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	<title>Vox Charta &#187; High Energy</title>
	<atom:link href="http://voxcharta.org/category/astro-ph/high-energy-astro-ph/feed/" rel="self" type="application/rss+xml" />
	<link>http://voxcharta.org</link>
	<description></description>
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		<title>The optically unbiased GRB host (TOUGH) survey. VI. Radio observations at z&lt;1 and consistency with typical star-forming galaxies</title>
		<link>http://voxcharta.org/2012/05/21/the-optically-unbiased-grb-host-tough-survey-vi-radio-observations-at-z1-and-consistency-with-typical-star-forming-galaxies/</link>
		<comments>http://voxcharta.org/2012/05/21/the-optically-unbiased-grb-host-tough-survey-vi-radio-observations-at-z1-and-consistency-with-typical-star-forming-galaxies/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:54:52 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[radio observation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/the-optically-unbiased-grb-host-tough-survey-vi-radio-observations-at-z1-and-consistency-with-typical-star-forming-galaxies/</guid>
		<description><![CDATA[We present late-time Hubble Space Telescope imaging of the fields of six Swift GRBs lying at 5.0&#60;z&#60;9.5. Our data includes very deep observations of the field of the most distant spectroscopically confirmed burst, GRB 090423, at z=8.2. Using the precise positions afforded by their afterglows we can place stringent limits on the luminosities of their [...]]]></description>
			<content:encoded><![CDATA[<p>We present late-time Hubble Space Telescope imaging of the fields of six Swift GRBs lying at 5.0&lt;z&lt;9.5. Our data includes very deep observations of the field of the most distant spectroscopically confirmed burst, GRB 090423, at z=8.2. Using the precise positions afforded by their afterglows we can place stringent limits on the luminosities of their host galaxies. In one case, that of GRB 060522 at z=5.11, there is a marginal excess of flux close to the GRB position which may be a detection of a host at a magnitude J(AB)=28.5. None of the others are significantly detected meaning that all the hosts lie below L\star at their respective redshifts, with star formation rates SFR&lt;4Mo/yr in all cases. Indeed, stacking the five fields with WFC3-IR data we conclude a mean SFR&lt;0.17Mo/yr per galaxy. These results support the proposition that the bulk of star formation, and hence integrated UV luminosity, at high redshifts arises in galaxies below the detection limits of deep-field observations. Making the reasonable assumption that GRB rate is proportional to UV luminosity at early times allows us to compare our limits with expectations based on galaxy luminosity functions derived from the Hubble Ultra-Deep Field (HUDF) and other deep fields. We infer that a luminosity function which is evolving rapidly towards steeper faint-end slope (alpha) and decreasing characteristic luminosity (L\star), as suggested by some other studies, is consistent with our observations, whereas a non-evolving LF shape is ruled out at &gt;90% confidence. Although it is not yet possible to make stronger statements, in the future, with larger samples and a fuller understanding of the conditions required for GRB production, studies like this hold great potential for probing the nature of star formation, the shape of the galaxy luminosity function, and the supply of ionizing photons in the early universe.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/the-optically-unbiased-grb-host-tough-survey-vi-radio-observations-at-z1-and-consistency-with-typical-star-forming-galaxies/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>X-ray variability of 104 active galactic nuclei. XMM-Newton power-spectrum density profiles</title>
		<link>http://voxcharta.org/2012/05/21/x-ray-variability-of-104-active-galactic-nuclei-xmm-newton-power-spectrum-density-profiles/</link>
		<comments>http://voxcharta.org/2012/05/21/x-ray-variability-of-104-active-galactic-nuclei-xmm-newton-power-spectrum-density-profiles/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:53:36 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[correspondence]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[density profile]]></category>
		<category><![CDATA[Newton]]></category>
		<category><![CDATA[power spectra]]></category>
		<category><![CDATA[power spectrum]]></category>
		<category><![CDATA[ray binaries]]></category>
		<category><![CDATA[scales]]></category>
		<category><![CDATA[shape]]></category>
		<category><![CDATA[uniform analysis]]></category>
		<category><![CDATA[variability]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/x-ray-variability-of-104-active-galactic-nuclei-xmm-newton-power-spectrum-density-profiles/</guid>
		<description><![CDATA[AGN, powered by accretion onto SMBHs, are thought to be scaled up versions of Galactic black hole X-ray binaries (BH-XRBs). In the past few years evidence of such correspondence include similarities in the broadband shape of the X-ray variability power spectra, with characteristic bend times-scales scaling with mass. We have performed a uniform analysis of [...]]]></description>
			<content:encoded><![CDATA[<p>AGN, powered by accretion onto SMBHs, are thought to be scaled up versions of Galactic black hole X-ray binaries (BH-XRBs). In the past few years evidence of such correspondence include similarities in the broadband shape of the X-ray variability power spectra, with characteristic bend times-scales scaling with mass. We have performed a uniform analysis of the power spectrum densities (PSDs) of 104 nearby (z&lt;0.4) AGN using 209 XMM-Newton/pn observations. The PSDs have been estimated in three energy bands: 0.2-10, 0.2-2, and 2-10 keV. The sample comprises 61 Type-1 AGN, 21 Type-2 AGN, 15 NLSy1, and 7 BLLACS. We have fitted each PSD to two models: (1) a single power-law model and (2) a bending power-law model. Among the entire sample, 72% show significant variability in at least one of the three bands tested. A high percentage of low-luminosity AGN do not show any significant variability. The PSD of the majority of the variable AGN was well described by a simple power-law with a mean index of 2. In 15 sources we found that the bending power law model was preferred with a mean slope of 3 and a mean bend frequency of 2.E-04 Hz. Only KUG1031+398 (REJ1034+396) shows evidence for quasi-periodic oscillations. The `fundamental plane&#039; relating variability timescale, black hole mass, and luminosity is demonstrated using the new X-ray timing results presented here together with a compilation of the previously detected timescales from the literature. Both quantitative (i.e. scaling with BH mass) and qualitative (overall PSD shapes) found in this sample of AGN are in agreement with the expectations for the SMBHs and BH-XRBs being the same phenomenon scaled-up with the size of the BH. The steep PSD slopes above the high frequency bend bear a closer resemblance to those of the `soft/thermal dominated&#039; BH-XRB states than other states.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/x-ray-variability-of-104-active-galactic-nuclei-xmm-newton-power-spectrum-density-profiles/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A Public Set of Synthetic Spectra from Expanding Atmospheres for X-Ray Novae. I. Solar Abundances</title>
		<link>http://voxcharta.org/2012/05/21/a-public-set-of-synthetic-spectra-from-expanding-atmospheres-for-x-ray-novae-i-solar-abundances/</link>
		<comments>http://voxcharta.org/2012/05/21/a-public-set-of-synthetic-spectra-from-expanding-atmospheres-for-x-ray-novae-i-solar-abundances/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:53:03 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorption line]]></category>
		<category><![CDATA[abundance]]></category>
		<category><![CDATA[atmosphere]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[eff]]></category>
		<category><![CDATA[example application]]></category>
		<category><![CDATA[grating]]></category>
		<category><![CDATA[line profile]]></category>
		<category><![CDATA[mass loss]]></category>
		<category><![CDATA[model parameter]]></category>
		<category><![CDATA[SGR]]></category>
		<category><![CDATA[solar set]]></category>
		<category><![CDATA[static model]]></category>
		<category><![CDATA[stellar atmosphere]]></category>
		<category><![CDATA[synthetic spectra]]></category>
		<category><![CDATA[van rossum]]></category>
		<category><![CDATA[white dwarf]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/a-public-set-of-synthetic-spectra-from-expanding-atmospheres-for-x-ray-novae-i-solar-abundances/</guid>
		<description><![CDATA[X-ray grating observations have revealed great detail in the spectra of Novae in the Super Soft Source (SSS) phase. Notable features in the SSS spectra are blue-shifted absorption lines, P-Cygni line profiles, and the absence of strong ionization edges, all of which are indicators of an expanding atmosphere.   We present, and make publicly [...]]]></description>
			<content:encoded><![CDATA[<p>X-ray grating observations have revealed great detail in the spectra of Novae in the Super Soft Source (SSS) phase. Notable features in the SSS spectra are blue-shifted absorption lines, P-Cygni line profiles, and the absence of strong ionization edges, all of which are indicators of an expanding atmosphere.   We present, and make publicly available, a set of 672 wind-type (WT) synthetic spectra, obtained from the expanding NLTE SSS models introduced in Van Rossum 2010 with the PHOENIX stellar atmosphere code. The set presented in this paper is limited to solar abundances with the aim to focus on the basic model parameters and their effect on the spectra, providing the basis upon which abundance effects can be studied using a much bigger non-solar set in the next paper in this series.   We fit the WT spectra to the five grating spectra taken in the SSS phase of nova V4743 Sgr 2003 as an example application of the WT models. Within the limits of solar abundances we demonstrate that the following parameters are constrained by the data (in order of decreasing accuracy): column density N_H, bolometric luminosity L_bol, effective temperature T_eff, white dwarf radius R, wind asymptotic velocity v_inf, and the mass-loss rate M_dot. The models are also sensitive to the assumed white dwarf mass M_wd but the effect on the spectra can largely be compensated by the other model parameters. The WT spectra with solar abundances fit the data better than abundance optimized hydro-static models.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/a-public-set-of-synthetic-spectra-from-expanding-atmospheres-for-x-ray-novae-i-solar-abundances/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A reduction in the UHE neutrino flux due to neutrino spin precession</title>
		<link>http://voxcharta.org/2012/05/21/a-reduction-in-the-uhe-neutrino-flux-due-to-neutrino-spin-precession/</link>
		<comments>http://voxcharta.org/2012/05/21/a-reduction-in-the-uhe-neutrino-flux-due-to-neutrino-spin-precession/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:51:36 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[astrophysical objects]]></category>
		<category><![CDATA[gamma ray burst]]></category>
		<category><![CDATA[intense magnetic field]]></category>
		<category><![CDATA[magnetic moment]]></category>
		<category><![CDATA[neutrino]]></category>
		<category><![CDATA[transition]]></category>
		<category><![CDATA[uhe]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/a-reduction-in-the-uhe-neutrino-flux-due-to-neutrino-spin-precession/</guid>
		<description><![CDATA[Motivated by the stringent flux limits for UHE neutrinos coming from gamma ray burst or active galactic nuclei, we explore the possibility that the active neutrinos generated in such astrophysical objects could oscillate to sterile right handed states due to a neutrino magnetic moment mu_nu. We find that a value as small as mu_nu ~1E-15 [...]]]></description>
			<content:encoded><![CDATA[<p>Motivated by the stringent flux limits for UHE neutrinos coming from gamma ray burst or active galactic nuclei, we explore the possibility that the active neutrinos generated in such astrophysical objects could oscillate to sterile right handed states due to a neutrino magnetic moment mu_nu. We find that a value as small as mu_nu ~1E-15 mu_B could produce such a transition thanks to the intense magnetic fields that are expected in these objects.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/a-reduction-in-the-uhe-neutrino-flux-due-to-neutrino-spin-precession/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The universal density profile of the central region of dark matter haloes</title>
		<link>http://voxcharta.org/2012/05/21/the-universal-density-profile-of-the-central-region-of-dark-matter-haloes/</link>
		<comments>http://voxcharta.org/2012/05/21/the-universal-density-profile-of-the-central-region-of-dark-matter-haloes/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:50:11 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[body simulation]]></category>
		<category><![CDATA[central core]]></category>
		<category><![CDATA[cusp]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[density profile]]></category>
		<category><![CDATA[extent]]></category>
		<category><![CDATA[initial condition]]></category>
		<category><![CDATA[perturbation]]></category>
		<category><![CDATA[structure formation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/the-universal-density-profile-of-the-central-region-of-dark-matter-haloes/</guid>
		<description><![CDATA[We consider the density profile of the central region of dark matter haloes. It turns out that under very general conditions the profile is universal: it depends almost not at all on the properties of the initial perturbation and is very akin, but not identical, to the Einasto profile.   We estimate the size [...]]]></description>
			<content:encoded><![CDATA[<p>We consider the density profile of the central region of dark matter haloes. It turns out that under very general conditions the profile is universal: it depends almost not at all on the properties of the initial perturbation and is very akin, but not identical, to the Einasto profile.   We estimate the size of the &#8216;central core&#8217; of the distribution, i.e., the extent of the very central region with a respectively gentle profile, and show that the cusp formation is unlikely, even if the dark matter is cold. We also indicate that the density profile of the outer part ($r&gt;0.5 R_{vir}$) of the haloes significantly depends on the initial conditions and should not be universal, in contrast to the central area. All these results can be useful both to indirect search of the dark matter and to N-body simulations of the structure formation.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/the-universal-density-profile-of-the-central-region-of-dark-matter-haloes/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Modeling the Spatial Distribution of Neutron Stars in the Galaxy</title>
