Wallingford. By night he was a dedicated amateur astronomer who enjoyed observing meteors, variable stars and many other objects. He began to search few new variable stars, his first discovery being the bright [...]]]></description>
			<content:encoded><![CDATA[<p>T. H. Astbury (1858-1922) was for many years the much-respected headmaster of a boys&#8217; junior school in the English market town of Wallingford. By night he was a dedicated amateur astronomer who enjoyed observing meteors, variable stars and many other objects. He began to search few new variable stars, his first discovery being the bright Cepheid variable, RT Aurigae. This, along with his discovery of 4 other variable stars, brought him to attention of some of the most famous professional astronomers of the age, including Herbert Hall Turner, Frank Dyson and Arthur Eddington.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/thomas-hinsley-astbury-from-an-english-market-town-schoolroom-to-the-internal-constitution-of-the-stars-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>New Bright Carbon Stars Found In The DFBS. (Research note, submitted to Astrophysics)</title>
		<link>http://voxcharta.org/2012/05/06/new-bright-carbon-stars-found-in-the-dfbs-research-note-submitted-to-astrophysics/</link>
		<comments>http://voxcharta.org/2012/05/06/new-bright-carbon-stars-found-in-the-dfbs-research-note-submitted-to-astrophysics/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:45:54 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absolute magnitude]]></category>
		<category><![CDATA[accurate knowledge]]></category>
		<category><![CDATA[aras]]></category>
		<category><![CDATA[astrophysics]]></category>
		<category><![CDATA[carbon star]]></category>
		<category><![CDATA[critical requirement]]></category>
		<category><![CDATA[distance]]></category>
		<category><![CDATA[galactic chemical evolution]]></category>
		<category><![CDATA[galactic evolution]]></category>
		<category><![CDATA[giant]]></category>
		<category><![CDATA[image analysis]]></category>
		<category><![CDATA[k band]]></category>
		<category><![CDATA[mass star]]></category>
		<category><![CDATA[medium resolution]]></category>
		<category><![CDATA[resolution spectra]]></category>
		<category><![CDATA[rich nature]]></category>
		<category><![CDATA[scenarios]]></category>
		<category><![CDATA[stellar population]]></category>
		<category><![CDATA[type star]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/new-bright-carbon-stars-found-in-the-dfbs-research-note-submitted-to-astrophysics/</guid>
		<description><![CDATA[Carbon rich stars of Population II, such as CH giants, can provide direct information on the role of low to intermediate mass stars of the Halo in early Galactic evolution. Moreover, accurate knowledge of the CH stellar population is a critical requirement for building up scenarios for early Galactic chemical evolution. The first list of [...]]]></description>
			<content:encoded><![CDATA[<p>Carbon rich stars of Population II, such as CH giants, can provide direct information on the role of low to intermediate mass stars of the Halo in early Galactic evolution. Moreover, accurate knowledge of the CH stellar population is a critical requirement for building up scenarios for early Galactic chemical evolution. The first list of the faint high latitude C stars (FHLCs), found in the Digitized First Byurakan Survey {<a href="http://byurakan.phys.uniroma1.it">http://byurakan.phys.uniroma1.it</a> and <a href="http://www.aras.am/Dfbs/dfbs.html">http://www.aras.am/Dfbs/dfbs.html</a>} (DFBS) is given in a paper recently submitted for publication in Astronomy ad Astrophysics. In the present work, we report the recent discovery of two additional CH type stars (not previously catalogued), namely DFBS J075331.98+190344.3 and DFBS J111422.94+091442.7, detected on the DFBS plates with help of the image analysis softwares (FITSView and SAOImage DS9). Medium resolution spectra confirm the C rich nature for both of them. Using infrared color magnitudes relationship, we estimated the distances and K band absolute magnitudes of the new objects.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/new-bright-carbon-stars-found-in-the-dfbs-research-note-submitted-to-astrophysics/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The first confirmed superoutburst of the dwarf nova GALEX J215818.5+241924</title>
		<link>http://voxcharta.org/2012/05/06/the-first-confirmed-superoutburst-of-the-dwarf-nova-galex-j215818-5241924/</link>
		<comments>http://voxcharta.org/2012/05/06/the-first-confirmed-superoutburst-of-the-dwarf-nova-galex-j215818-5241924/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:45:39 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abrupt change]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[dramatic evolution]]></category>
		<category><![CDATA[dwarf nova]]></category>
		<category><![CDATA[dwarf novae]]></category>
		<category><![CDATA[epsilon]]></category>
		<category><![CDATA[galex]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[maximum brightness]]></category>
		<category><![CDATA[orbital period]]></category>
		<category><![CDATA[outburst]]></category>
		<category><![CDATA[peak amplitude]]></category>
		<category><![CDATA[peak to peak]]></category>
		<category><![CDATA[pegasus]]></category>
		<category><![CDATA[photometry]]></category>
		<category><![CDATA[plateau phase]]></category>
		<category><![CDATA[porb]]></category>
		<category><![CDATA[power spectrum]]></category>
		<category><![CDATA[psh]]></category>
		<category><![CDATA[residuals]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/the-first-confirmed-superoutburst-of-the-dwarf-nova-galex-j215818-5241924/</guid>
		<description><![CDATA[GALEX J215818.5+241924 was initially identified as a possible nova in Pegasus. We report unfiltered photometry of the object which revealed the presence of superhumps, with peak-to-peak amplitude of up to 0.22 magnitudes, diagnostic of it being a member of the SU UMa family of dwarf novae. The outburst amplitude was 4.3 magnitudes and it lasted [...]]]></description>
			<content:encoded><![CDATA[<p>GALEX J215818.5+241924 was initially identified as a possible nova in Pegasus. We report unfiltered photometry of the object which revealed the presence of superhumps, with peak-to-peak amplitude of up to 0.22 magnitudes, diagnostic of it being a member of the SU UMa family of dwarf novae. The outburst amplitude was 4.3 magnitudes and it lasted at least 10 days, with a maximum brightness of magnitude 14.3. We determined the mean superhump period from our first 5 nights of observations as Psh = 0.06728(21) d. However analysis of the O-C residuals showed a dramatic evolution in Psh during the outburst. During the first part of the plateau phase the period increased with dPsh/dt = +2.67(15) \times 10-4. There was then an abrupt change following which the period decreased with dPsh/dt = -2.08(9)\times10-4. We found a signal in the power spectrum of the photometry which we interpret as the orbital signal with Porb = 0.06606(35) d. Thus the superhump period excess was epsilon = 0.020(8), such value being consistent with other SU UMa systems of similar orbital period.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/the-first-confirmed-superoutburst-of-the-dwarf-nova-galex-j215818-5241924/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Surface Alfven waves in solar flux tubes</title>
		<link>http://voxcharta.org/2012/05/06/surface-alfven-waves-in-solar-flux-tubes/</link>
		<comments>http://voxcharta.org/2012/05/06/surface-alfven-waves-in-solar-flux-tubes/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:44:35 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[axisymmetric]]></category>
		<category><![CDATA[continuous variation]]></category>
		<category><![CDATA[contrary]]></category>
		<category><![CDATA[cylinder boundary]]></category>
		<category><![CDATA[density profile]]></category>
		<category><![CDATA[discontinuity]]></category>
		<category><![CDATA[infinite extent]]></category>
		<category><![CDATA[interval]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[mhd waves]]></category>
		<category><![CDATA[overtone]]></category>
		<category><![CDATA[phase velocity]]></category>
		<category><![CDATA[plasma]]></category>
		<category><![CDATA[solar atmosphere]]></category>
		<category><![CDATA[solar flux]]></category>
		<category><![CDATA[sonic waves]]></category>
		<category><![CDATA[uniform density]]></category>
		<category><![CDATA[uniformity]]></category>
		<category><![CDATA[wave mode]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/surface-alfven-waves-in-solar-flux-tubes/</guid>
		<description><![CDATA[Magnetohydrodynamic (MHD) waves are ubiquitous in the solar atmosphere. Alfven waves and magneto-sonic waves are particular classes of MHD waves. These wave modes are clearly different and have pure properties in uniform plasmas of infinite extent only. Due to plasma non-uniformity MHD waves have mixed properties and cannot be classified as pure Alfven or magneto-sonic [...]]]></description>
			<content:encoded><![CDATA[<p>Magnetohydrodynamic (MHD) waves are ubiquitous in the solar atmosphere. Alfven waves and magneto-sonic waves are particular classes of MHD waves. These wave modes are clearly different and have pure properties in uniform plasmas of infinite extent only. Due to plasma non-uniformity MHD waves have mixed properties and cannot be classified as pure Alfven or magneto-sonic waves. However, vorticity is a quantity unequivocally related to Alfven waves as compression is for magneto-sonic waves. Here, we investigate MHD waves superimposed on a one-dimensional non-uniform straight cylinder with constant magnetic field. For a piecewise constant density profile we find that the fundamental radial modes of the non-axisymmetric waves have the same properties as surface Alfven waves at a true discontinuity in density. Contrary to the classic Alfveen waves in a uniform plasma of infinite extent, vorticity is zero everywhere except at the cylinder boundary. If the discontinuity in density is replaced with a continuous variation of density, vorticity is spread out over the whole interval with non-uniform density. The fundamental radial modes of the non-axisymmetric waves do not need compression to exist unlike the radial overtones. In thin magnetic cylinders the fundamental radial modes of the non-axisymmetric waves with phase velocities between the internal and the external Alfven velocities can be considered as surface Alfven waves. On the contrary, the radial overtones can be related to fast-like magneto-sonic modes.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>On Simulating Type Ia Supernovae</title>