		<link>http://voxcharta.org/2012/05/21/modeling-the-spatial-distribution-of-neutron-stars-in-the-galaxy/</link>
		<comments>http://voxcharta.org/2012/05/21/modeling-the-spatial-distribution-of-neutron-stars-in-the-galaxy/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:49:52 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[galactic plane]]></category>
		<category><![CDATA[gamma function]]></category>
		<category><![CDATA[gravitational potential]]></category>
		<category><![CDATA[initial distribution]]></category>
		<category><![CDATA[initial velocity]]></category>
		<category><![CDATA[monte carlo simulation]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[progenitor]]></category>
		<category><![CDATA[radial dependence]]></category>
		<category><![CDATA[radial distribution]]></category>
		<category><![CDATA[radial expansion]]></category>
		<category><![CDATA[spatial distribution]]></category>
		<category><![CDATA[stars in the galaxy]]></category>
		<category><![CDATA[toru]]></category>
		<category><![CDATA[velocities]]></category>
		<category><![CDATA[velocity distribution]]></category>
		<category><![CDATA[vertical distribution]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/modeling-the-spatial-distribution-of-neutron-stars-in-the-galaxy/</guid>
		<description><![CDATA[In this paper we investigate the space and velocity distributions of old neutron stars (aged 109 to 1010 yr) in our Galaxy. Galactic old Neutron Stars (NSs) population fills a torus-like area extending to a few tens kiloparsecs above the galactic plane. The initial velocity distribution of NSs is not well known, in this work [...]]]></description>
			<content:encoded><![CDATA[<p>In this paper we investigate the space and velocity distributions of old neutron stars (aged 109 to 1010 yr) in our Galaxy. Galactic old Neutron Stars (NSs) population fills a torus-like area extending to a few tens kiloparsecs above the galactic plane. The initial velocity distribution of NSs is not well known, in this work we adopt a three component initial distribution, as given by the contribution of kick velocities, circular velocities and Maxwellian velocities. For the spatial initial distribution we use a Gamma function. We then use Monte Carlo simulations to follow the evolution of the NSs under the influence of the Paczy{\P}nski Galactic gravitational potential. Our calculations show that NS orbits have a very large Galactic radial expansion and that their radial distribution peak is quite close to their progenitors&#8217; one. We also study the NS vertical distribution and find that it can well be described by a double exponential low. Finally, we investigate the correlation of the vertical and radial distribution and study the radial dependence of scale-heights.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/modeling-the-spatial-distribution-of-neutron-stars-in-the-galaxy/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>AE Aquarii represents a new subclass of Cataclysmic Variables</title>
		<link>http://voxcharta.org/2012/05/21/ae-aquarii-represents-a-new-subclass-of-cataclysmic-variables/</link>
		<comments>http://voxcharta.org/2012/05/21/ae-aquarii-represents-a-new-subclass-of-cataclysmic-variables/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:49:20 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[aqr]]></category>
		<category><![CDATA[binary system]]></category>
		<category><![CDATA[cataclysmic variables]]></category>
		<category><![CDATA[diffusion]]></category>
		<category><![CDATA[dwarf surface]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[intermediate polars]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetic moment]]></category>
		<category><![CDATA[mass exchange]]></category>
		<category><![CDATA[missing link]]></category>
		<category><![CDATA[plasma]]></category>
		<category><![CDATA[red dwarf]]></category>
		<category><![CDATA[subclass]]></category>
		<category><![CDATA[system component]]></category>
		<category><![CDATA[transition]]></category>
		<category><![CDATA[white dwarf]]></category>

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

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

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/spectral-analysis-of-the-13-kev-feature-in-xte-j1810-197-implications-for-axp-models/</guid>
		<description><![CDATA[During 2003 and 2004 the Anomalous X-Ray Pulsar XTE J1810-197 went through a series of four bursts. The spectrum in the tail of one of these bursts shows a strong, significant emission feature ~13 keV, thereby encoding a wealth of information about the environment surrounding this object. In this paper we analyse this emission feature [...]]]></description>
			<content:encoded><![CDATA[<p>During 2003 and 2004 the Anomalous X-Ray Pulsar XTE J1810-197 went through a series of four bursts. The spectrum in the tail of one of these bursts shows a strong, significant emission feature ~13 keV, thereby encoding a wealth of information about the environment surrounding this object. In this paper we analyse this emission feature considering both cyclotron and atomic emission processes and weigh our findings against three leading AXP models: the Magnetar model, Fall-back disk model and the Quark nova model. We find that atomic emission from Rubidium within a Keplerian ring ($\sim$15 km from a compact object of $\sim 2M_\odot$) is the most consistent scenario with the observations, supporting the Quark nova model. Cyclotron emission from an atmosphere a few hundred meters thick also fits the feature well, but is ruled out on account of its positional coincidence in three separate AXP sources.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/spectral-analysis-of-the-13-kev-feature-in-xte-j1810-197-implications-for-axp-models/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Contributions to the cross shock electric field at supercritical perpendicular shocks: Impact of the pickup ions [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/21/contributions-to-the-cross-shock-electric-field-at-supercritical-perpendicular-shocks-impact-of-the-pickup-ions-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/21/contributions-to-the-cross-shock-electric-field-at-supercritical-perpendicular-shocks-impact-of-the-pickup-ions-cross-listing/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:48:23 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[gyro]]></category>
		<category><![CDATA[ion dynamics]]></category>
		<category><![CDATA[lorentz]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[pickup ions]]></category>
		<category><![CDATA[pis]]></category>
		<category><![CDATA[preliminary results]]></category>
		<category><![CDATA[ramp]]></category>
		<category><![CDATA[reformation]]></category>
		<category><![CDATA[shock]]></category>
		<category><![CDATA[shock front]]></category>
		<category><![CDATA[solar wind ions]]></category>
		<category><![CDATA[stationary foot]]></category>
		<category><![CDATA[striking point]]></category>

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

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/energy-dependent-orbital-modulation-of-x-rays-and-a-constraint-on-emission-of-the-jet-in-cyg-x-3/</guid>
		<description><![CDATA[We study orbital modulation of X-rays from Cyg X-3, using data from Swift, INTEGRAL and RXTE. Given the wealth of the presently available data and an improved calculation method, we obtain energy-dependent folded and averaged light curves with unprecedented accuracy. We find that above ~5 keV, the modulation depth decreases with the increasing energy, which [...]]]></description>
			<content:encoded><![CDATA[<p>We study orbital modulation of X-rays from Cyg X-3, using data from Swift, INTEGRAL and RXTE. Given the wealth of the presently available data and an improved calculation method, we obtain energy-dependent folded and averaged light curves with unprecedented accuracy. We find that above ~5 keV, the modulation depth decreases with the increasing energy, which is consistent with the modulation being caused by both bound-free absorption and Compton scattering in the stellar wind of the donor, with minima corresponding to the highest optical depth, which occurs around the superior conjunction. We find a decrease of the depth below ~3 keV, which appears to be due to re-emission of the absorbed continuum by the wind in soft X-ray lines. Based on the shape of the folded light curves, any X-ray contribution from the jet in Cyg X-3, which emits gamma-rays detected at energies $&gt;0.1$ GeV in soft spectral states, is found to be minor up to ~100 keV. We also calculate phase-resolved RXTE X-ray spectra, and show the difference between the spectra corresponding to phases around the superior and inferior conjunctions can indeed be accounted for by a combined effect of bound-free absorption in an ionized medium and Compton scattering.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/energy-dependent-orbital-modulation-of-x-rays-and-a-constraint-on-emission-of-the-jet-in-cyg-x-3/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>On energetics of particle collisions near black holes: BSW effect versus Penrose process [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/21/on-energetics-of-particle-collisions-near-black-holes-bsw-effect-versus-penrose-process-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/21/on-energetics-of-particle-collisions-near-black-holes-bsw-effect-versus-penrose-process-cross-listing/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:47:48 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[centre of mass]]></category>
		<category><![CDATA[dependence]]></category>
		<category><![CDATA[distant observer]]></category>
		<category><![CDATA[energetics]]></category>
		<category><![CDATA[energy particle]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[horizon]]></category>
		<category><![CDATA[mass frame]]></category>
		<category><![CDATA[particle collision]]></category>
		<category><![CDATA[penrose]]></category>
		<category><![CDATA[upper bound]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/on-energetics-of-particle-collisions-near-black-holes-bsw-effect-versus-penrose-process-cross-listing/</guid>
		<description><![CDATA[If two particles collide near the horizon of a rotating or charged black hole, under certain conditions the energy E_{c.m.} in the centre of mass frame can grow without limit (the so-called BSW effect). Let collision produce two another particles. We show that for an outgoing particle detected by a distant observer, there exist upper [...]]]></description>
			<content:encoded><![CDATA[<p>If two particles collide near the horizon of a rotating or charged black hole, under certain conditions the energy E_{c.m.} in the centre of mass frame can grow without limit (the so-called BSW effect). Let collision produce two another particles. We show that for an outgoing particle detected by a distant observer, there exist upper bounds on the mass and energy E_{out}. For a static charged black hole, the dependence of E_{out} on the energy E_{in} of an ingoing &#8220;critical&#8221; particle (responsible for the BSW effect) is decreasing. For neutral rotating black holes it is increasing but for the high-energy particles the ratio E_{out}/E_{in}&lt;1. As a result, the BSW effect is inconsistent with the Penrose process. The obtained results suggest astrophysical limits on possibility of observation of the products of the BSW effect. From the other hand, collisions with finite E_{c.m.} can produce particles with unbound ratio E_{out}/E_{in}.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/on-energetics-of-particle-collisions-near-black-holes-bsw-effect-versus-penrose-process-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A note on the observational evidence for the existence of event horizons in astrophysical black hole candidates [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/21/a-note-on-the-observational-evidence-for-the-existence-of-event-horizons-in-astrophysical-black-hole-candidates-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/21/a-note-on-the-observational-evidence-for-the-existence-of-event-horizons-in-astrophysical-black-hole-candidates-cross-listing/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:41:34 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[astrophysical observations]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[electromagnetic radiation]]></category>
		<category><![CDATA[event horizon]]></category>
		<category><![CDATA[existence]]></category>
		<category><![CDATA[hole candidate]]></category>
		<category><![CDATA[observation]]></category>
		<category><![CDATA[observational evidence]]></category>
		<category><![CDATA[universe today]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/a-note-on-the-observational-evidence-for-the-existence-of-event-horizons-in-astrophysical-black-hole-candidates-cross-listing/</guid>
		<description><![CDATA[Black holes have the peculiar and intriguing property of having an event horizon, a one-way membrane causally separating their internal region from the rest of the Universe. Today astrophysical observations provide some evidence for the existence of event horizons in astrophysical black hole candidates. In this short paper, I compare the constraint we can infer [...]]]></description>
			<content:encoded><![CDATA[<p>Black holes have the peculiar and intriguing property of having an event horizon, a one-way membrane causally separating their internal region from the rest of the Universe. Today astrophysical observations provide some evidence for the existence of event horizons in astrophysical black hole candidates. In this short paper, I compare the constraint we can infer from the non-observation of electromagnetic radiation from the putative surface of these objects with the bound coming from the ergoregion instability, pointing out the respective assumptions and limitations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/a-note-on-the-observational-evidence-for-the-existence-of-event-horizons-in-astrophysical-black-hole-candidates-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Spectral and spatial variations of the diffuse gamma-ray background in the vicinity of the Galactic plane and possible nature of the feature at 130 GeV</title>
		<link>http://voxcharta.org/2012/05/21/spectral-and-spatial-variations-of-the-diffuse-gamma-ray-background-in-the-vicinity-of-the-galactic-plane-and-possible-nature-of-the-feature-at-130-gev/</link>
		<comments>http://voxcharta.org/2012/05/21/spectral-and-spatial-variations-of-the-diffuse-gamma-ray-background-in-the-vicinity-of-the-galactic-plane-and-possible-nature-of-the-feature-at-130-gev/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:39:06 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[confidence]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[diffuse background]]></category>
		<category><![CDATA[dips]]></category>
		<category><![CDATA[excesses]]></category>
		<category><![CDATA[features change]]></category>
		<category><![CDATA[galactic center]]></category>
		<category><![CDATA[galactic plane]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[law component]]></category>
		<category><![CDATA[shape]]></category>
		<category><![CDATA[sky]]></category>
		<category><![CDATA[smooth power]]></category>
		<category><![CDATA[spatial variation]]></category>
		<category><![CDATA[spectral feature]]></category>
		<category><![CDATA[spectrum]]></category>
		<category><![CDATA[vicinity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/spectral-and-spatial-variations-of-the-diffuse-gamma-ray-background-in-the-vicinity-of-the-galactic-plane-and-possible-nature-of-the-feature-at-130-gev/</guid>
		<description><![CDATA[We study the properties of the diffuse gamma-ray background around the Galactic plane at energies 60 &#8211; 200 GeV. We find that the spectrum of this emission possesses spacial variations having significant features (excesses and dips) as compared to the average smooth (power law) component. The positions and shapes of these spectral features change with [...]]]></description>
			<content:encoded><![CDATA[<p>We study the properties of the diffuse gamma-ray background around the Galactic plane at energies 60 &#8211; 200 GeV. We find that the spectrum of this emission possesses spacial variations having significant features (excesses and dips) as compared to the average smooth (power law) component. The positions and shapes of these spectral features change with direction on the sky. We therefore argue, that the spectral feature around 130 GeV, found in several regions around the Galactic Center and the Galactic plane in [1204.2797,1205.1045], can not be interpreted with confidence as a gamma-ray line, but may be a component of the diffuse background and can be of instrumental or astrophysical origin. Therefore, the dark matter origin of this spectral feature becomes dubious.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/spectral-and-spatial-variations-of-the-diffuse-gamma-ray-background-in-the-vicinity-of-the-galactic-plane-and-possible-nature-of-the-feature-at-130-gev/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>X-Ray And Optical Flux Ratio Anomalies In Quadruply Lensed Quasars. II. Mapping the Dark Matter Content in Elliptical Galaxies [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/x-ray-and-optical-flux-ratio-anomalies-in-quadruply-lensed-quasars-ii-mapping-the-dark-matter-content-in-elliptical-galaxies-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/x-ray-and-optical-flux-ratio-anomalies-in-quadruply-lensed-quasars-ii-mapping-the-dark-matter-content-in-elliptical-galaxies-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:38:41 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[anomaly]]></category>
		<category><![CDATA[bayesian analysis]]></category>
		<category><![CDATA[chandra observation]]></category>
		<category><![CDATA[dark matter content]]></category>
		<category><![CDATA[elliptical galaxy]]></category>
		<category><![CDATA[ensembles]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[impact parameter]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[lensed quasar]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[optical flux]]></category>
		<category><![CDATA[quasar images]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/x-ray-and-optical-flux-ratio-anomalies-in-quadruply-lensed-quasars-ii-mapping-the-dark-matter-content-in-elliptical-galaxies-replacement/</guid>
		<description><![CDATA[We present a microlensing analysis of 61 Chandra observations of 14 quadruply lensed quasars. X-ray flux measurements of the individual quasar images give a clean determination of the microlensing effects in the lensing galaxy and thus offer a direct assessment of the local fraction of stellar matter making up the total integrated mass along the [...]]]></description>
			<content:encoded><![CDATA[<p>We present a microlensing analysis of 61 Chandra observations of 14 quadruply lensed quasars. X-ray flux measurements of the individual quasar images give a clean determination of the microlensing effects in the lensing galaxy and thus offer a direct assessment of the local fraction of stellar matter making up the total integrated mass along the lines of sight through the lensing galaxy. A Bayesian analysis of the ensemble of lensing galaxies gives a most likely local stellar fraction of 7%, with the other 93% in a smooth, dark matter component, at an average impact parameter R_c of 6.6 kpc from the center of the lensing galaxy. We divide the systems into smaller ensembles based on R_c and find that the most likely local stellar fraction varies qualitatively and quantitatively as expected, decreasing as a function of R_c.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/x-ray-and-optical-flux-ratio-anomalies-in-quadruply-lensed-quasars-ii-mapping-the-dark-matter-content-in-elliptical-galaxies-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Constraining neutrino superluminality from searches for sterile neutrino decays [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/constraining-neutrino-superluminality-from-searches-for-sterile-neutrino-decays-replacement-2/</link>
		<comments>http://voxcharta.org/2012/05/21/constraining-neutrino-superluminality-from-searches-for-sterile-neutrino-decays-replacement-2/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:36:10 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absence]]></category>
		<category><![CDATA[cern]]></category>
		<category><![CDATA[energy range]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[opera]]></category>
		<category><![CDATA[pair production]]></category>
		<category><![CDATA[signature]]></category>
		<category><![CDATA[sn1987a]]></category>
		<category><![CDATA[sterile neutrino]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/constraining-neutrino-superluminality-from-searches-for-sterile-neutrino-decays-replacement-2/</guid>
		<description><![CDATA[Superluminal neutrinos are expected to lose energy due to bremstrauhlung. It is dominated by e+e&#8211;pair production if kinematically allowed. The same signature was used in searches for 3-body decays of hypothetical heavy sterile neutrinos. From the absence of these processes in CERN PS191 and CHARM experiments we set upper limits on the neutrino velocity in [...]]]></description>
			<content:encoded><![CDATA[<p>Superluminal neutrinos are expected to lose energy due to bremstrauhlung. It is dominated by e+e&#8211;pair production if kinematically allowed. The same signature was used in searches for 3-body decays of hypothetical heavy sterile neutrinos. From the absence of these processes in CERN PS191 and CHARM experiments we set upper limits on the neutrino velocity in the energy range from 0.2 GeV to 280 GeV. Our limits are well below the neutrino velocity favored by the recent OPERA results. For energy-independent neutrino velocity the limits obtained in this paper are stronger than those coming from ICARUS experiment and observations of Supernova SN1987a.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/constraining-neutrino-superluminality-from-searches-for-sterile-neutrino-decays-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Acceleration of particles by black holes as a result of deceleration: ultimate manifestation of kinematic nature of BSW effect [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/acceleration-of-particles-by-black-holes-as-a-result-of-deceleration-ultimate-manifestation-of-kinematic-nature-of-bsw-effect-replacement-2/</link>
		<comments>http://voxcharta.org/2012/05/21/acceleration-of-particles-by-black-holes-as-a-result-of-deceleration-ultimate-manifestation-of-kinematic-nature-of-bsw-effect-replacement-2/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:34:40 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[deceleration]]></category>
		<category><![CDATA[horizon surface]]></category>
		<category><![CDATA[manifestation]]></category>
		<category><![CDATA[mass frame]]></category>
		<category><![CDATA[massive particle]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[repulsion]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/acceleration-of-particles-by-black-holes-as-a-result-of-deceleration-ultimate-manifestation-of-kinematic-nature-of-bsw-effect-replacement-2/</guid>
		<description><![CDATA[The recently discovered so-called BSW effect consists in the unbound growth of the energy E_{c.m.} in the centre of mass frame of two colliding particles near the black hole horizon. We consider a new type of the corresponding scenario when one of two particles (&#8220;critical&#8221;) remains at rest near the horizon of the charged near-extremal [...]]]></description>
			<content:encoded><![CDATA[<p>The recently discovered so-called BSW effect consists in the unbound growth of the energy E_{c.m.} in the centre of mass frame of two colliding particles near the black hole horizon. We consider a new type of the corresponding scenario when one of two particles (&#8220;critical&#8221;) remains at rest near the horizon of the charged near-extremal black hole due to balance between the attractive and repulsion forces. The other one hits it with a speed close to that of light. This scenario shows in a most pronounced way the kinematic nature of the BSW effect. In the extremal limit, one would gain formally infinite E_{c.m.} but this does not happen since it would have require the critical massive particle to remain at rest on the null horizon surface that is impossible. We also discuss the BSW effect in the metric of the extremal Reissner-Nordstr\&#8221;om black hole when the critical particle remains at rest near the horizon.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/acceleration-of-particles-by-black-holes-as-a-result-of-deceleration-ultimate-manifestation-of-kinematic-nature-of-bsw-effect-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<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>The Nature of the Compton-thick X-ray Reprocessor in NGC 4945 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/the-nature-of-the-compton-thick-x-ray-reprocessor-in-ngc-4945-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/the-nature-of-the-compton-thick-x-ray-reprocessor-in-ngc-4945-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:32:43 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[agns]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[Chandra]]></category>
		<category><![CDATA[cm 2]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[compton]]></category>
		<category><![CDATA[continuum]]></category>
		<category><![CDATA[eddington luminosity]]></category>
		<category><![CDATA[Fermi]]></category>
		<category><![CDATA[galaxy ngc]]></category>
		<category><![CDATA[line emission]]></category>
		<category><![CDATA[methodology]]></category>
		<category><![CDATA[orders of magnitude]]></category>
		<category><![CDATA[reflection model]]></category>
		<category><![CDATA[restriction]]></category>
		<category><![CDATA[shape]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectrum]]></category>
		<category><![CDATA[variability]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/the-nature-of-the-compton-thick-x-ray-reprocessor-in-ngc-4945-replacement/</guid>
		<description><![CDATA[We present an exhaustive methodology for fitting Compton-thick X-ray reprocessor models to obscured AGNs and for interpreting the results. We focus on the MYTORUS model but also utilize other models. We apply the techniques to Suzaku, BeppoSAX, and Swift BAT spectra of the Sy 2 galaxy NGC 4945, but the methods are applicable to other [...]]]></description>
			<content:encoded><![CDATA[<p>We present an exhaustive methodology for fitting Compton-thick X-ray reprocessor models to obscured AGNs and for interpreting the results. We focus on the MYTORUS model but also utilize other models. We apply the techniques to Suzaku, BeppoSAX, and Swift BAT spectra of the Sy 2 galaxy NGC 4945, but the methods are applicable to other AGNs including Compton-thin sources. The models overcome a major restriction of disk-reflection models, namely the assumption of an infinite column density. Finite column-density models produce a richer variety of spectral shapes and characteristics, even for Compton-thin AGNs. Although NGC 4945 is one of the brightest AGNs above 10 keV, the models span nearly a factor of 3 in column density (~2 to 6 x 10^{24} cm^{-2}) and 2 orders of magnitude in the intrinsic 2-195 keV luminosity. Models in which the continuum above 10 keV is dominated by the direct (unscattered) continuum or Compton-scattered continuum give the highest and lowest intrinsic luminosities respectively. Variability properties favor solutions in which the unscattered continuum dominates above 10 keV. The data require that the Compton-scattered continuum and Fe Kalpha line emission come predominantly from the illuminated surfaces of the X-ray reprocessor, implying a clumpy medium with a global covering factor that is small enough that the Compton-scattered continuum does not dominate the spectrum above 10 keV. This can be identified with the ~30 pc region spatially resolved by Chandra. The implied intrinsic bolometric luminosity is close to, or greater than, the Eddington luminosity. However, a strongly beamed AGN embedded in a shell of Compton-thick (but clumpy) matter requires less fine-tuning of the covering factor. Beaming is consistent with recent radio and Fermi results. Such beamed Compton-thick AGNs would be preferentially selected in surveys over unbeamed Compton-thick AGNs.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/the-nature-of-the-compton-thick-x-ray-reprocessor-in-ngc-4945-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>High energy gamma-ray emission from compact galactic sources in the context of observations with the next generation Cherenkov Telescope Arrays [Replacement]</title>