		<link>http://voxcharta.org/2012/05/06/on-simulating-type-ia-supernovae/</link>
		<comments>http://voxcharta.org/2012/05/06/on-simulating-type-ia-supernovae/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:43:18 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[architecture]]></category>
		<category><![CDATA[combustion]]></category>
		<category><![CDATA[cosmological studies]]></category>
		<category><![CDATA[flame]]></category>
		<category><![CDATA[host galaxy]]></category>
		<category><![CDATA[leadership class]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[numerical model]]></category>
		<category><![CDATA[paradigm]]></category>
		<category><![CDATA[performance results]]></category>
		<category><![CDATA[physical processes]]></category>
		<category><![CDATA[progenitor]]></category>
		<category><![CDATA[realistic model]]></category>
		<category><![CDATA[scales]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[stellar explosion]]></category>
		<category><![CDATA[systematics]]></category>
		<category><![CDATA[type ia supernovae]]></category>
		<category><![CDATA[white dwarf star]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/on-simulating-type-ia-supernovae/</guid>
		<description><![CDATA[Type Ia supernovae are bright stellar explosions distinguished by standardizable light curves that allow for their use as distance indicators for cosmological studies. Despite their highly successful use in this capacity, the progenitors of these events are incompletely understood. We describe simulating type Ia supernovae in the paradigm of a thermonuclear runaway occurring in a [...]]]></description>
			<content:encoded><![CDATA[<p>Type Ia supernovae are bright stellar explosions distinguished by standardizable light curves that allow for their use as distance indicators for cosmological studies. Despite their highly successful use in this capacity, the progenitors of these events are incompletely understood. We describe simulating type Ia supernovae in the paradigm of a thermonuclear runaway occurring in a massive white dwarf star. We describe the multi-scale physical processes that realistic models must incorporate and the numerical models for these that we employ. In particular, we describe a flame-capturing scheme that addresses the problem of turbulent thermonuclear combustion on unresolved scales. We present the results of our study of the systematics of type Ia supernovae including trends in brightness following from properties of the host galaxy that agree with observations. We also present performance results from simulations on leadership-class architectures.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/on-simulating-type-ia-supernovae/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Primary neutral helium in the heliosphere</title>
		<link>http://voxcharta.org/2012/05/06/primary-neutral-helium-in-the-heliosphere/</link>
		<comments>http://voxcharta.org/2012/05/06/primary-neutral-helium-in-the-heliosphere/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:43:06 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accounting]]></category>
		<category><![CDATA[analytic calculation]]></category>
		<category><![CDATA[distribution function]]></category>
		<category><![CDATA[estimates]]></category>
		<category><![CDATA[helium atom]]></category>
		<category><![CDATA[ibex]]></category>
		<category><![CDATA[inner heliosphere]]></category>
		<category><![CDATA[local interstellar medium]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[neutral helium]]></category>
		<category><![CDATA[neutral particle]]></category>
		<category><![CDATA[oxygen]]></category>
		<category><![CDATA[particle species]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[trajectory]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/primary-neutral-helium-in-the-heliosphere/</guid>
		<description><![CDATA[Two years of neutral measurements by IBEX-Lo have yielded several direct observations of interstellar neutral helium and oxygen during preferred viewing seasons. Besides the interstellar signal, there are indications of the presence of secondary neutral helium and oxygen created in the heliosphere. Detailed modeling of these particle species is necessary to connect the measured fluxes [...]]]></description>
			<content:encoded><![CDATA[<p>Two years of neutral measurements by IBEX-Lo have yielded several direct observations of interstellar neutral helium and oxygen during preferred viewing seasons. Besides the interstellar signal, there are indications of the presence of secondary neutral helium and oxygen created in the heliosphere. Detailed modeling of these particle species is necessary to connect the measured fluxes to the pristine local interstellar medium while accounting for loss and production of neutral particles during their path through the heliosphere. In this contribution, global heliosphere models are coupled to analytic calculations of neutral trajectories to obtain detailed estimates of the neutral distribution function of primary interstellar helium atoms in the heliosphere, in particular in the inner heliosphere.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/primary-neutral-helium-in-the-heliosphere/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Spectral Typing of Late Type Stellar Companions to Young Stars from Low Dispersion Near-Infrared Integral Field Unit Data</title>
		<link>http://voxcharta.org/2012/05/06/spectral-typing-of-late-type-stellar-companions-to-young-stars-from-low-dispersion-near-infrared-integral-field-unit-data/</link>
		<comments>http://voxcharta.org/2012/05/06/spectral-typing-of-late-type-stellar-companions-to-young-stars-from-low-dispersion-near-infrared-integral-field-unit-data/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:41:11 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astrometry]]></category>
		<category><![CDATA[astronomical results]]></category>
		<category><![CDATA[coronagraph]]></category>
		<category><![CDATA[dispersion]]></category>
		<category><![CDATA[epochs]]></category>
		<category><![CDATA[extraction processes]]></category>
		<category><![CDATA[infrared spectra]]></category>
		<category><![CDATA[integral field]]></category>
		<category><![CDATA[model atmosphere]]></category>
		<category><![CDATA[multiple systems]]></category>
		<category><![CDATA[phoenix model]]></category>
		<category><![CDATA[solar type stars]]></category>
		<category><![CDATA[spectral extraction]]></category>
		<category><![CDATA[spectral library]]></category>
		<category><![CDATA[spectral type]]></category>
		<category><![CDATA[stellar companion]]></category>
		<category><![CDATA[surface gravity]]></category>
		<category><![CDATA[synthetic spectra]]></category>
		<category><![CDATA[young stars]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/spectral-typing-of-late-type-stellar-companions-to-young-stars-from-low-dispersion-near-infrared-integral-field-unit-data/</guid>
		<description><![CDATA[We used the Project 1640 near-infrared coronagraph and integral field spectrograph to observe 19 young solar type stars. Five of these stars are known binary stars and we detected the late-type secondaries and were able to measure their JH spectra with a resolution of R\sim30. The reduced, extracted, and calibrated spectra were compared to template [...]]]></description>
			<content:encoded><![CDATA[<p>We used the Project 1640 near-infrared coronagraph and integral field spectrograph to observe 19 young solar type stars. Five of these stars are known binary stars and we detected the late-type secondaries and were able to measure their JH spectra with a resolution of R\sim30. The reduced, extracted, and calibrated spectra were compared to template spectra from the IRTF spectral library. With this comparison we test the accuracy and consistency of spectral type determination with the low-resolution near-infrared spectra from P1640. Additionally, we determine effective temperature and surface gravity of the companions by fitting synthetic spectra calculated with the PHOENIX model atmosphere code. We also present several new epochs of astrometry of each of the systems. Together these data increase our knowledge and understanding of the stellar make up of these systems. In addition to the astronomical results, the analysis presented helps validate the Project 1640 data reduction and spectral extraction processes and the utility of low-resolution, near-infrared spectra for characterizing late-type companions in multiple systems.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/spectral-typing-of-late-type-stellar-companions-to-young-stars-from-low-dispersion-near-infrared-integral-field-unit-data/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>New SX Phoenicis Variables in the Globular Cluster NGC 4833</title>
		<link>http://voxcharta.org/2012/05/06/new-sx-phoenicis-variables-in-the-globular-cluster-ngc-4833/</link>
		<comments>http://voxcharta.org/2012/05/06/new-sx-phoenicis-variables-in-the-globular-cluster-ngc-4833/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:40:13 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[10x10]]></category>
		<category><![CDATA[algol]]></category>
		<category><![CDATA[astronomy]]></category>
		<category><![CDATA[cerro tololo interamerican]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[image subtraction]]></category>
		<category><![CDATA[images]]></category>
		<category><![CDATA[interamerican observatory]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[meter telescope]]></category>
		<category><![CDATA[period]]></category>
		<category><![CDATA[relative number]]></category>
		<category><![CDATA[rrc]]></category>
		<category><![CDATA[southeastern association]]></category>
		<category><![CDATA[southern globular cluster]]></category>
		<category><![CDATA[ursae majoris]]></category>
		<category><![CDATA[variable star]]></category>
		<category><![CDATA[variables]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/new-sx-phoenicis-variables-in-the-globular-cluster-ngc-4833/</guid>
		<description><![CDATA[We report the discovery of 6 SX Phoenicis stars in the southern globular cluster NGC 4833. Images were obtained from January through June 2011 with the Southeastern Association for Research in Astronomy 0.6 meter telescope located at Cerro Tololo Interamerican Observatory. The image subtraction method of Alard &#38; Lupton (1998)was used to search for variable [...]]]></description>