		<link>http://voxcharta.org/2012/05/21/high-energy-gamma-ray-emission-from-compact-galactic-sources-in-the-context-of-observations-with-the-next-generation-cherenkov-telescope-arrays-replacement/</link>
		<comments>http://voxcharta.org/2012/05/21/high-energy-gamma-ray-emission-from-compact-galactic-sources-in-the-context-of-observations-with-the-next-generation-cherenkov-telescope-arrays-replacement/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:32:03 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[compact object]]></category>
		<category><![CDATA[cta]]></category>
		<category><![CDATA[energetic particle]]></category>
		<category><![CDATA[energy range]]></category>
		<category><![CDATA[galactic sources]]></category>
		<category><![CDATA[gamma ray emission]]></category>
		<category><![CDATA[gev energy]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[hypothesis]]></category>
		<category><![CDATA[observational result]]></category>
		<category><![CDATA[order of magnitude]]></category>
		<category><![CDATA[physical processes]]></category>
		<category><![CDATA[ray astronomy]]></category>
		<category><![CDATA[ray sources]]></category>
		<category><![CDATA[telescope array]]></category>
		<category><![CDATA[telescopes]]></category>
		<category><![CDATA[tev energies]]></category>
		<category><![CDATA[theoretical implications]]></category>
		<category><![CDATA[time resolution]]></category>
		<category><![CDATA[unexpected feature]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/high-energy-gamma-ray-emission-from-compact-galactic-sources-in-the-context-of-observations-with-the-next-generation-cherenkov-telescope-arrays-replacement/</guid>
		<description><![CDATA[The observational progress in the $\gamma$-ray astronomy in the last few years has led to the discovery of more than a thousand sources at GeV energies and more than a hundred sources at TeV energies. A few different classes of compact objects in the Galaxy have been established. They show many unexpected features at high [...]]]></description>
			<content:encoded><![CDATA[<p>The observational progress in the $\gamma$-ray astronomy in the last few years has led to the discovery of more than a thousand sources at GeV energies and more than a hundred sources at TeV energies. A few different classes of compact objects in the Galaxy have been established. They show many unexpected features at high energies the physics of which remains mainly unknown. At present it is clear that detailed investigation of these new phenomena can be performed only with the technical equipment which offer an order of magnitude better sensitivity, and a few times better energy, angular and time resolution in the broad energy range staring from a few tens of GeV up to a few hundreds TeV. Such facilities can be realized by the next generation of instruments such as the planned Cherenkov Telescope Array (CTA).   The aim of this report is to summarize up to date observational results on the compact galactic sources in the GeV-TeV $\gamma$-ray energy range, discuss their theoretical implications, and indicate which hypothesis considered at present might be verified with the next generation of telescopes. We point out which of the observational features of the $\gamma$-ray sources are important to investigate with special care with the planned CTA in order to put a new light on physical processes involved. Their knowledge should finally allow us to answer the question on the origin of energetic particles in our Galaxy.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/high-energy-gamma-ray-emission-from-compact-galactic-sources-in-the-context-of-observations-with-the-next-generation-cherenkov-telescope-arrays-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Observing Black Holes: Quasi-Periodic Oscillations [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/21/observing-black-holes-quasi-periodic-oscillations-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/21/observing-black-holes-quasi-periodic-oscillations-cross-listing/#comments</comments>
		<pubDate>Tue, 22 May 2012 00:31:05 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[angular momentum]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[circular orbit]]></category>
		<category><![CDATA[existence]]></category>
		<category><![CDATA[frequency qpos]]></category>
		<category><![CDATA[fundamental frequency]]></category>
		<category><![CDATA[general relativity]]></category>
		<category><![CDATA[gravity]]></category>
		<category><![CDATA[high frequency]]></category>
		<category><![CDATA[kerr]]></category>
		<category><![CDATA[maxima]]></category>
		<category><![CDATA[numerical analysis]]></category>
		<category><![CDATA[observable effects]]></category>
		<category><![CDATA[orbital frequency]]></category>
		<category><![CDATA[periodic oscillation]]></category>
		<category><![CDATA[qualitative agreement]]></category>
		<category><![CDATA[spacetime geometry]]></category>
		<category><![CDATA[stable orbit]]></category>
		<category><![CDATA[twin peak]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/21/observing-black-holes-quasi-periodic-oscillations-cross-listing/</guid>
		<description><![CDATA[The twin peaks high-frequency quasiperiodic oscillations (QPOs), which are observed in a number of black hole binaries, can be related to the epicyclic frequencies of the geodesic motion, thereby providing a testing ground for the spacetime geometry near the black holes. In this paper, we explore some observable effects of the geodesic motion in the [...]]]></description>
			<content:encoded><![CDATA[<p>The twin peaks high-frequency quasiperiodic oscillations (QPOs), which are observed in a number of black hole binaries, can be related to the epicyclic frequencies of the geodesic motion, thereby providing a testing ground for the spacetime geometry near the black holes. In this paper, we explore some observable effects of the geodesic motion in the spacetime of rotating black holes in general relativity and braneworld gravity. We focus on the description of the motion in terms of three fundamental frequencies: the orbital frequency, the radial and vertical epicyclic frequencies. For a Kerr black hole, we perform a detailed numerical analysis of these frequencies at the innermost stable circular orbits and beyond them as well as at the characteristic stable orbits, for which the radial epicyclic frequency attains its highest value. We find that the values of the radial and vertical epicyclic frequencies at particular orbits are in good qualitative agreement with the observed frequencies of the twin peaks QPOs in some black hole binaries. It is interesting that at the characteristic stable circular orbits, where the radial epicyclic frequency has maxima, the vertical and radial epicyclic frequencies exhibit an approximate 2 : 1 ratio even in the case of near-extreme rotation of the black hole. We also perform a similar analysis of the fundamental frequencies for a rotating braneworld black hole and argue that the existence of such a black hole with a negative tidal charge, whose angular momentum exceeds the Kerr bound in general relativity, does not confront with the observations of high frequency QPOs.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/21/observing-black-holes-quasi-periodic-oscillations-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Medium modification of the charged current neutrino opacity and its implications</title>
		<link>http://voxcharta.org/2012/05/20/medium-modification-of-the-charged-current-neutrino-opacity-and-its-implications/</link>
		<comments>http://voxcharta.org/2012/05/20/medium-modification-of-the-charged-current-neutrino-opacity-and-its-implications/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:39:50 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[antineutrino]]></category>
		<category><![CDATA[boltzmann equation]]></category>
		<category><![CDATA[closer to one]]></category>
		<category><![CDATA[collisional]]></category>
		<category><![CDATA[cross section]]></category>
		<category><![CDATA[driven wind]]></category>
		<category><![CDATA[electron neutrino]]></category>
		<category><![CDATA[interaction rate]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[neutrino interaction]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[nucleon]]></category>
		<category><![CDATA[nucleosynthesis]]></category>
		<category><![CDATA[opacity]]></category>
		<category><![CDATA[particle energy]]></category>
		<category><![CDATA[period of time]]></category>
		<category><![CDATA[proto]]></category>
		<category><![CDATA[proton]]></category>
		<category><![CDATA[symmetry]]></category>
		<category><![CDATA[vector]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/medium-modification-of-the-charged-current-neutrino-opacity-and-its-implications/</guid>
		<description><![CDATA[Previous work on neutrino emission from proto-neutron stars which employed full solutions of the Boltzmann equation showed that the average energies of emitted electron neutrinos and antineutrinos are closer to one another than predicted by older, more approximate work. This in turn implied that the neutrino driven wind is proton rich during its entire life, [...]]]></description>
			<content:encoded><![CDATA[<p>Previous work on neutrino emission from proto-neutron stars which employed full solutions of the Boltzmann equation showed that the average energies of emitted electron neutrinos and antineutrinos are closer to one another than predicted by older, more approximate work. This in turn implied that the neutrino driven wind is proton rich during its entire life, precluding $r$-process nucleosynthesis and the synthesis of Sr, Y, and Zr. This work relied on charged current neutrino interaction rates that are appropriate for a free nucleon gas. Here, it is shown in detail that the inclusion of the nucleon potential energies and collisional broadening of the response significantly alters this conclusion. Iso-vector interactions, which give rise to the nuclear symmetry energy, produce a difference between neutron and proton single-particle energies $\Delta U=U_n-U_p$ and alter the kinematics of the charged current reaction. In neutron-rich matter, and for a given neutrino/antineutrino energy, the rate for $\nu_e+n\rightarrow e^-+p$ is enhanced while $ \bar{\nu}_e+p\rightarrow n+e^+$ is suppressed because the $Q$ value for these reactions is altered by $\pm\Delta U$, respectively. Collisional broadening acts to enhance both $\nu_e$ and $\bar{\nu}_e$ cross-sections, but mean field shifts have a larger effect. Therefore, electron neutrinos decouple at lower temperature than when the nucleons are assumed to be free and have lower average energies. The change is large enough to allow for a reasonable period of time when the neutrino driven wind is predicted to be neutron rich. It is also shown that the electron fraction in the wind is influenced by the nuclear symmetry energy.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/medium-modification-of-the-charged-current-neutrino-opacity-and-its-implications/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>GRB980923. A burst with a short duration high energy component</title>
		<link>http://voxcharta.org/2012/05/20/grb980923-a-burst-with-a-short-duration-high-energy-component/</link>
		<comments>http://voxcharta.org/2012/05/20/grb980923-a-burst-with-a-short-duration-high-energy-component/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:39:24 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[burst]]></category>
		<category><![CDATA[clear evidence]]></category>
		<category><![CDATA[duration]]></category>
		<category><![CDATA[egret]]></category>
		<category><![CDATA[energy component]]></category>
		<category><![CDATA[gamma ray burst]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[keV]]></category>
		<category><![CDATA[lad]]></category>
		<category><![CDATA[light curve]]></category>
		<category><![CDATA[observation]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[sim 2]]></category>
		<category><![CDATA[spectral components]]></category>
		<category><![CDATA[spectral index]]></category>
		<category><![CDATA[spectrum]]></category>
		<category><![CDATA[tasc]]></category>
		<category><![CDATA[variability]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/grb980923-a-burst-with-a-short-duration-high-energy-component/</guid>
		<description><![CDATA[The prompt emission of Gamma Ray Bursts (GRBs) is usually well described by the Band function: two power-laws joined smoothly at a given break energy. In addition to the Band component, a few bursts (GRB941017, GRB090510, GRB090902B and GRB090926A) show clear evidence for a distinct high-energy spectral component, which in some cases evolves independently from [...]]]></description>
			<content:encoded><![CDATA[<p>The prompt emission of Gamma Ray Bursts (GRBs) is usually well described by the Band function: two power-laws joined smoothly at a given break energy. In addition to the Band component, a few bursts (GRB941017, GRB090510, GRB090902B and GRB090926A) show clear evidence for a distinct high-energy spectral component, which in some cases evolves independently from the prompt keV component and is well described by a power-law (PL), sometimes with a cut-off energy; this component is found to have long duration, even longer than the burst itself for all the four bursts. Here we report the observation of an anomalous short duration high energy component in GRB980923. GRB980923 is one of the brightest Gamma-Ray Bursts (GRBs) observed by BATSE. Its light curve is characterized by a rapid variability phase lasting \sim 40 s, followed by a smooth emission tail lasting \sim 400 s. A detailed joint analysis of BATSE (LAD and SD) and EGRET TASC data of GRB980923 reveles the presence of an anomalous keV to MeV component in the spectrum that evolves independently from the prompt keV one. This component is well described by a PL with a spectral index of 1.44 and lasts only \sim 2 s; it represents one of the three clearly separated spectral components identified in GRB980923, the other two being the keV prompt emission, well described by the Band function and the tail, well fit by a Smoothly Broken Power Law (SBPL).</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/grb980923-a-burst-with-a-short-duration-high-energy-component/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Three-Dimensional Explosion Geometry of Stripped-Envelope Core-Collapse Supernovae. I. Spectropolarimetric Observations</title>