			<content:encoded><![CDATA[<p>We report the discovery of 6 SX Phoenicis stars in the southern globular cluster NGC 4833. Images were obtained from January through June 2011 with the Southeastern Association for Research in Astronomy 0.6 meter telescope located at Cerro Tololo Interamerican Observatory. The image subtraction method of Alard &amp; Lupton (1998)was used to search for variable stars in the cluster. We confirmed 17 previously cataloged variables by Demers &amp; Wehlau(1977). In addition to the previously known variables we have identified 10 new variables. Of the total number of confirmed variables in our 10&#215;10 arcmin^2 field, we classified 10 RRab variables, with a mean period of 0.69591 days, 7 RRc, with a mean period of 0.39555 days, 2 possible RRe variables with a mean period of 0.30950 days, a W Ursae Majoris contact binary, an Algol-type binary, and the 6 SX Phoenicis stars with a mean period of 0.05847 days. The periods, relative numbers of RRab and RRc variables, and Bailey diagram are indicative of the cluster being of the Oosterhoff type II. We present the phased-light curves, periods of previously known variables and the periods and classifications of the newly discovered variables, and their location on the color-magnitude diagram.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/new-sx-phoenicis-variables-in-the-globular-cluster-ngc-4833/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Thermal signatures of tether-cutting reconnections in pre-eruption coronal flux ropes: hot central voids in coronal cavities</title>
		<link>http://voxcharta.org/2012/05/06/thermal-signatures-of-tether-cutting-reconnections-in-pre-eruption-coronal-flux-ropes-hot-central-voids-in-coronal-cavities/</link>
		<comments>http://voxcharta.org/2012/05/06/thermal-signatures-of-tether-cutting-reconnections-in-pre-eruption-coronal-flux-ropes-hot-central-voids-in-coronal-cavities/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:39:57 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[3d mhd]]></category>
		<category><![CDATA[cavity]]></category>
		<category><![CDATA[central void]]></category>
		<category><![CDATA[critical height]]></category>
		<category><![CDATA[emergence]]></category>
		<category><![CDATA[high density]]></category>
		<category><![CDATA[hot channel]]></category>
		<category><![CDATA[line of sight]]></category>
		<category><![CDATA[low density]]></category>
		<category><![CDATA[magnetic energy]]></category>
		<category><![CDATA[mhd simulation]]></category>
		<category><![CDATA[neutral line]]></category>
		<category><![CDATA[prominence]]></category>
		<category><![CDATA[reconnection]]></category>
		<category><![CDATA[rope]]></category>
		<category><![CDATA[thermal conduction]]></category>
		<category><![CDATA[thermal features]]></category>
		<category><![CDATA[thermal signature]]></category>
		<category><![CDATA[vertical column]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/thermal-signatures-of-tether-cutting-reconnections-in-pre-eruption-coronal-flux-ropes-hot-central-voids-in-coronal-cavities/</guid>
		<description><![CDATA[Using a 3D MHD simulation, we model the quasi-static evolution and the onset of eruption of a coronal flux rope. The simulation begins with a twisted flux rope emerging at the lower boundary and pushing into a pre-existing coronal potential arcade field. At a chosen time the emergence is stopped with the lower boundary taken [...]]]></description>
			<content:encoded><![CDATA[<p>Using a 3D MHD simulation, we model the quasi-static evolution and the onset of eruption of a coronal flux rope. The simulation begins with a twisted flux rope emerging at the lower boundary and pushing into a pre-existing coronal potential arcade field. At a chosen time the emergence is stopped with the lower boundary taken to be rigid. Then the coronal flux rope settles into a quasi-static rise phase with an underlying, central sigmoid-shaped current layer developing. Reconnections in the dissipating current layer during the quasi-static phase effectively add twisted flux to the flux rope and thus allow it to rise quasi-statically, even though the magnetic energy is decreasing as the system relaxes. We examine the thermal features produced by such &#8220;tether-cutting&#8221; reconnections as a result of heating and field aligned thermal conduction. It is found that a central hot, low-density channel containing reconnected, twisted flux threading under the flux rope axis forms on top of the central current layer. When viewed in the line of sight roughly aligned with the hot channel (which is roughly along the neutral line), the central current layer appears as a high-density vertical column with upward extensions as a &#8220;U&#8221; shaped dense shell enclosing a central hot, low-density void. Such thermal features have been observed within coronal prominence cavities. Our MHD simulations suggest that they are the signatures and consequences of the tether-cutting reconnections, and that the central void grows and rises with the reconnections, until the flux rope reaches the critical height for the onset of the torus instability and dynamic eruption ensues.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/thermal-signatures-of-tether-cutting-reconnections-in-pre-eruption-coronal-flux-ropes-hot-central-voids-in-coronal-cavities/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>New Variable Stars in the Globular Cluster NGC 6584</title>
		<link>http://voxcharta.org/2012/05/06/new-variable-stars-in-the-globular-cluster-ngc-6584/</link>
		<comments>http://voxcharta.org/2012/05/06/new-variable-stars-in-the-globular-cluster-ngc-6584/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:39:24 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[10x10]]></category>
		<category><![CDATA[alard]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[eclipsing binary]]></category>
		<category><![CDATA[globular cluster ngc]]></category>
		<category><![CDATA[image subtraction]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[liller]]></category>
		<category><![CDATA[lyrae]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[meter telescope]]></category>
		<category><![CDATA[milli]]></category>
		<category><![CDATA[rrc]]></category>
		<category><![CDATA[rre]]></category>
		<category><![CDATA[southeastern association]]></category>
		<category><![CDATA[southern globular cluster]]></category>
		<category><![CDATA[tololo]]></category>
		<category><![CDATA[v band]]></category>
		<category><![CDATA[variable star]]></category>
		<category><![CDATA[variables]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/new-variable-stars-in-the-globular-cluster-ngc-6584/</guid>
		<description><![CDATA[Using the Southeastern Association for Research in Astronomy 0.6 meter telescope located at Cerro Tololo, we searched for variable stars in the southern globular cluster NGC 6584. We obtained images during 8 nights between 28 May and 6 July of 2011. After processing the images, we used the image subtraction package ISIS developed by Alard [...]]]></description>
			<content:encoded><![CDATA[<p>Using the Southeastern Association for Research in Astronomy 0.6 meter telescope located at Cerro Tololo, we searched for variable stars in the southern globular cluster NGC 6584. We obtained images during 8 nights between 28 May and 6 July of 2011. After processing the images, we used the image subtraction package ISIS developed by Alard (2000)to search for the variable stars. We identified a total of 69 variable stars in our 10&#215;10 arcmin^2 field, including 43 variables cataloged by Millis &amp; Liller (1980) and 26 hereto unknown variables. In total, we classified 46 of the variables as type RRab, with a mean period of 0.56776 days, 15 as type RRc with a mean period of 0.30886 days, perhaps one lower amplitude type RRe, with a period of 0.26482 days, 4 eclipsing binaries, and 3 long period (P &gt; 2 days) variable stars. As many as 15 of the RRab Lyrae stars exhibited the Blazhko Effect. Furthermore, the mean periods of the RR Lyrae types, the exhibited period/amplitude relationship, and the ratio of N_c/(N_ab+N_c) of 0.25 are consistent with an Oosterhoff Type I cluster. Here we present refined periods, V-band light curves, and classifications for each of the 69 variables, as well as a color-magnitude diagram of the cluster.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/new-variable-stars-in-the-globular-cluster-ngc-6584/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Statistical properties of the Disk Counterparts of Type II Spicules from simultaneous observations of RBEs in Ca II 8542 and H{\alpha} [Replacement]</title>
		<link>http://voxcharta.org/2012/05/06/statistical-properties-of-the-disk-counterparts-of-type-ii-spicules-from-simultaneous-observations-of-rbes-in-ca-ii-8542-and-halpha-replacement/</link>
		<comments>http://voxcharta.org/2012/05/06/statistical-properties-of-the-disk-counterparts-of-type-ii-spicules-from-simultaneous-observations-of-rbes-in-ca-ii-8542-and-halpha-replacement/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:32:36 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cadence]]></category>
		<category><![CDATA[continuation]]></category>
		<category><![CDATA[counterpart]]></category>
		<category><![CDATA[crisp]]></category>
		<category><![CDATA[doppler velocity]]></category>
		<category><![CDATA[exponent]]></category>
		<category><![CDATA[motion]]></category>
		<category><![CDATA[order of magnitude]]></category>
		<category><![CDATA[quality time]]></category>
		<category><![CDATA[rbes]]></category>
		<category><![CDATA[simultaneous observations]]></category>
		<category><![CDATA[solar limb]]></category>
		<category><![CDATA[spectral line]]></category>
		<category><![CDATA[spicule]]></category>
		<category><![CDATA[sst]]></category>
		<category><![CDATA[statistical properties]]></category>
		<category><![CDATA[time sequence]]></category>
		<category><![CDATA[transverse motion]]></category>
		<category><![CDATA[velocities]]></category>
		<category><![CDATA[velocity range]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/statistical-properties-of-the-disk-counterparts-of-type-ii-spicules-from-simultaneous-observations-of-rbes-in-ca-ii-8542-and-halpha-replacement/</guid>
		<description><![CDATA[Spicules were recently found to exist as two types when a new class of so-called type II spicules was discovered at the solar limb with Hinode. The type II spicules have been linked with on-disk observations of Rapid Blue-shifted Excursions (RBEs) in the Ha and Ca 8542 lines. Here we analyze observations optimized for the [...]]]></description>
			<content:encoded><![CDATA[<p>Spicules were recently found to exist as two types when a new class of so-called type II spicules was discovered at the solar limb with Hinode. The type II spicules have been linked with on-disk observations of Rapid Blue-shifted Excursions (RBEs) in the Ha and Ca 8542 lines. Here we analyze observations optimized for the detection of RBEs in both Ha and Ca 8542 simultaneously at a high temporal cadence taken with CRISP at the SST. This study used a high-quality time sequence for RBEs at different blue-shifts and employed an automated detection routine to detect a large number of RBEs in order to expand on the statistics of RBEs. We find that the number of detected RBEs is dependent on the Doppler velocity of the images on which the search is performed. Detection of RBEs at lower velocities increases the estimated number of RBEs to the same order of magnitude expected from limb spicules. This shows that RBEs and type II spicules are exponents of the same phenomenon. We provide evidence that Ca 8542 RBEs are connected to Ha RBEs and are located closer to the network regions with the Ha RBEs being the continuation, and show that RBEs have an average lifetime of 83.9 s when observed in both spectral lines with Doppler velocity ranges of 10-25 km/s in Ca 8542 and 30-50 km/s in Ha. In addition, we determine the transverse motion of a much larger sample of RBEs than previous studies and find that like type II spicules, RBEs undergo significant transverse motions, 5-10 km/s. Finally, we find that the intergranular jets discovered in BBSO are a subset of RBEs.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/statistical-properties-of-the-disk-counterparts-of-type-ii-spicules-from-simultaneous-observations-of-rbes-in-ca-ii-8542-and-halpha-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Differential rotation of main-sequence dwarfs: predicting the dependence on surface temperature and rotation rate [Replacement]</title>
		<link>http://voxcharta.org/2012/05/06/differential-rotation-of-main-sequence-dwarfs-predicting-the-dependence-on-surface-temperature-and-rotation-rate-replacement/</link>
		<comments>http://voxcharta.org/2012/05/06/differential-rotation-of-main-sequence-dwarfs-predicting-the-dependence-on-surface-temperature-and-rotation-rate-replacement/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:32:23 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[approximation]]></category>
		<category><![CDATA[boundary layer]]></category>
		<category><![CDATA[convection zone]]></category>
		<category><![CDATA[differential]]></category>
		<category><![CDATA[differential rotation]]></category>
		<category><![CDATA[flow changes]]></category>
		<category><![CDATA[flow increases]]></category>
		<category><![CDATA[input parameter]]></category>
		<category><![CDATA[main sequence]]></category>
		<category><![CDATA[meridional flow]]></category>
		<category><![CDATA[rotation period]]></category>
		<category><![CDATA[rotation rate]]></category>
		<category><![CDATA[rotators]]></category>
		<category><![CDATA[stellar parameters]]></category>
		<category><![CDATA[stellar rotation]]></category>
		<category><![CDATA[surface temperature]]></category>
		<category><![CDATA[theoretical findings]]></category>
		<category><![CDATA[theoretical prediction]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/differential-rotation-of-main-sequence-dwarfs-predicting-the-dependence-on-surface-temperature-and-rotation-rate-replacement/</guid>
		<description><![CDATA[Gyrochronology and recent theoretical findings are used to reduce the number of input parameters of differential rotation models. This eventually leads to a theoretical prediction for the surface differential rotation as a function of only two stellar parameters &#8211; surface temperature and rotation period &#8211; that can be defined observationally. An analytical approximation for this [...]]]></description>
			<content:encoded><![CDATA[<p>Gyrochronology and recent theoretical findings are used to reduce the number of input parameters of differential rotation models. This eventually leads to a theoretical prediction for the surface differential rotation as a function of only two stellar parameters &#8211; surface temperature and rotation period &#8211; that can be defined observationally. An analytical approximation for this function is suggested. The tendency for the differential rotation to increase with temperature is confirmed. The increase is much steeper for late F-stars compared to G- and K-dwarfs. Slow and fast rotation regimes for internal stellar rotation are identified. A star attains its maximum differential rotation at rotation rates intermediate between these two regimes. The amplitude of the meridional flow increases with surface temperature and rotation rate. The structure of the flow changes considerably between cases of slow and fast rotation. The flow in rapid rotators is concentrated in the boundary layers near the top and bottom of the convection zone with very weak circulation in between.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/differential-rotation-of-main-sequence-dwarfs-predicting-the-dependence-on-surface-temperature-and-rotation-rate-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Observational Study Of the Quasi-Periodic Fast Propagating Magnetosonic Waves and the Associated Flare on 2011 May 30 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/06/observational-study-of-the-quasi-periodic-fast-propagating-magnetosonic-waves-and-the-associated-flare-on-2011-may-30-replacement/</link>
		<comments>http://voxcharta.org/2012/05/06/observational-study-of-the-quasi-periodic-fast-propagating-magnetosonic-waves-and-the-associated-flare-on-2011-may-30-replacement/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:31:37 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[concentric circle]]></category>
		<category><![CDATA[corona]]></category>
		<category><![CDATA[coronal loop]]></category>
		<category><![CDATA[dispersion relation]]></category>
		<category><![CDATA[flare light]]></category>
		<category><![CDATA[kernel]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[low frequency]]></category>
		<category><![CDATA[mode oscillations]]></category>
		<category><![CDATA[observational study]]></category>
		<category><![CDATA[observatory]]></category>
		<category><![CDATA[omega]]></category>
		<category><![CDATA[phase speed]]></category>
		<category><![CDATA[photosphere]]></category>
		<category><![CDATA[physical origin]]></category>
		<category><![CDATA[qfp]]></category>
		<category><![CDATA[straight ridge]]></category>
		<category><![CDATA[wave]]></category>
		<category><![CDATA[wave train]]></category>
		<category><![CDATA[wavelet technique]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/observational-study-of-the-quasi-periodic-fast-propagating-magnetosonic-waves-and-the-associated-flare-on-2011-may-30-replacement/</guid>
		<description><![CDATA[On 2011 May 30, quasi-periodic fast propagating (QFP) magnetosonic waves accompanied by a C2.8 flare were directly imaged by the Atomospheric Imaging Assembly instrument on board the Solar Dynamics Observatory. The QFP waves successively emanated from the flare kernel, they propagated along a cluster of open coronal loops with a phase speed of 834 km/s [...]]]></description>
			<content:encoded><![CDATA[<p>On 2011 May 30, quasi-periodic fast propagating (QFP) magnetosonic waves accompanied by a C2.8 flare were directly imaged by the Atomospheric Imaging Assembly instrument on board the Solar Dynamics Observatory. The QFP waves successively emanated from the flare kernel, they propagated along a cluster of open coronal loops with a phase speed of 834 km/s during the flare&#8217;s rising phase, and the multiple arc-shaped wave trains can be fitted with a series of concentric circles. We generate the k-omega diagram of the Fourier power and find a straight ridge that represents the dispersion relation of the waves. Along the ridge, we find a lot of prominent nodes which represent the available frequencies of the QFP waves. On the other hand, the frequencies of the flare are also obtained by analyzing the flare light curves using the wavelet technique. The results indicate that almost all the main frequencies of the flare are consistent with those of the QFP waves. This suggests that the flare and the QFP waves were possibly excited by a common physical origin. On the other hand, a few low frequencies revealed by the k-omega diagram can not be found in the accompanying flare. We propose that these low frequencies were possibly due to the leakage of the pressure-driven p-mode oscillations from the photosphere into the low corona, which should be a noticeable mechanism for driving the QFP waves observed in the corona.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/observational-study-of-the-quasi-periodic-fast-propagating-magnetosonic-waves-and-the-associated-flare-on-2011-may-30-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Imaging the Algol Triple System in H Band with the CHARA Interferometer [Replacement]</title>
		<link>http://voxcharta.org/2012/05/06/imaging-the-algol-triple-system-in-h-band-with-the-chara-interferometer-replacement/</link>
		<comments>http://voxcharta.org/2012/05/06/imaging-the-algol-triple-system-in-h-band-with-the-chara-interferometer-replacement/#comments</comments>
		<pubDate>Mon, 07 May 2012 00:31:06 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[algol]]></category>
		<category><![CDATA[angular size]]></category>
		<category><![CDATA[art image]]></category>
		<category><![CDATA[baseline]]></category>
		<category><![CDATA[chara interferometer]]></category>
		<category><![CDATA[eclipse]]></category>
		<category><![CDATA[epochs]]></category>
		<category><![CDATA[image reconstruction]]></category>
		<category><![CDATA[image sequence]]></category>
		<category><![CDATA[inclination]]></category>
		<category><![CDATA[main sequence]]></category>
		<category><![CDATA[mass ratio]]></category>
		<category><![CDATA[mass transfer]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[orbital element]]></category>
		<category><![CDATA[reconstruction algorithm]]></category>
		<category><![CDATA[roche lobe]]></category>