		<link>http://voxcharta.org/2012/05/20/three-dimensional-explosion-geometry-of-stripped-envelope-core-collapse-supernovae-i-spectropolarimetric-observations/</link>
		<comments>http://voxcharta.org/2012/05/20/three-dimensional-explosion-geometry-of-stripped-envelope-core-collapse-supernovae-i-spectropolarimetric-observations/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:38:33 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[core collapse supernovae]]></category>
		<category><![CDATA[dispersion]]></category>
		<category><![CDATA[distributions]]></category>
		<category><![CDATA[ejecta]]></category>
		<category><![CDATA[explosion]]></category>
		<category><![CDATA[polarization]]></category>
		<category><![CDATA[SNe]]></category>
		<category><![CDATA[three dimensional geometry]]></category>
		<category><![CDATA[type ic]]></category>
		<category><![CDATA[wavelength]]></category>

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

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/130-gev-gamma-ray-line-from-dark-matter-decay-cross-listing/</guid>
		<description><![CDATA[The 130 GeV gamma-ray line based on tentative analyses on the Fermi-LAT data is hard to be understood with dark matter annihilation in the conventional framework of the MSSM. We point out that it can be nicely explained with two body decay of a scalar dark matter ($\tilde{\phi}_{\rm DM}\rightarrow\gamma\gamma$) by the dimension 6 operator suppressed [...]]]></description>
			<content:encoded><![CDATA[<p>The 130 GeV gamma-ray line based on tentative analyses on the Fermi-LAT data is hard to be understood with dark matter annihilation in the conventional framework of the MSSM. We point out that it can be nicely explained with two body decay of a scalar dark matter ($\tilde{\phi}_{\rm DM}\rightarrow\gamma\gamma$) by the dimension 6 operator suppressed with the mass of the grand unification scale ($\sim 10^{16}$ GeV), ${\cal L}\supset|\tilde{\phi}_{\rm DM}|^2F_{\mu\nu}F^{\mu\nu}/M_{\rm GUT}^2$, in which the scalar dark matter $\tilde{\phi}_{\rm DM}$ develops a TeV scale vacuum expectation value. We propose a viable model, which can explain the 130 GeV gamma-ray line and also the abundance of $\tilde{\phi}_{\rm DM}$.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/130-gev-gamma-ray-line-from-dark-matter-decay-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A Suzaku Study of Ejecta Structure and Origin of Hard X-ray Emission in the Supernova Remnant G156.2+5.7</title>
		<link>http://voxcharta.org/2012/05/20/a-suzaku-study-of-ejecta-structure-and-origin-of-hard-x-ray-emission-in-the-supernova-remnant-g156-25-7/</link>
		<comments>http://voxcharta.org/2012/05/20/a-suzaku-study-of-ejecta-structure-and-origin-of-hard-x-ray-emission-in-the-supernova-remnant-g156-25-7/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:37:10 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cluster of galaxies]]></category>
		<category><![CDATA[diameter]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[element]]></category>
		<category><![CDATA[equilibrium]]></category>
		<category><![CDATA[extent]]></category>
		<category><![CDATA[ism]]></category>
		<category><![CDATA[radial structure]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[robust evidence]]></category>
		<category><![CDATA[shock]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[supernova remnant]]></category>
		<category><![CDATA[thermal emission]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/a-suzaku-study-of-ejecta-structure-and-origin-of-hard-x-ray-emission-in-the-supernova-remnant-g156-25-7/</guid>
		<description><![CDATA[We report an X-ray study of the evolved Galactic supernova remnant (SNR) G156.2+5.7 based on six pointing observations with Suzaku. The remnant&#8217;s large extent (100$\arcmin$ in diameter) allows us to investigate its radial structure in the northwestern and eastern directions from the apparent center. The X-ray spectra were well fit with a two-component non-equilibrium ionization [...]]]></description>
			<content:encoded><![CDATA[<p>We report an X-ray study of the evolved Galactic supernova remnant (SNR) G156.2+5.7 based on six pointing observations with Suzaku. The remnant&#8217;s large extent (100$\arcmin$ in diameter) allows us to investigate its radial structure in the northwestern and eastern directions from the apparent center. The X-ray spectra were well fit with a two-component non-equilibrium ionization model representing the swept-up interstellar medium (ISM) and the metal-rich ejecta. We found prominent central concentrations of Si, S and Fe from the ejecta component; the lighter elements of O, Ne and Mg were distributed more uniformly. The temperature of the ISM component suggests a slow shock (610-960 km s$^{-1}$), hence the remnant&#8217;s age is estimated to be 7,000-15,000 yr, assuming its distance to be $\sim$1.1 kpc. G156.2+5.7 has also been thought to emit hard, non-thermal X-rays, despite being considerably older than any other such remnant. In response to a recent discovery of a background cluster of galaxies (2XMM J045637.2+522411), we carefully excluded its contribution, and reexamined the origin of the hard X-ray emission. We found that the residual hard X-ray emission is consistent with the expected level of the cosmic X-ray background. Thus, no robust evidence for the non-thermal emission was obtained from G156.2+5.7. These results are consistent with the picture of an evolved SNR.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/a-suzaku-study-of-ejecta-structure-and-origin-of-hard-x-ray-emission-in-the-supernova-remnant-g156-25-7/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Regulation of Black Hole Winds and Jets Across the Mass Scale</title>
		<link>http://voxcharta.org/2012/05/20/regulation-of-black-hole-winds-and-jets-across-the-mass-scale/</link>
		<comments>http://voxcharta.org/2012/05/20/regulation-of-black-hole-winds-and-jets-across-the-mass-scale/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:36:36 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[eddington]]></category>
		<category><![CDATA[energetics]]></category>
		<category><![CDATA[grating]]></category>
		<category><![CDATA[hole accretion]]></category>
		<category><![CDATA[hole mass]]></category>
		<category><![CDATA[ionization]]></category>
		<category><![CDATA[jet power]]></category>
		<category><![CDATA[jet production]]></category>
		<category><![CDATA[mass scale]]></category>
		<category><![CDATA[mechanical power]]></category>
		<category><![CDATA[outflow velocity]]></category>
		<category><![CDATA[possible connection]]></category>
		<category><![CDATA[snr]]></category>
		<category><![CDATA[uniform analysis]]></category>
		<category><![CDATA[wind power]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/regulation-of-black-hole-winds-and-jets-across-the-mass-scale/</guid>
		<description><![CDATA[We present a study of the mechanical power generated by both winds and jets across the black hole mass scale. We begin with the study of ionized X-ray winds and present a uniform analysis using Chandra grating spectra. The high quality grating spectra facilitate the characterization of the outflow velocity, ionization and column density of [...]]]></description>
			<content:encoded><![CDATA[<p>We present a study of the mechanical power generated by both winds and jets across the black hole mass scale. We begin with the study of ionized X-ray winds and present a uniform analysis using Chandra grating spectra. The high quality grating spectra facilitate the characterization of the outflow velocity, ionization and column density of the absorbing gas. We find that the kinetic power of the winds scales with increasing bolometric luminosity as log(L_wind) \propto (1.57 \pm 0.07) log(L_Bol). This means that SMBH may be more efficient than stellar-mass black holes in launching winds. In addition, the simplicity of the scaling may suggest common driving mechanisms across the mass scale. For comparison, we next examine jet production, estimating jet power based on the energy required to inflate local bubbles. The jet relation is log(L_Jet)\propto (1.18\pm0.24) log(L_Bol). The energetics of the bubble associated with Cygnus X-1 are particularly difficult to determine, and the bubble could be a background SNR. If we exclude Cygnus X-1, then the jets follow a consistent relation to the winds within errors but with a higher normalization, log(L_Jet) \propto (1.34 \pm 0.50) log(L_Bol). The formal consistency in the wind and jet scaling relations suggests that a common launching mechanism may drive both flows; magnetic processes are viable possibilities. We also examine winds with especially high velocities, v &gt; 0.01c. These ultra-fast outflows tend to resemble the jets more than the winds, indicating we may be observing a regime in which winds become jets. This study allows for the total power from black hole accretion, both mechanical and radiative, to be characterized in a simple manner and suggests a possible connection between winds and jets. Finally, we find at low Eddington fractions, the jet power is dominant, and at high Eddington fractions the wind power is dominant.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/regulation-of-black-hole-winds-and-jets-across-the-mass-scale/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Supernova 1998S at 14 years Postmortem: Continuing CSM Interaction and Dust Formation [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/supernova-1998s-at-14-years-postmortem-continuing-csm-interaction-and-dust-formation-replacement/</link>
		<comments>http://voxcharta.org/2012/05/20/supernova-1998s-at-14-years-postmortem-continuing-csm-interaction-and-dust-formation-replacement/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:32:58 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[Solar and Stellar]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[centroid]]></category>
		<category><![CDATA[circumstellar material]]></category>
		<category><![CDATA[clump]]></category>
		<category><![CDATA[dust extinction]]></category>
		<category><![CDATA[dust formation]]></category>
		<category><![CDATA[emission features]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[large binocular telescope]]></category>
		<category><![CDATA[last decade]]></category>
		<category><![CDATA[optical spectrum]]></category>
		<category><![CDATA[oxygen profiles]]></category>
		<category><![CDATA[radial distribution]]></category>
		<category><![CDATA[red supergiant]]></category>
		<category><![CDATA[red wing]]></category>
		<category><![CDATA[SNe]]></category>
		<category><![CDATA[strong wind]]></category>
		<category><![CDATA[type iin]]></category>
		<category><![CDATA[wavelength dependence]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/supernova-1998s-at-14-years-postmortem-continuing-csm-interaction-and-dust-formation-replacement/</guid>
		<description><![CDATA[We report late-time spectroscopic observations of the Type IIn SN 1998S, taken 14 years after explosion using the Large Binocular Telescope. The optical spectrum exhibits broad emission features of [O I], [O II], [O III], H-alpha, H-beta, and [Fe II]. The last decade of evolution has exhibited a strengthening of the oxygen transitions, evidence that [...]]]></description>
			<content:encoded><![CDATA[<p>We report late-time spectroscopic observations of the Type IIn SN 1998S, taken 14 years after explosion using the Large Binocular Telescope. The optical spectrum exhibits broad emission features of [O I], [O II], [O III], H-alpha, H-beta, and [Fe II]. The last decade of evolution has exhibited a strengthening of the oxygen transitions, evidence that the late-time emission is powered by increasingly metal-rich SN ejecta crossing the reverse shock. The H-alpha luminosity requires that SN 1998S is still interacting with dense circumstellar material (CSM), probably produced by the strong wind of a red supergiant progenitor at least ~1000 years before explosion. The emission lines exhibit asymmetric blueshifted profiles, which implies that the receding hemisphere of the SN is obscured by dust. The [O III] line, in particular, exhibits a complete suppression of its red wing. This could be the result of the expected wavelength dependence for dust extinction or a smaller radial distribution for [O III]. In the latter case, the red wing of [O III] could be absorbed by core dust, while both the blue and red wings are absorbed by dust within the cool dense shell between the forward and reverse shocks; this interpretation could explain why late-time [O III] emission from SNe is often weaker than models predict. The [O I] line exhibits double-peaked structure on top of the broader underlying profile, possibly due to emission from individual clumps of ejecta or ring-like structures of metal-rich debris. The centroids of the peaks are blueshifted and lack a red counterpart. However, an archival spectrum obtained on day 1093 exhibits a third, redshifted peak, which we suspect has become extinguished by dust that formed over the last decade. This implies that the &#8220;missing&#8221; red components of multi-peaked oxygen profiles observed in other SNe might be obscured by varying degrees of dust extinction.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/supernova-1998s-at-14-years-postmortem-continuing-csm-interaction-and-dust-formation-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The parsec-scale jet of PKS 1749+096 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/20/the-parsec-scale-jet-of-pks-1749096-replacement/</link>
		<comments>http://voxcharta.org/2012/05/20/the-parsec-scale-jet-of-pks-1749096-replacement/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:32:22 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bimodal distribution]]></category>
		<category><![CDATA[bl lac objects]]></category>
		<category><![CDATA[coincidence]]></category>
		<category><![CDATA[distinct component]]></category>
		<category><![CDATA[doppler]]></category>
		<category><![CDATA[epochs]]></category>
		<category><![CDATA[flare]]></category>
		<category><![CDATA[high resolution]]></category>
		<category><![CDATA[inverse compton]]></category>