		<category><![CDATA[stellar pair]]></category>
		<category><![CDATA[telescopes]]></category>
		<category><![CDATA[three star]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/06/imaging-the-algol-triple-system-in-h-band-with-the-chara-interferometer-replacement/</guid>
		<description><![CDATA[Algol (Beta Per) is an extensively studied hierarchical triple system whose inner pair is a prototype semi-detached binary with mass transfer occurring from the sub-giant secondary to the main-sequence primary. We present here the results of our Algol observations made between 2006 and 2010 at the CHARA interferometer with the Michigan Infrared Combiner in the [...]]]></description>
			<content:encoded><![CDATA[<p>Algol (Beta Per) is an extensively studied hierarchical triple system whose inner pair is a prototype semi-detached binary with mass transfer occurring from the sub-giant secondary to the main-sequence primary. We present here the results of our Algol observations made between 2006 and 2010 at the CHARA interferometer with the Michigan Infrared Combiner in the H band. The use of four telescopes with long baselines allows us to achieve better than 0.5 mas resolution and to unambiguously resolve the three stars. The inner and outer orbital elements, as well as the angular sizes and mass ratios for the three components are determined independently from previous studies. We report a significantly improved orbit for the inner stellar pair with the consequence of a 15% change in the primary mass compared to previous studies. We also determine the mutual inclination of the orbits to be much closer to perpendicularity than previously established. State-of-the-art image reconstruction algorithms are used to image the full triple system. In particular an image sequence of 55 distinct phases of the inner pair orbit is reconstructed, clearly showing the Roche-lobe-filling secondary revolving around the primary, with several epochs corresponding to the primary and secondary eclipses.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/06/imaging-the-algol-triple-system-in-h-band-with-the-chara-interferometer-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Solving the mode identification problem in asteroseismology of F stars observed with Kepler</title>
		<link>http://voxcharta.org/2012/05/03/solving-the-mode-identification-problem-in-asteroseismology-of-f-stars-observed-with-kepler/</link>
		<comments>http://voxcharta.org/2012/05/03/solving-the-mode-identification-problem-in-asteroseismology-of-f-stars-observed-with-kepler/#comments</comments>
		<pubDate>Fri, 04 May 2012 00:57:59 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absolute mode]]></category>
		<category><![CDATA[ambiguity]]></category>
		<category><![CDATA[epsilon]]></category>
		<category><![CDATA[f stars]]></category>
		<category><![CDATA[impasse]]></category>
		<category><![CDATA[kepler]]></category>
		<category><![CDATA[mode frequency]]></category>
		<category><![CDATA[mode identification]]></category>
		<category><![CDATA[oscillation modes]]></category>
		<category><![CDATA[oscillator]]></category>
		<category><![CDATA[type star]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/03/solving-the-mode-identification-problem-in-asteroseismology-of-f-stars-observed-with-kepler/</guid>
		<description><![CDATA[Asteroseismology of F-type stars has been hindered by an ambiguity in identification of their oscillation modes. The regular mode pattern that makes this task trivial in cooler stars is masked by increased linewidths. The absolute mode frequencies, encapsulated in the asteroseismic variable epsilon, can help solve this impasse because the values of epsilon implied by [...]]]></description>
			<content:encoded><![CDATA[<p>Asteroseismology of F-type stars has been hindered by an ambiguity in identification of their oscillation modes. The regular mode pattern that makes this task trivial in cooler stars is masked by increased linewidths. The absolute mode frequencies, encapsulated in the asteroseismic variable epsilon, can help solve this impasse because the values of epsilon implied by the two possible mode identifications are distinct. We find that the correct epsilon can be deduced from the effective temperature and the linewidths and we apply these methods to a sample of solar-like oscillators observed with Kepler.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/03/solving-the-mode-identification-problem-in-asteroseismology-of-f-stars-observed-with-kepler/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Detection of gravity modes in the massive binary V380 Cyg from Kepler spacebased photometry and high-resolution spectroscopy</title>
		<link>http://voxcharta.org/2012/05/03/detection-of-gravity-modes-in-the-massive-binary-v380-cyg-from-kepler-spacebased-photometry-and-high-resolution-spectroscopy/</link>
		<comments>http://voxcharta.org/2012/05/03/detection-of-gravity-modes-in-the-massive-binary-v380-cyg-from-kepler-spacebased-photometry-and-high-resolution-spectroscopy/#comments</comments>
		<pubDate>Fri, 04 May 2012 00:54:42 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[5 months]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[aperture]]></category>
		<category><![CDATA[binary star]]></category>
		<category><![CDATA[core physics]]></category>
		<category><![CDATA[cyg]]></category>
		<category><![CDATA[fundamental parameters]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[intrinsic variability]]></category>
		<category><![CDATA[kepler]]></category>
		<category><![CDATA[line profile]]></category>
		<category><![CDATA[mode oscillations]]></category>
		<category><![CDATA[noise spectroscopy]]></category>
		<category><![CDATA[orbital frequency]]></category>
		<category><![CDATA[photometric data]]></category>
		<category><![CDATA[photometry]]></category>
		<category><![CDATA[resolution spectroscopy]]></category>
		<category><![CDATA[signal to noise]]></category>
		<category><![CDATA[type star]]></category>
		<category><![CDATA[unprecedented quality]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/03/detection-of-gravity-modes-in-the-massive-binary-v380-cyg-from-kepler-spacebased-photometry-and-high-resolution-spectroscopy/</guid>
		<description><![CDATA[We report the discovery of low-amplitude gravity-mode oscillations in the massive binary star V380 Cyg, from 180 d of Kepler custom-aperture space photometry and 5 months of high-resolution high signal-to-noise spectroscopy. The new data are of unprecedented quality and allowed to improve the orbital and fundamental parameters for this binary. The orbital solution was subtracted [...]]]></description>
			<content:encoded><![CDATA[<p>We report the discovery of low-amplitude gravity-mode oscillations in the massive binary star V380 Cyg, from 180 d of Kepler custom-aperture space photometry and 5 months of high-resolution high signal-to-noise spectroscopy. The new data are of unprecedented quality and allowed to improve the orbital and fundamental parameters for this binary. The orbital solution was subtracted from the photometric data and led to the detection of periodic intrinsic variability with frequencies of which some are multiples of the orbital frequency and others are not. Spectral disentangling allowed the detection of line-profile variability in the primary. With our discovery of intrinsic variability interpreted as gravity mode oscillations, V380 Cyg becomes an important laboratory for future seismic tuning of the near-core physics in massive B-type stars.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/03/detection-of-gravity-modes-in-the-massive-binary-v380-cyg-from-kepler-spacebased-photometry-and-high-resolution-spectroscopy/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The locations of SNe Ib/c and their comparison to those of WR stars and GRBs</title>
		<link>http://voxcharta.org/2012/05/03/the-locations-of-sne-ibc-and-their-comparison-to-those-of-wr-stars-and-grbs/</link>
		<comments>http://voxcharta.org/2012/05/03/the-locations-of-sne-ibc-and-their-comparison-to-those-of-wr-stars-and-grbs/#comments</comments>
		<pubDate>Fri, 04 May 2012 00:52:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[burst]]></category>
		<category><![CDATA[environments]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[grbs]]></category>
		<category><![CDATA[massive star]]></category>
		<category><![CDATA[metallicity]]></category>
		<category><![CDATA[number of galaxies]]></category>
		<category><![CDATA[progenitor]]></category>
		<category><![CDATA[SNe]]></category>
		<category><![CDATA[spectroscopic study]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[supernovae]]></category>
		<category><![CDATA[wn distribution]]></category>
		<category><![CDATA[wr stars]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/03/the-locations-of-sne-ibc-and-their-comparison-to-those-of-wr-stars-and-grbs/</guid>
		<description><![CDATA[The locations of long GRBs and stripped supernovae are compared to those of their favored progenitors, WR stars, and their sub-classes. Compared to Leloudas et al. (2010), we have doubled the number of galaxies with suitable WR data. In the combined sample, WC stars are found, on average, in brighter locations than WN stars. The [...]]]></description>
			<content:encoded><![CDATA[<p>The locations of long GRBs and stripped supernovae are compared to those of their favored progenitors, WR stars, and their sub-classes. Compared to Leloudas et al. (2010), we have doubled the number of galaxies with suitable WR data. In the combined sample, WC stars are found, on average, in brighter locations than WN stars. The WN distribution is fully consistent with the one of SNe Ib, while it is inconsistent with those of SNe II, Ic and GRBs. The WC distribution is both consistent with SNe Ib and Ic. It is inconsistent with SNe II, and marginally consistent with GRBs. Furthermore, we present a spectroscopic study of the locations of SNe Ib/c. The average metallicity in the environments of SNe Ic is found to be a little higher than for SNe Ib, but the difference is small and not significant within our sample. Under the assumption that the SN regions were formed in an instantaneous burst of star formation, we find that a fraction of them appear older than what is allowed in order to host SNe Ib/c from single massive stars. Within this framework, these SNe must come from lower mass binaries.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/03/the-locations-of-sne-ibc-and-their-comparison-to-those-of-wr-stars-and-grbs/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>First Simultaneous Detection of Moving Magnetic Features in Photospheric Intensity and Magnetic Field Data</title>