		<category><![CDATA[jet parameters]]></category>
		<category><![CDATA[kinematic]]></category>
		<category><![CDATA[lorentz factor]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[morphology]]></category>
		<category><![CDATA[motion]]></category>
		<category><![CDATA[new jet]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectral property]]></category>
		<category><![CDATA[target]]></category>
		<category><![CDATA[variability]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/the-parsec-scale-jet-of-pks-1749096-replacement/</guid>
		<description><![CDATA[PKS 1749+096 is a BL Lac object showing weak extended jet emission to the northeast of the compact VLBI core on parsec scales. We aim at better understanding the jet kinematics and variability of this source and finding clues that may applicable to other BL Lac objects. The jet was studied with multi-epoch multi-frequency high-resolution [...]]]></description>
			<content:encoded><![CDATA[<p>PKS 1749+096 is a BL Lac object showing weak extended jet emission to the northeast of the compact VLBI core on parsec scales. We aim at better understanding the jet kinematics and variability of this source and finding clues that may applicable to other BL Lac objects. The jet was studied with multi-epoch multi-frequency high-resolution VLBI observations. The jet is characterized by a one-sided curved morphology at all epochs and all frequencies. The VLBI core, located at the southern end of the jet, was identified based on its spectral properties. The equipartition magnetic field of the core was investigated, through which we derived a Doppler factor of 5, largely consistent with that derived from kinematics (component C5). The study of the detailed jet kinematics at 22 and 15 GHz, spanning a period of more than 10 years, indicates the possible existence of a bimodal distribution of the jet apparent speed. Ballistic and non-ballistic components are found to coexist in the jet. Superluminal motions in the range of 5-21 c were measured in 11 distinct components. We estimated the physical jet parameters with the minimum Lorentz factor of 10.2 and Doppler factors in the range of 10.2-20.4 (component C5). The coincidence in time of the component&#8217;s ejection and flares supports the idea that, at least in PKS 1749+096, ejection of new jet components is connected with major outbursts in flux density. For the best-traced component (C5) we found that the flux density decays rapidly as it travels downstream the jet, accompanied by a steepening of its spectra, which argues in favor of a contribution of inverse Compton cooling. These properties make PKS 1749+096 a suitable target for an intensive monitoring to decipher the variability phenomenon of BL Lac objects.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/the-parsec-scale-jet-of-pks-1749096-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Influence of internal structure on the motion of test bodies in extreme mass ratio situations [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/20/influence-of-internal-structure-on-the-motion-of-test-bodies-in-extreme-mass-ratio-situations-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/20/influence-of-internal-structure-on-the-motion-of-test-bodies-in-extreme-mass-ratio-situations-cross-listing/#comments</comments>
		<pubDate>Mon, 21 May 2012 00:31:05 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[approximation method]]></category>
		<category><![CDATA[binding energy]]></category>
		<category><![CDATA[equatorial plane]]></category>
		<category><![CDATA[general relativity]]></category>
		<category><![CDATA[geometry]]></category>
		<category><![CDATA[gravitational wave physics]]></category>
		<category><![CDATA[internal structure]]></category>
		<category><![CDATA[kerr]]></category>
		<category><![CDATA[mass ratio]]></category>
		<category><![CDATA[tidal interaction]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/20/influence-of-internal-structure-on-the-motion-of-test-bodies-in-extreme-mass-ratio-situations-cross-listing/</guid>
		<description><![CDATA[We investigate the motion of test bodies with internal structure in General Relativity. With the help of a multipolar approximation method for extended test bodies we derive the equations of motion up to the quadrupolar order. The motion of pole-dipole and quadrupole test bodies is studied in the context of the Kerr geometry. For an [...]]]></description>
			<content:encoded><![CDATA[<p>We investigate the motion of test bodies with internal structure in General Relativity. With the help of a multipolar approximation method for extended test bodies we derive the equations of motion up to the quadrupolar order. The motion of pole-dipole and quadrupole test bodies is studied in the context of the Kerr geometry. For an explicit quadrupole model, which includes spin and tidal interactions, the motion in the equatorial plane is characterized by an effective potential and by the binding energy. We compare our findings to recent results for the conservative part of the self-force of bodies in extreme mass ratio situations. Possible implications for gravitational wave physics are outlined.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/20/influence-of-internal-structure-on-the-motion-of-test-bodies-in-extreme-mass-ratio-situations-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>The Optically Unbiased GRB Host (TOUGH) survey. IV. Lyman-alpha emitters</title>
		<link>http://voxcharta.org/2012/05/17/the-optically-unbiased-grb-host-tough-survey-iv-lyman-alpha-emitters/</link>
		<comments>http://voxcharta.org/2012/05/17/the-optically-unbiased-grb-host-tough-survey-iv-lyman-alpha-emitters/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:56:59 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[40a]]></category>
		<category><![CDATA[alpha emission]]></category>
		<category><![CDATA[equivalent width]]></category>
		<category><![CDATA[extinction]]></category>
		<category><![CDATA[formation rates]]></category>
		<category><![CDATA[gamma ray burst]]></category>
		<category><![CDATA[grbs]]></category>
		<category><![CDATA[host galaxy]]></category>
		<category><![CDATA[hosts]]></category>
		<category><![CDATA[lyman alpha]]></category>
		<category><![CDATA[redshift range]]></category>
		<category><![CDATA[rest frame]]></category>
		<category><![CDATA[spectroscopic search]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/the-optically-unbiased-grb-host-tough-survey-iv-lyman-alpha-emitters/</guid>
		<description><![CDATA[We report the results of a spectroscopic search for Lyman-alpha emission from gamma-ray burst host galaxies. Based on the well-defined TOUGH sample of 69 X-ray selected Swift GRBs, we have targeted the hosts of a subsample of 20 GRBs known from afterglow spectroscopy to be in the redshift range 1.8-4.5. We detect Lya emission from [...]]]></description>
			<content:encoded><![CDATA[<p>We report the results of a spectroscopic search for Lyman-alpha emission from gamma-ray burst host galaxies. Based on the well-defined TOUGH sample of 69 X-ray selected Swift GRBs, we have targeted the hosts of a subsample of 20 GRBs known from afterglow spectroscopy to be in the redshift range 1.8-4.5. We detect Lya emission from 7 out of the 20 hosts, with the typical limiting 3sigma line flux being 8E-18 erg/cm2/s, corresponding to a Lya luminosity of 6E41 erg/s at z=3. The Lya luminosities for the 7 hosts in which we detect Lya emission are in the range (0.6-2.3)E42 erg/s corresponding to star-formation rates of 0.6-2.1 Msun/yr (not corrected for extinction). The rest-frame Lya equivalent widths (EWs) for the 7 hosts are in the range 9-40A. For 6 of the 13 hosts for which Lya is not detected we place fairly strong 3sigma upper limits on the EW (&lt;20A), while for others the EW is either unconstrained or has a less constraining upper limit. We find that the distribution of Lya EWs is inconsistent with being drawn from the Lya EW distribution of bright Lyman break galaxies at the 98.3% level, in the sense that the TOUGH hosts on average have larger EWs than bright LBGs. We can exclude an early indication, based on a smaller, heterogeneous sample of pre-Swift GRB hosts, that all GRB hosts are Lya emitters. We find that the TOUGH hosts on average have lower EWs than the pre-Swift GRB hosts, but the two samples are only inconsistent at the 92% level. The velocity centroid of the Lya line is redshifted by 200-700 km/s with respect to the systemic velocity, similar to what is seen for LBGs, possibly indicating star-formation driven outflows from the host galaxies. There seems to be a trend between the Lya EW and the optical to X-ray spectral index of the afterglow (beta_OX), hinting that dust plays a role in the observed strength and even presence of Lya emission. [ABRIDGED]</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/the-optically-unbiased-grb-host-tough-survey-iv-lyman-alpha-emitters/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Cosmic Rays and Stochastic Magnetic Reconnection in the Heliotail</title>
		<link>http://voxcharta.org/2012/05/17/cosmic-rays-and-stochastic-magnetic-reconnection-in-the-heliotail/</link>
		<comments>http://voxcharta.org/2012/05/17/cosmic-rays-and-stochastic-magnetic-reconnection-in-the-heliotail/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:56:13 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration processes]]></category>
		<category><![CDATA[anisotropy]]></category>
		<category><![CDATA[arrival direction]]></category>
		<category><![CDATA[convective processes]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[diffusion model]]></category>
		<category><![CDATA[energetic particle]]></category>
		<category><![CDATA[energy dependence]]></category>
		<category><![CDATA[energy spectrum]]></category>
		<category><![CDATA[experimental evidence]]></category>
		<category><![CDATA[galactic cosmic rays]]></category>
		<category><![CDATA[heliosphere]]></category>
		<category><![CDATA[interstellar medium]]></category>
		<category><![CDATA[magnetic reconnection]]></category>
		<category><![CDATA[parsec]]></category>
		<category><![CDATA[shock acceleration]]></category>
		<category><![CDATA[smearing]]></category>
		<category><![CDATA[supernova remnant]]></category>
		<category><![CDATA[tev energies]]></category>
		<category><![CDATA[wind gradient]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/cosmic-rays-and-stochastic-magnetic-reconnection-in-the-heliotail/</guid>
		<description><![CDATA[Galactic cosmic rays are believed to be generated by diffusive shock acceleration processes in Supernova Remnants, and the arrival direction is likely determined by the distribution of their sources throughout the Galaxy, in particular by the nearest and youngest ones. Transport to Earth through the interstellar medium is expected to affect the cosmic ray properties [...]]]></description>
			<content:encoded><![CDATA[<p>Galactic cosmic rays are believed to be generated by diffusive shock acceleration processes in Supernova Remnants, and the arrival direction is likely determined by the distribution of their sources throughout the Galaxy, in particular by the nearest and youngest ones. Transport to Earth through the interstellar medium is expected to affect the cosmic ray properties as well. However, the observed anisotropy of TeV cosmic rays and its energy dependence cannot be explained with diffusion models of particle propagation in the Galaxy. Within a distance of a few parsec, diffusion regime is not valid and particles with energy below about 100 TeV must be influenced by the heliosphere and its elongated tail. The observation of a highly significant localized excess region of cosmic rays from the apparent direction of the downstream interstellar flow at 1-10 TeV energies might provide the first experimental evidence that the heliotail can affect the transport of energetic particles. In particular, TeV cosmic rays propagating through the heliotail interact with the 100-300 AU wide magnetic field polarity domains generated by the 11 year cycles. Since the strength of non-linear convective processes is expected to be larger than viscous damping, the plasma in the heliotail is turbulent. Where magnetic field domains converge on each other due to solar wind gradient, stochastic magnetic reconnection likely occurs. Such processes may be efficient enough to re-accelerate a fraction of TeV particles as long as scattering processes are not strong. Therefore the fractional excess of TeV cosmic rays from the narrow region toward the heliotail direction traces sightlines with the lowest smearing scattering effects, that can also explain the observation of a harder than average energy spectrum.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/cosmic-rays-and-stochastic-magnetic-reconnection-in-the-heliotail/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>A Brightest Cluster Galaxy with an Extremely Large Flat Core</title>
		<link>http://voxcharta.org/2012/05/17/a-brightest-cluster-galaxy-with-an-extremely-large-flat-core/</link>
		<comments>http://voxcharta.org/2012/05/17/a-brightest-cluster-galaxy-with-an-extremely-large-flat-core/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:48:33 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bcg]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[cluster galaxy]]></category>
		<category><![CDATA[core structure]]></category>
		<category><![CDATA[cusp]]></category>
		<category><![CDATA[density profile]]></category>
		<category><![CDATA[extrapolation]]></category>
		<category><![CDATA[galaxy cluster abell]]></category>
		<category><![CDATA[hole mass]]></category>
		<category><![CDATA[hubble show]]></category>
		<category><![CDATA[hubble space telescope]]></category>
		<category><![CDATA[hubble space telescope images]]></category>
		<category><![CDATA[interior surface]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[perturbation]]></category>
		<category><![CDATA[space telescope images]]></category>
		<category><![CDATA[stellar density]]></category>
		<category><![CDATA[surface brightness]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/a-brightest-cluster-galaxy-with-an-extremely-large-flat-core/</guid>
		<description><![CDATA[Hubble Space Telescope images of the galaxy cluster Abell 2261, obtained as part of the Cluster Lensing And Supernova survey with Hubble, show that the brightest galaxy in the cluster, A2261-BCG, has the largest core yet detected in any galaxy. The cusp radius of A2261-BCG is 3.2 kpc, twice as big as the next largest [...]]]></description>