		<link>http://voxcharta.org/2012/05/03/first-simultaneous-detection-of-moving-magnetic-features-in-photospheric-intensity-and-magnetic-field-data/</link>
		<comments>http://voxcharta.org/2012/05/03/first-simultaneous-detection-of-moving-magnetic-features-in-photospheric-intensity-and-magnetic-field-data/#comments</comments>
		<pubDate>Fri, 04 May 2012 00:52:22 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[big bear solar observatory]]></category>
		<category><![CDATA[bipolar]]></category>
		<category><![CDATA[broadband]]></category>
		<category><![CDATA[doppler velocity]]></category>
		<category><![CDATA[filament]]></category>
		<category><![CDATA[filamentary structure]]></category>
		<category><![CDATA[hinode]]></category>
		<category><![CDATA[intensity image]]></category>
		<category><![CDATA[magnetic field data]]></category>
		<category><![CDATA[mmf]]></category>
		<category><![CDATA[penumbra]]></category>
		<category><![CDATA[photometric properties]]></category>
		<category><![CDATA[polarity]]></category>
		<category><![CDATA[simultaneous detection]]></category>
		<category><![CDATA[solar telescope]]></category>
		<category><![CDATA[temporal evolution]]></category>
		<category><![CDATA[temporal resolution]]></category>
		<category><![CDATA[vector]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/03/first-simultaneous-detection-of-moving-magnetic-features-in-photospheric-intensity-and-magnetic-field-data/</guid>
		<description><![CDATA[The formation and the temporal evolution of a bipolar moving magnetic feature (MMF) was studied with high spatial and temporal resolution. The photometric properties were observed with the New Solar Telescope at Big Bear Solar Observatory using a broadband TiO filter (705.7 nm), while the magnetic field was analyzed using the spectropolarimetric data obtained by [...]]]></description>
			<content:encoded><![CDATA[<p>The formation and the temporal evolution of a bipolar moving magnetic feature (MMF) was studied with high spatial and temporal resolution. The photometric properties were observed with the New Solar Telescope at Big Bear Solar Observatory using a broadband TiO filter (705.7 nm), while the magnetic field was analyzed using the spectropolarimetric data obtained by Hinode. For the first time, we observed a bipolar MMF simultaneously in intensity images and magnetic field data, and studied the details of its structure. The vector magnetic field and the Doppler velocity of the MMF were also studied. A bipolar MMF having its positive polarity closer to the negative penumbra formed being accompanied by a bright, filamentary structure in the TiO data connecting the MMF and a dark penumbral filament. A fast downflow (&lt;2km/s) was detected at the positive polarity. The vector magnetic field obtained from the full Stokes inversion revealed that a bipolar MMF has a U-shaped magnetic field configuration. Our observations provide a clear intensity counterpart of the observed MMF in the photosphere, and strong evidence of the connection between the MMF and the penumbral filament as a serpentine field.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/03/first-simultaneous-detection-of-moving-magnetic-features-in-photospheric-intensity-and-magnetic-field-data/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Modeling the irregularities of solar cycle using flux transport dynamo models</title>
		<link>http://voxcharta.org/2012/05/03/modeling-the-irregularities-of-solar-cycle-using-flux-transport-dynamo-models/</link>
		<comments>http://voxcharta.org/2012/05/03/modeling-the-irregularities-of-solar-cycle-using-flux-transport-dynamo-models/#comments</comments>
		<pubDate>Fri, 04 May 2012 00:49:45 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[convection zone]]></category>
		<category><![CDATA[diffusivity]]></category>
		<category><![CDATA[dynamo models]]></category>
		<category><![CDATA[fluctuation]]></category>
		<category><![CDATA[irregular features]]></category>
		<category><![CDATA[irregular manner]]></category>
		<category><![CDATA[irregularity]]></category>
		<category><![CDATA[solar cycle]]></category>
		<category><![CDATA[sunspot number]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/03/modeling-the-irregularities-of-solar-cycle-using-flux-transport-dynamo-models/</guid>
		<description><![CDATA[The sunspot number varies roughly periodically with time. However the individual cycle durations and the amplitudes are found to vary in an irregular manner. It is observed that the stronger cycles are having shorter rise times and vice versa. This leads to an important effect know as the Waldmeier effect. Another important feature of the [...]]]></description>
			<content:encoded><![CDATA[<p>The sunspot number varies roughly periodically with time. However the individual cycle durations and the amplitudes are found to vary in an irregular manner. It is observed that the stronger cycles are having shorter rise times and vice versa. This leads to an important effect know as the Waldmeier effect. Another important feature of the solar cycle irregularity are the grand minima during which the activity level is strongly reduced. We explore whether these solar cycle irregularities can be studied with the help of the flux transport dynamo model of the solar cycle. We show that with a suitable stochastic fluctuations in a regular dynamo model, we are able to reproduce many irregular features of the solar cycle including the Waldmeier effect and the grand minimum. However, we get all these results only if the value of the turbulent diffusivity in the convection zone is reasonably high.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/03/modeling-the-irregularities-of-solar-cycle-using-flux-transport-dynamo-models/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A unifying picture of helical and azimuthal MRI, and the universal significance of the Liu limit</title>
		<link>http://voxcharta.org/2012/05/03/a-unifying-picture-of-helical-and-azimuthal-mri-and-the-universal-significance-of-the-liu-limit/</link>
		<comments>http://voxcharta.org/2012/05/03/a-unifying-picture-of-helical-and-azimuthal-mri-and-the-universal-significance-of-the-liu-limit/#comments</comments>
		<pubDate>Fri, 04 May 2012 00:47:43 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion disk]]></category>
		<category><![CDATA[approximation]]></category>
		<category><![CDATA[cosmic structure formation]]></category>
		<category><![CDATA[helical]]></category>
		<category><![CDATA[key role]]></category>
		<category><![CDATA[liu]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[mri]]></category>
		<category><![CDATA[prandtl number]]></category>
		<category><![CDATA[ratios]]></category>
		<category><![CDATA[short wavelength]]></category>
		<category><![CDATA[Turbulence]]></category>
		<category><![CDATA[unified description]]></category>
		<category><![CDATA[universal behaviour]]></category>
		<category><![CDATA[universal character]]></category>
		<category><![CDATA[universal significance]]></category>
		<category><![CDATA[wavenumber]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/03/a-unifying-picture-of-helical-and-azimuthal-mri-and-the-universal-significance-of-the-liu-limit/</guid>
		<description><![CDATA[The magnetorotational instability (MRI) plays a key role for cosmic structure formation by triggering turbulence in the rotating flows of accretion disks that would be otherwise hydrodynamically stable. In the limit of small magnetic Prandtl number, the helical and the azimuthal version of MRI are known to be governed by a quite different scaling behaviour [...]]]></description>
			<content:encoded><![CDATA[<p>The magnetorotational instability (MRI) plays a key role for cosmic structure formation by triggering turbulence in the rotating flows of accretion disks that would be otherwise hydrodynamically stable. In the limit of small magnetic Prandtl number, the helical and the azimuthal version of MRI are known to be governed by a quite different scaling behaviour than the standard MRI with a vertical applied magnetic field. Using the short-wavelength approximation for an incompressible, resistive, and viscous rotating fluid we present a unified description of helical and azimuthal MRI, and we identify the universal character of the Liu limit Ro= -0.8284 for the critical Rossby number. From this universal behaviour we are also lead to the prediction of higher azimuthal wavenumber for rather small ratios of azimuthal to axial applied fields.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/03/a-unifying-picture-of-helical-and-azimuthal-mri-and-the-universal-significance-of-the-liu-limit/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Sensitivity of astrophysical reaction rates to nuclear uncertainties</title>
		<link>http://voxcharta.org/2012/05/03/sensitivity-of-astrophysical-reaction-rates-to-nuclear-uncertainties/</link>
		<comments>http://voxcharta.org/2012/05/03/sensitivity-of-astrophysical-reaction-rates-to-nuclear-uncertainties/#comments</comments>
		<pubDate>Fri, 04 May 2012 00:46:32 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[dripline]]></category>
		<category><![CDATA[neutron]]></category>
		<category><![CDATA[nuclear properties]]></category>
		<category><![CDATA[nuclear reaction rates]]></category>
		<category><![CDATA[proton]]></category>
		<category><![CDATA[target nuclei]]></category>
		<category><![CDATA[uncertainty]]></category>
		<category><![CDATA[variation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/03/sensitivity-of-astrophysical-reaction-rates-to-nuclear-uncertainties/</guid>
		<description><![CDATA[Sensitivities of nuclear reaction rates to a variation of nuclear properties are studied. Target nuclei range from proton- to neutron-dripline for 10&#60;=Z&#60;=83. Reactions considered are nucleon- and alpha-induced reactions mediated by the strong interaction. The contribution of reactions proceeding on the target ground state to the total stellar rate is also given. General dependences on [...]]]></description>
			<content:encoded><![CDATA[<p>Sensitivities of nuclear reaction rates to a variation of nuclear properties are studied. Target nuclei range from proton- to neutron-dripline for 10&lt;=Z&lt;=83. Reactions considered are nucleon- and alpha-induced reactions mediated by the strong interaction. The contribution of reactions proceeding on the target ground state to the total stellar rate is also given. General dependences on various input quantities are discussed. Additionally, sensitivities of laboratory cross sections of nucleon-, alpha-, and gamma-induced reactions are shown, allowing to estimate the impact of cross section measurements. Finally, recommended procedures to explore and improve reaction rate uncertainties using the present sensitivity data are outlined.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/03/sensitivity-of-astrophysical-reaction-rates-to-nuclear-uncertainties/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Properties of Ground Level Enhancement Events and the Associated Solar Eruptions during Solar Cycle 23</title>
		<link>http://voxcharta.org/2012/05/03/properties-of-ground-level-enhancement-events-and-the-associated-solar-eruptions-during-solar-cycle-23/</link>
		<comments>http://voxcharta.org/2012/05/03/properties-of-ground-level-enhancement-events-and-the-associated-solar-eruptions-during-solar-cycle-23/#comments</comments>
		<pubDate>Fri, 04 May 2012 00:46:04 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration]]></category>
		<category><![CDATA[class flare]]></category>
		<category><![CDATA[dependence]]></category>
		<category><![CDATA[dispersion analysis]]></category>
		<category><![CDATA[earth observer]]></category>
		<category><![CDATA[gle]]></category>
		<category><![CDATA[initial acceleration]]></category>
		<category><![CDATA[low frequency]]></category>
		<category><![CDATA[msh]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[reames]]></category>
		<category><![CDATA[shock formation]]></category>
		<category><![CDATA[soft x]]></category>
		<category><![CDATA[solar cycle]]></category>
		<category><![CDATA[solar eruption]]></category>
		<category><![CDATA[speed profile]]></category>
		<category><![CDATA[velocity dispersion]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/03/properties-of-ground-level-enhancement-events-and-the-associated-solar-eruptions-during-solar-cycle-23/</guid>
		<description><![CDATA[We present an overview of the observed properties of the GLEs and those of the associated flares and CMEs. The solar eruptions are very intense involving X-class flares and extreme CME speeds (average ~2000 km/s). The active regions in which the GLE events originate are generally large: 1290 msh (median 1010 msh) compared to 934 [...]]]></description>
			<content:encoded><![CDATA[<p>We present an overview of the observed properties of the GLEs and those of the associated flares and CMEs. The solar eruptions are very intense involving X-class flares and extreme CME speeds (average ~2000 km/s). The active regions in which the GLE events originate are generally large: 1290 msh (median 1010 msh) compared to 934 msh (median: 790 msh) for SEP-producing active regions. The initial acceleration of GLE-associated CMEs is much larger (by a factor of 2) than that of ordinary CMEs (2.3 km/s2 vs.1 km/s2). The GLE particle release is delayed with respect to the onset of all electromagnetic signatures of the eruptions: type II bursts, low frequency type III bursts, soft X-ray flares and CMEs. The presence of metric type II radio bursts some 17 min (median: 16 min; range: 3 to 48 min) before the GLE onset indicates shock formation well before the particle release. The release of GLE particles occurs when the CMEs reach an average height of ~3.09 Rs for well-connected events. For poorly connected events, the average CME height at GLE particle release is ~66% larger (mean: 5.18 Rs). The longitudinal dependence is consistent with shock accelerations because the shocks from poorly connected events need to expand more to cross the field lines connecting to an Earth observer. The CME height at metric type II burst onset is in the narrow range 1.29 to 1.8 Rs, with A mean of 1.53 Rs. The CME heights at metric type II burst onset and GLE particle release correspond to the minimum and maximum in the Alfven speed profile. The CME heights at GLE particle release are in good agreement with those obtained from the velocity dispersion analysis (Reames, 2009a,b) including the source longitude dependence. We also discuss the implications of the delay of GLE particle release with respect to complex type III bursts and hard X-ray emission.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/03/properties-of-ground-level-enhancement-events-and-the-associated-solar-eruptions-during-solar-cycle-23/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Relationship Between the Expansion Speed and Radial Speed of CMEs Confirmed Using Quadrature Observations of the 2011 February 15 CME</title>
		<link>http://voxcharta.org/2012/05/03/the-relationship-between-the-expansion-speed-and-radial-speed-of-cmes-confirmed-using-quadrature-observations-of-the-2011-february-15-cme/</link>
		<comments>http://voxcharta.org/2012/05/03/the-relationship-between-the-expansion-speed-and-radial-speed-of-cmes-confirmed-using-quadrature-observations-of-the-2011-february-15-cme/#comments</comments>
		<pubDate>Fri, 04 May 2012 00:44:13 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[board soho]]></category>
		<category><![CDATA[coronagraph]]></category>
		<category><![CDATA[earth line]]></category>
		<category><![CDATA[earth view]]></category>
		<category><![CDATA[empirical relationship]]></category>
		<category><![CDATA[geometrical considerations]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[lasco observations]]></category>
		<category><![CDATA[Measurement]]></category>
		<category><![CDATA[plane speed]]></category>
		<category><![CDATA[radial speed]]></category>
		<category><![CDATA[sky]]></category>
		<category><![CDATA[soho lasco]]></category>
		<category><![CDATA[space weather]]></category>
		<category><![CDATA[stereo measurements]]></category>
		<category><![CDATA[stereo spacecraft]]></category>
		<category><![CDATA[sun earth]]></category>
		<category><![CDATA[true speed]]></category>
		<category><![CDATA[vexp]]></category>
		<category><![CDATA[weather application]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/03/the-relationship-between-the-expansion-speed-and-radial-speed-of-cmes-confirmed-using-quadrature-observations-of-the-2011-february-15-cme/</guid>
		<description><![CDATA[It is difficult to measure the true speed of Earth-directed CMEs from a coronagraph located along the Sun-Earth line because of the occulting disk. However, the expansion speed (the speed with which the CME appears to spread in the sky plane) can be measured by such a coronagraph. In order to convert the expansion speed [...]]]></description>
			<content:encoded><![CDATA[<p>It is difficult to measure the true speed of Earth-directed CMEs from a coronagraph located along the Sun-Earth line because of the occulting disk. However, the expansion speed (the speed with which the CME appears to spread in the sky plane) can be measured by such a coronagraph. In order to convert the expansion speed to radial speed (which is important for space weather applications) one can use an empirical relationship between the two that assumes an average width for all CMEs. If we have the width information from quadrature observations, we can confirm the relationship between expansion and radial speeds derived by Gopalswamy et al. (2009a). The STEREO spacecraft were in qudrature with SOHO (STEREO-A ahead of Earth by 87o and STEREO-B 94o behind Earth) on 2011 February 15, when a fast Earth-directed CME occurred. The CME was observed as a halo by the Large-Angle and Spectrometric Coronagraph (LASCO) on board SOHO. The sky-plane speed was measured by SOHO/LASCO as the expansion speed, while the radial speed was measured by STEREO-A and STEREO-B. In addition, STEREO-A and STEREO-B images provided the width of the CME, which is unknown from Earth view. From the SOHO and STEREO measurements, we confirm the relationship between the expansion speed (Vexp) and radial speed (Vrad) derived previously from geometrical considerations (Gopalswamy et al. 2009a): Vrad = 1/2 (1 + cot w)Vexp, where w is the half width of the CME. STEREO-B images of the CME, we found that CME had a full width of 76o, so w = 38o. This gives the relation as Vrad = 1.14 Vexp. From LASCO observations, we measured Vexp = 897 km/s, so we get the radial speed as 1023 km/s. Direct measurement of radial speed yields 945 km/s (STEREO-A) and 1058 km/s (STEREO-B). These numbers are different only by 7.6% and 3.4% (for STEREO-A and STEREO-B, respectively) from the computed value.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/03/the-relationship-between-the-expansion-speed-and-radial-speed-of-cmes-confirmed-using-quadrature-observations-of-the-2011-february-15-cme/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Interpreting Magnetic Variance Anisotropy Measurements in the Solar Wind [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/03/interpreting-magnetic-variance-anisotropy-measurements-in-the-solar-wind-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/03/interpreting-magnetic-variance-anisotropy-measurements-in-the-solar-wind-cross-listing/#comments</comments>
		<pubDate>Fri, 04 May 2012 00:43:43 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[anisotropy measurements]]></category>
		<category><![CDATA[composition]]></category>
		<category><![CDATA[fluctuation]]></category>
		<category><![CDATA[informative method]]></category>
		<category><![CDATA[interval]]></category>
		<category><![CDATA[linear theory]]></category>
		<category><![CDATA[literature]]></category>
		<category><![CDATA[scales]]></category>
		<category><![CDATA[solar wind]]></category>
		<category><![CDATA[spacecraft data]]></category>
		<category><![CDATA[turbulence simulation]]></category>
		<category><![CDATA[turbulent fluctuations]]></category>
		<category><![CDATA[variance]]></category>
		<category><![CDATA[wind measurements]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/03/interpreting-magnetic-variance-anisotropy-measurements-in-the-solar-wind-cross-listing/</guid>
		<description><![CDATA[The magnetic variance anisotropy ($\mathcal{A}_m$) of the solar wind has been used widely as a method to identify the nature of solar wind turbulent fluctuations; however, a thorough discussion of the meaning and interpretation of the $\mathcal{A}_m$ has not appeared in the literature. This paper explores the implications and limitations of using the $\mathcal{A}_m$ as [...]]]></description>