			<content:encoded><![CDATA[<p>Hubble Space Telescope images of the galaxy cluster Abell 2261, obtained as part of the Cluster Lensing And Supernova survey with Hubble, show that the brightest galaxy in the cluster, A2261-BCG, has the largest core yet detected in any galaxy. The cusp radius of A2261-BCG is 3.2 kpc, twice as big as the next largest core known, and ~3x bigger than those typically seen in the most luminous BCGs. The morphology of the core in A2261-BCG is also unusual, having a flat or even slightly-depressed interior surface brightness profile, rather than the typical shallow cusp. This implies that the galaxy has a core with constant or even centrally decreasing stellar density. Interpretation of the core as an end product of the &#8220;scouring&#8221; action of a binary supermassive black hole implies a total black hole mass ~1E+10 M_sun from the extrapolation of most relationships between core structure and black hole mass. The core falls 1-sigma above the cusp-radius versus galaxy luminosity relation. Its large size in real terms, and the extremely large black hole mass required to generate it, raise the possibility that the core has been enlarged by additional processes, such as the ejection of the black holes that originally generated the core. The flat central stellar density profile is consistent with this hypothesis. The core is also displaced by 0.7 kpc from the center of the surrounding envelope, consistent with a local dynamical perturbation of the core.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
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		<title>Radiation reaction at 3.5 post-Newtonian order in effective field theory [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/17/radiation-reaction-at-3-5-post-newtonian-order-in-effective-field-theory-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/17/radiation-reaction-at-3-5-post-newtonian-order-in-effective-field-theory-cross-listing/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:48:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[confirmation]]></category>
		<category><![CDATA[constituent]]></category>
		<category><![CDATA[field theory]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[inspiral]]></category>
		<category><![CDATA[lagrangian]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[previous results]]></category>
		<category><![CDATA[radiation reaction]]></category>
		<category><![CDATA[theory approach]]></category>
		<category><![CDATA[variational principle]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/radiation-reaction-at-3-5-post-newtonian-order-in-effective-field-theory-cross-listing/</guid>
		<description><![CDATA[We derive the radiation reaction forces on a compact binary inspiral through 3.5 order in the post-Newtonian expansion using the effective field theory approach. We utilize a recent formulation of Hamilton&#8217;s variational principle that rigorously extends the usual Lagrangian and Hamiltonian formalisms to dissipative systems, including the inspiral of a compact binary from the emission [...]]]></description>
			<content:encoded><![CDATA[<p>We derive the radiation reaction forces on a compact binary inspiral through 3.5 order in the post-Newtonian expansion using the effective field theory approach. We utilize a recent formulation of Hamilton&#8217;s variational principle that rigorously extends the usual Lagrangian and Hamiltonian formalisms to dissipative systems, including the inspiral of a compact binary from the emission of gravitational waves. We find agreement with previous results, which thus provides a non-trivial confirmation of the extended variational principle. The results from this work nearly complete the equations of motion for the generic inspiral of a compact binary with spinning constituents through 3.5 post-Newtonian order, as derived entirely with effective field theory, with only the spin-orbit corrections to the potential at 3.5 post-Newtonian remaining.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/radiation-reaction-at-3-5-post-newtonian-order-in-effective-field-theory-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Viscous-Resistive ADAF with a general Large-Scale Magnetic Field</title>
		<link>http://voxcharta.org/2012/05/17/viscous-resistive-adaf-with-a-general-large-scale-magnetic-field/</link>
		<comments>http://voxcharta.org/2012/05/17/viscous-resistive-adaf-with-a-general-large-scale-magnetic-field/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:47:02 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[adaf]]></category>
		<category><![CDATA[diffusivity]]></category>
		<category><![CDATA[dominant mechanism]]></category>
		<category><![CDATA[energy dissipation]]></category>
		<category><![CDATA[existence]]></category>
		<category><![CDATA[field parameter]]></category>
		<category><![CDATA[global magnetic field]]></category>
		<category><![CDATA[keplerian]]></category>
		<category><![CDATA[kinematic viscosity]]></category>
		<category><![CDATA[numerical result]]></category>
		<category><![CDATA[radial velocity]]></category>
		<category><![CDATA[realistic model]]></category>
		<category><![CDATA[resistivity]]></category>
		<category><![CDATA[rotational velocity]]></category>
		<category><![CDATA[sound speed]]></category>
		<category><![CDATA[Turbulence]]></category>
		<category><![CDATA[velocities]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/viscous-resistive-adaf-with-a-general-large-scale-magnetic-field/</guid>
		<description><![CDATA[We have studied the structure of hot accretion flow bathed in a general large-scale magnetic field. We have considered magnetic parameters $ \beta_{r,\varphi,z}[=c^2_{r,\varphi,z}/(2c^2_{s})] $, where $ c^2_{r, \varphi, z} $ are the Alfv\&#8217;{e}n sound speeds in three direction of cylindrical coordinate $ (r,\varphi,z) $. The dominant mechanism of energy dissipation is assumed to be the [...]]]></description>
			<content:encoded><![CDATA[<p>We have studied the structure of hot accretion flow bathed in a general large-scale magnetic field. We have considered magnetic parameters $ \beta_{r,\varphi,z}[=c^2_{r,\varphi,z}/(2c^2_{s})] $, where $ c^2_{r, \varphi, z} $ are the Alfv\&#8217;{e}n sound speeds in three direction of cylindrical coordinate $ (r,\varphi,z) $. The dominant mechanism of energy dissipation is assumed to be the magnetic diffusivity due to turbulence and viscosity in the accretion flow. Also, we adopt a more realistic model for kinematic viscosity $ (\nu=\alpha c_{s} H) $, with both $ c_{s} $ and $ H $ as a function of magnetic field. As a result in our model, the kinematic viscosity and magnetic diffusivity $ (\eta=\eta_{0}c_{s} H) $ are not constant. In order to solve the integrated equations that govern the behavior of the accretion flow, a self-similar method is used. It is found that the existence of magnetic resistivity will increase the radial infall velocity as well as sound speed and vertical thickness of the disk. However the rotational velocity of the disk decreases by the increase of magnetic resistivity. Moreover, we study the effect of three components of global magnetic field on the structure of the disk. We found out that the radial velocity and sound speed are Sub-Keplerian for all values of magnetic field parameters, but the rotational velocity can be Super-Keplerian by the increase of toroidal magnetic field. Also, Our numerical results show that all components of magnetic field can be important and have a considerable effect on velocities and vertical thickness of the disk.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
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		<title>Non-axisymmetric oscillations of rapidly rotating relativistic stars by conformal flatness approximation [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/17/non-axisymmetric-oscillations-of-rapidly-rotating-relativistic-stars-by-conformal-flatness-approximation-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/17/non-axisymmetric-oscillations-of-rapidly-rotating-relativistic-stars-by-conformal-flatness-approximation-cross-listing/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:46:39 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[approximation]]></category>
		<category><![CDATA[degree of freedom]]></category>
		<category><![CDATA[flatness]]></category>
		<category><![CDATA[general relativity]]></category>
		<category><![CDATA[gravitational radiation]]></category>
		<category><![CDATA[modes]]></category>
		<category><![CDATA[numerical code]]></category>
		<category><![CDATA[oscillation]]></category>
		<category><![CDATA[relativistic gravity]]></category>
		<category><![CDATA[relativistic stars]]></category>
		<category><![CDATA[rotating stars]]></category>
		<category><![CDATA[sequence]]></category>
		<category><![CDATA[similarity]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/non-axisymmetric-oscillations-of-rapidly-rotating-relativistic-stars-by-conformal-flatness-approximation-cross-listing/</guid>
		<description><![CDATA[We present a new numerical code to compute non-axisymmetric eigenmodes of rapidly rotating relativistic stars by adopting spatially conformal flat approximation of general relativity. The approximation omits the radiative degree of freedom of relativistic gravity and the set of equations can be cast into the similar form as those in the corresponding Newtonian problem. The [...]]]></description>
			<content:encoded><![CDATA[<p>We present a new numerical code to compute non-axisymmetric eigenmodes of rapidly rotating relativistic stars by adopting spatially conformal flat approximation of general relativity. The approximation omits the radiative degree of freedom of relativistic gravity and the set of equations can be cast into the similar form as those in the corresponding Newtonian problem. The code developed computes eigenmodes of rapidly rotating stars by taking advantage of this similarity to Newtonian problem. The code is tested against the low order f- and p-modes of slowly rotating stars which shows a good agreement of frequencies computed by our new code and those by the full theory. Also entire sequences of the low order counter-rotating f-modes are computed, which are susceptible to an instability driven by gravitational radiation.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/non-axisymmetric-oscillations-of-rapidly-rotating-relativistic-stars-by-conformal-flatness-approximation-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Relativistic jet models for two low-luminosity radio galaxies: evidence for backflow?</title>
		<link>http://voxcharta.org/2012/05/17/relativistic-jet-models-for-two-low-luminosity-radio-galaxies-evidence-for-backflow/</link>
		<comments>http://voxcharta.org/2012/05/17/relativistic-jet-models-for-two-low-luminosity-radio-galaxies-evidence-for-backflow/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:45:29 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[25c]]></category>
		<category><![CDATA[added component]]></category>
		<category><![CDATA[asymmetry]]></category>
		<category><![CDATA[backflow]]></category>
		<category><![CDATA[component structure]]></category>
		<category><![CDATA[jet axis]]></category>
		<category><![CDATA[jet model]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[linear polarization]]></category>
		<category><![CDATA[lobes]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[radio emission]]></category>
		<category><![CDATA[radio galaxy]]></category>
		<category><![CDATA[radio jet]]></category>
		<category><![CDATA[relativistic jet]]></category>
		<category><![CDATA[relativistic outflows]]></category>
		<category><![CDATA[spectral index]]></category>
		<category><![CDATA[ugc]]></category>
		<category><![CDATA[very large array]]></category>

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

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/integralibis-9-year-galactic-hard-x-ray-survey/</guid>
		<description><![CDATA[Context. The INTEGRAL observatory operating in a hard X-ray/gamma domain gathered a large observational data set over nine years since 2003. Dominant fraction of the observing time was dedicated to the Galactic source population study making the possibility of the deepest Galactic survey in hard X-rays ever compiled. Aims. The aim of the current Galactic [...]]]></description>
			<content:encoded><![CDATA[<p>Context. The INTEGRAL observatory operating in a hard X-ray/gamma domain gathered a large observational data set over nine years since 2003. Dominant fraction of the observing time was dedicated to the Galactic source population study making the possibility of the deepest Galactic survey in hard X-rays ever compiled. Aims. The aim of the current Galactic survey is to make a basis for Galactic source population studies, and perform mapping of the Milky Way in hard X-rays over the maximum exposure available at |b|&lt;17.5 deg. Methods. We used sky reconstruction algorithms specially developed for the high quality imaging of INTEGRAL/IBIS data. Results. We present sky images, sensitivity maps, and catalogs of detected sources in three energy bands: 17-60, 17-35, and 35-80 keV in the Galactic plane at |b|5 sigma has an identification completeness of ~91%, which is valuable for population studies.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
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		<title>Anisotropy of TeV and PeV cosmic rays with IceCube and IceTop</title>
		<link>http://voxcharta.org/2012/05/17/anisotropy-of-tev-and-pev-cosmic-rays-with-icecube-and-icetop/</link>
		<comments>http://voxcharta.org/2012/05/17/anisotropy-of-tev-and-pev-cosmic-rays-with-icecube-and-icetop/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:43:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[angular scale]]></category>
		<category><![CDATA[anisotropy]]></category>
		<category><![CDATA[array]]></category>
		<category><![CDATA[arrival direction]]></category>
		<category><![CDATA[atmosphere]]></category>
		<category><![CDATA[cosmic ray data]]></category>
		<category><![CDATA[cosmic ray studies]]></category>
		<category><![CDATA[earth]]></category>
		<category><![CDATA[energy range]]></category>
		<category><![CDATA[extensive air showers]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[IceCube]]></category>
		<category><![CDATA[interaction]]></category>
		<category><![CDATA[neutrino telescope]]></category>
		<category><![CDATA[observation]]></category>
		<category><![CDATA[primary cosmic rays]]></category>