			<content:encoded><![CDATA[<p>The magnetic variance anisotropy ($\mathcal{A}_m$) of the solar wind has been used widely as a method to identify the nature of solar wind turbulent fluctuations; however, a thorough discussion of the meaning and interpretation of the $\mathcal{A}_m$ has not appeared in the literature. This paper explores the implications and limitations of using the $\mathcal{A}_m$ as a method for constraining the solar wind fluctuation mode composition and presents a more informative method for interpreting spacecraft data. The paper also compares predictions of the $\mathcal{A}_m$ from linear theory to nonlinear turbulence simulations and solar wind measurements. In both cases, linear theory compares well and suggests the solar wind for the interval studied is dominantly Alfv\&#8217;{e}nic in the inertial and dissipation ranges to scales $k \rho_i \simeq 5$.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/03/interpreting-magnetic-variance-anisotropy-measurements-in-the-solar-wind-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Imaging the Algol Triple System in H Band with the CHARA Interferometer</title>
		<link>http://voxcharta.org/2012/05/03/imaging-the-algol-triple-system-in-h-band-with-the-chara-interferometer/</link>
		<comments>http://voxcharta.org/2012/05/03/imaging-the-algol-triple-system-in-h-band-with-the-chara-interferometer/#comments</comments>
		<pubDate>Fri, 04 May 2012 00:43:11 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[algol]]></category>
		<category><![CDATA[angular size]]></category>
		<category><![CDATA[art image]]></category>
		<category><![CDATA[baseline]]></category>
		<category><![CDATA[chara interferometer]]></category>
		<category><![CDATA[eclipse]]></category>
		<category><![CDATA[epochs]]></category>
		<category><![CDATA[image reconstruction]]></category>
		<category><![CDATA[image sequence]]></category>
		<category><![CDATA[inclination]]></category>
		<category><![CDATA[main sequence]]></category>
		<category><![CDATA[mass ratio]]></category>
		<category><![CDATA[mass transfer]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[orbital element]]></category>
		<category><![CDATA[reconstruction algorithm]]></category>
		<category><![CDATA[roche lobe]]></category>
		<category><![CDATA[stellar pair]]></category>
		<category><![CDATA[telescopes]]></category>
		<category><![CDATA[three star]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/03/imaging-the-algol-triple-system-in-h-band-with-the-chara-interferometer/</guid>
		<description><![CDATA[Algol (Beta Per) is an extensively studied hierarchical triple system whose inner pair is a prototype semi-detached binary with mass transfer occurring from the main-sequence primary to the sub-giant secondary. We present here the results of our Algol observations made between 2006 and 2010 at the CHARA interferometer with the Michigan Infrared Combiner in the [...]]]></description>
			<content:encoded><![CDATA[<p>Algol (Beta Per) is an extensively studied hierarchical triple system whose inner pair is a prototype semi-detached binary with mass transfer occurring from the main-sequence primary to the sub-giant secondary. We present here the results of our Algol observations made between 2006 and 2010 at the CHARA interferometer with the Michigan Infrared Combiner in the H band. The use of four telescopes with long baselines allows us to achieve better than 0.5 mas resolution and to unambiguously resolve the three stars. The inner and outer orbital elements, as well as the angular sizes and mass ratios for the three components are determined independently from previous studies. We report a significantly improved orbit for the inner stellar pair with the consequence of a 15% change in the primary mass compared to previous studies. We also determine the mutual inclination of the orbits to be much closer to perpendicularity than previously established. State-of-the-art image reconstruction algorithms are used to image the full triple system. In particular an image sequence of 55 distinct phases of the inner pair orbit is reconstructed, clearly showing the Roche-lobe-filling secondary revolving around the primary, with several epochs corresponding to the primary and secondary eclipses.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/03/imaging-the-algol-triple-system-in-h-band-with-the-chara-interferometer/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Theoretical Delay Time Distributions [Replacement]</title>
		<link>http://voxcharta.org/2012/05/03/theoretical-delay-time-distributions-replacement/</link>
		<comments>http://voxcharta.org/2012/05/03/theoretical-delay-time-distributions-replacement/#comments</comments>
		<pubDate>Fri, 04 May 2012 00:31:48 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[delay time]]></category>
		<category><![CDATA[efficiency]]></category>
		<category><![CDATA[hydrogen]]></category>
		<category><![CDATA[population]]></category>
		<category><![CDATA[progenitor]]></category>
		<category><![CDATA[research group]]></category>
		<category><![CDATA[synthesis]]></category>
		<category><![CDATA[time distribution]]></category>
		<category><![CDATA[type ia]]></category>
		<category><![CDATA[white dwarf]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/03/theoretical-delay-time-distributions-replacement/</guid>
		<description><![CDATA[We briefly discuss the method of population synthesis to calculate theoretical delay time distributions of type Ia supernova progenitors. We also compare the results of the different research groups and conclude that although one of the main differences in the results for single degenerate progenitors is the retention efficiency with which accreted hydrogen is added [...]]]></description>
			<content:encoded><![CDATA[<p>We briefly discuss the method of population synthesis to calculate theoretical delay time distributions of type Ia supernova progenitors. We also compare the results of the different research groups and conclude that although one of the main differences in the results for single degenerate progenitors is the retention efficiency with which accreted hydrogen is added to the white dwarf core, this cannot explain all the differences.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/03/theoretical-delay-time-distributions-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Observing Simulated Protostars with Outflows: How Accurate are Protostellar Properties Inferred from SEDs?</title>
		<link>http://voxcharta.org/2012/05/02/observing-simulated-protostars-with-outflows-how-accurate-are-protostellar-properties-inferred-from-seds/</link>
		<comments>http://voxcharta.org/2012/05/02/observing-simulated-protostars-with-outflows-how-accurate-are-protostellar-properties-inferred-from-seds/#comments</comments>
		<pubDate>Thu, 03 May 2012 00:50:19 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[adaptive mesh refinement]]></category>
		<category><![CDATA[aperture size]]></category>
		<category><![CDATA[disk mass]]></category>
		<category><![CDATA[evolutionary stage]]></category>
		<category><![CDATA[fitting model]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[mass star]]></category>
		<category><![CDATA[molecular cloud]]></category>
		<category><![CDATA[protostar]]></category>
		<category><![CDATA[radiation hydrodynamics]]></category>
		<category><![CDATA[radiative transfer code]]></category>
		<category><![CDATA[radiative transfer model]]></category>
		<category><![CDATA[simulation properties]]></category>
		<category><![CDATA[source parameters]]></category>
		<category><![CDATA[spectral energy distribution]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[stellar parameters]]></category>
		<category><![CDATA[temperature distribution]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/02/observing-simulated-protostars-with-outflows-how-accurate-are-protostellar-properties-inferred-from-seds/</guid>
		<description><![CDATA[The properties of unresolved protostars and their local environment are frequently inferred from spectral energy distributions (SEDs) using radiative transfer modeling. We perform synthetic observations of realistic star formation simulations to evaluate the accuracy of properties inferred from fitting model SEDs to observations. We use ORION, an adaptive mesh refinement (AMR) three-dimensional gravito-radiation-hydrodynamics code, to [...]]]></description>
			<content:encoded><![CDATA[<p>The properties of unresolved protostars and their local environment are frequently inferred from spectral energy distributions (SEDs) using radiative transfer modeling. We perform synthetic observations of realistic star formation simulations to evaluate the accuracy of properties inferred from fitting model SEDs to observations. We use ORION, an adaptive mesh refinement (AMR) three-dimensional gravito-radiation-hydrodynamics code, to simulate low-mass star formation in a turbulent molecular cloud including the effects of protostellar outflows. To obtain the dust temperature distribution and SEDs of the forming protostars, we post-process the simulations using HYPERION, a state-of-the-art Monte-Carlo radiative transfer code. We find that the ORION and HYPERION dust temperatures typically agree within a factor of two. We compare synthetic SEDs of embedded protostars for a range of evolutionary times, simulation resolutions, aperture sizes, and viewing angles. We demonstrate that complex, asymmetric gas morphology leads to a variety of classifications for individual objects as a function of viewing angle. We derive best-fit source parameters for each SED through comparison with a pre-computed grid of radiative transfer models. While the SED models correctly identify the evolutionary stage of the synthetic sources as embedded protostars, we show that the disk and stellar parameters can be very discrepant from the simulated values. Parameters such as the stellar accretion rate, stellar mass, and disk mass show better agreement, but can still deviate significantly, and the agreement may in some cases be artificially good due to the limited range of parameters in the set of model SEDs. Lack of correlation between the model and simulation properties in many individual instances cautions against over-interpreting properties inferred from SEDs for unresolved protostellar sources. (Abridged)</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/02/observing-simulated-protostars-with-outflows-how-accurate-are-protostellar-properties-inferred-from-seds/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
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