		<category><![CDATA[secondary particles]]></category>
		<category><![CDATA[statistics data]]></category>
		<category><![CDATA[TeV]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/anisotropy-of-tev-and-pev-cosmic-rays-with-icecube-and-icetop/</guid>
		<description><![CDATA[The interaction of high energy cosmic rays with the Earth&#8217;s atmosphere produces extensive air showers of secondary particles with a large muon component. By exploiting the sensitivity of neutrino telescopes to high energy muons, it is possible to use these detectors for precision cosmic ray studies. The high rate of cosmic-ray muon events provides a [...]]]></description>
			<content:encoded><![CDATA[<p>The interaction of high energy cosmic rays with the Earth&#8217;s atmosphere produces extensive air showers of secondary particles with a large muon component. By exploiting the sensitivity of neutrino telescopes to high energy muons, it is possible to use these detectors for precision cosmic ray studies. The high rate of cosmic-ray muon events provides a high-statistics data sample that can be used to look for anisotropy in the arrival directions of the parent particles at the per-mille level.   This paper reports on the observation of anisotropy in the cosmic ray data collected with the IceCube neutrino telescope in the 20-400 TeV energy range at multiple angular scales. New data from the IceTop air shower array, located on the ice surface above IceCube, shows an anisotropy that is consistent with the high-energy IceCube results. The sensitivity of IceTop to all the components of the extensive air shower will allow us to explore in more detail the characteristics of the primary cosmic rays associated with the observed anisotropy.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/anisotropy-of-tev-and-pev-cosmic-rays-with-icecube-and-icetop/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>X-ray Emission from Transient Jet Model in Black Hole Binaries [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/x-ray-emission-from-transient-jet-model-in-black-hole-binaries-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/x-ray-emission-from-transient-jet-model-in-black-hole-binaries-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:37:51 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[compton]]></category>
		<category><![CDATA[electron]]></category>
		<category><![CDATA[hole binaries]]></category>
		<category><![CDATA[inflow and outflow]]></category>
		<category><![CDATA[infrared emission]]></category>
		<category><![CDATA[inner radius]]></category>
		<category><![CDATA[jet model]]></category>
		<category><![CDATA[keV]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[new model]]></category>
		<category><![CDATA[outburst]]></category>
		<category><![CDATA[possible connection]]></category>
		<category><![CDATA[radii]]></category>
		<category><![CDATA[ray binaries]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[synchrotron]]></category>
		<category><![CDATA[transient nature]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xte j1118]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/x-ray-emission-from-transient-jet-model-in-black-hole-binaries-replacement/</guid>
		<description><![CDATA[While the non-thermal radio through at least near-infrared emission in the hard state in X-ray binaries (XRBs) is known to originate in jets, the source of the non-thermal X-ray component is still uncertain. We introduce a new model for this emission, which takes into account the transient nature of outflows, and show that it can [...]]]></description>
			<content:encoded><![CDATA[<p>While the non-thermal radio through at least near-infrared emission in the hard state in X-ray binaries (XRBs) is known to originate in jets, the source of the non-thermal X-ray component is still uncertain. We introduce a new model for this emission, which takes into account the transient nature of outflows, and show that it can explain the observed properties of the X-ray spectrum. Rapid radiative cooling of the electrons naturally accounts for the break often seen below around 10 keV, and for the canonical spectral slope F_\nu ~ \nu^{-1/2} observed below the break. We derive the constraints set by the data for both synchrotron- and Compton-dominated models. We show that for the synchrotron-dominated case, the jet should be launched at radii comparable to the inner radius of the disk (~few 100 r_s for the 2000 outburst of XTE J1118+480), with typical magnetic field B &gt;~ 10^{6} G. We discuss the consequences of our results on the possible connection between the inflow and outflow in the hard state of XRBs.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/x-ray-emission-from-transient-jet-model-in-black-hole-binaries-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Panchromatic Observations of SN 2011dh Point to a Compact Progenitor Star [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/panchromatic-observations-of-sn-2011dh-point-to-a-compact-progenitor-star-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/panchromatic-observations-of-sn-2011dh-point-to-a-compact-progenitor-star-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:37:05 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[circumstellar environment]]></category>
		<category><![CDATA[current instruments]]></category>
		<category><![CDATA[density profile]]></category>
		<category><![CDATA[emission radio]]></category>
		<category><![CDATA[equipartition]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[hst observation]]></category>
		<category><![CDATA[inverse compton]]></category>
		<category><![CDATA[mass loss]]></category>
		<category><![CDATA[optical emission]]></category>
		<category><![CDATA[optical photometry]]></category>
		<category><![CDATA[optical photons]]></category>
		<category><![CDATA[progenitor star]]></category>
		<category><![CDATA[radio data]]></category>
		<category><![CDATA[ray observations]]></category>
		<category><![CDATA[spatial coverage]]></category>
		<category><![CDATA[stellar density]]></category>
		<category><![CDATA[synchrotron emission]]></category>
		<category><![CDATA[type iib]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/panchromatic-observations-of-sn-2011dh-point-to-a-compact-progenitor-star-replacement/</guid>
		<description><![CDATA[We report the discovery and detailed monitoring of X-ray emission associated with the Type IIb SN 2011dh using data from the Swift and Chandra satellites, placing it among the best studied X-ray supernovae to date. We further present millimeter and radio data obtained with the SMA, CARMA, and EVLA during the first three weeks after [...]]]></description>
			<content:encoded><![CDATA[<p>We report the discovery and detailed monitoring of X-ray emission associated with the Type IIb SN 2011dh using data from the Swift and Chandra satellites, placing it among the best studied X-ray supernovae to date. We further present millimeter and radio data obtained with the SMA, CARMA, and EVLA during the first three weeks after explosion. Combining these observations with early optical photometry, we show that the panchromatic dataset is well-described by non-thermal synchrotron emission (radio/mm) with inverse Compton scattering (X-ray) of a thermal population of optical photons. In this scenario, the shock partition fractions deviate from equipartition by a factor, (e_e/e_B) ~ 30. We derive the properties of the shockwave and the circumstellar environment and find a shock velocity, v~0.1c, and a progenitor mass loss rate of ~6e-5 M_sun/yr. These properties are consistent with the sub-class of Type IIb SNe characterized by compact progenitors (Type cIIb) and dissimilar from those with extended progenitors (Type eIIb). Furthermore, we consider the early optical emission in the context of a cooling envelope model to estimate a progenitor radius of ~1e+11 cm, in line with the expectations for a Type cIIb SN. Together, these diagnostics are difficult to reconcile with the extended radius of the putative yellow supergiant progenitor star identified in archival HST observations, unless the stellar density profile is unusual. Finally, we searched for the high energy shock breakout pulse using X-ray and gamma-ray observations obtained during the purported explosion date range. Based on the compact radius of the progenitor, we estimate that the breakout pulse was detectable with current instruments but likely missed due to their limited temporal/spatial coverage. [Abridged]</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/panchromatic-observations-of-sn-2011dh-point-to-a-compact-progenitor-star-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The relation between broad lines and gamma&#8211;ray luminosities in Fermi blazars [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/the-relation-between-broad-lines-and-gamma-ray-luminosities-in-fermi-blazars-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/the-relation-between-broad-lines-and-gamma-ray-luminosities-in-fermi-blazars-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:36:07 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absolute value]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[bl lac]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[blazar]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[digital sky survey]]></category>
		<category><![CDATA[eddington]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[energy emission]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[hole mass]]></category>
		<category><![CDATA[jet power]]></category>
		<category><![CDATA[mev]]></category>
		<category><![CDATA[proxy]]></category>
		<category><![CDATA[sdss]]></category>
		<category><![CDATA[sloan digital]]></category>
		<category><![CDATA[spectrum radio]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/the-relation-between-broad-lines-and-gamma-ray-luminosities-in-fermi-blazars-replacement/</guid>
		<description><![CDATA[We study the relation between the mass accretion rate, the jet power, and the black hole mass of blazars. To this aim, we make use of the Sloan Digital Sky Survey (SDSS) and the 11 months catalog of blazars detected at energies larger than 100 MeV by the Large Area Telescope (LAT) onboard the Fermi [...]]]></description>
			<content:encoded><![CDATA[<p>We study the relation between the mass accretion rate, the jet power, and the black hole mass of blazars. To this aim, we make use of the Sloan Digital Sky Survey (SDSS) and the 11 months catalog of blazars detected at energies larger than 100 MeV by the Large Area Telescope (LAT) onboard the Fermi satellite. This allows to construct a relatively large sample of blazars with information about the luminosity (or upper limits) of their emission lines used as a proxy for the strength of the disc luminosity and on the luminosity of the high energy emission, used as a proxy for the jet power. We find a good correlation between the luminosity of the broad lines and the gamma-ray luminosity as detected by Fermi, both using absolute values of the luminosities and normalising them to the Eddington value. The data we have analyzed confirm that the division of blazars into BL Lacs and Flat Spectrum Radio Quasars (FSRQs) is controlled by the line luminosity in Eddington units. For small values of this ratio the object is a BL Lac, while it is a FSRQs for large values. The transition appears smooth, but a much larger number of objects is needed to confirm this point.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/the-relation-between-broad-lines-and-gamma-ray-luminosities-in-fermi-blazars-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Multiphase, non-spherical gas accretion onto a black hole [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/multiphase-non-spherical-gas-accretion-onto-a-black-hole-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/multiphase-non-spherical-gas-accretion-onto-a-black-hole-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:34:46 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[3d simulation]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[astrophysical implications]]></category>
		<category><![CDATA[central mass]]></category>
		<category><![CDATA[dense clump]]></category>
		<category><![CDATA[density region]]></category>
		<category><![CDATA[filament]]></category>
		<category><![CDATA[filamentary structure]]></category>
		<category><![CDATA[formation of clouds]]></category>
		<category><![CDATA[formation of stars]]></category>
		<category><![CDATA[inflow rate]]></category>
		<category><![CDATA[line regions]]></category>
		<category><![CDATA[low density]]></category>
		<category><![CDATA[radii]]></category>
		<category><![CDATA[spatial location]]></category>
		<category><![CDATA[supermassive black hole]]></category>
		<category><![CDATA[thermal instability]]></category>
		<category><![CDATA[x limit]]></category>
		<category><![CDATA[x ray]]></category>

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

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/light-dark-matter-light-higgs-and-the-electroweak-phase-transition-replacement-2/</guid>
		<description><![CDATA[We propose a minimal extension of the Standard Model by two real singlet fields that could provide a good candidate for light Dark Matter, and give a strong first order electroweak phase transition. As a result, there are two CP even scalars; one is lighter than \sim 70 GeV, and the other one with mass [...]]]></description>
			<content:encoded><![CDATA[<p>We propose a minimal extension of the Standard Model by two real singlet fields that could provide a good candidate for light Dark Matter, and give a strong first order electroweak phase transition. As a result, there are two CP even scalars; one is lighter than \sim 70 GeV, and the other one with mass in the range of 280-400 GeV; and consistent with electroweak precision tests. We show that the light scalar mass can be as small as 25 GeV while still being consistent with the LEP data. The predicted dark matter scattering cross section is large enough to accommodate CoGeNT and can be probed by future XENON experiment. We also show that for dark matter mass around 2 GeV, the branching fraction of the process (B^+\rightarrowK^++2(DM)) can be accessible in SuperB factories.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/light-dark-matter-light-higgs-and-the-electroweak-phase-transition-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Dark matter origin of the gamma ray emission from the galactic center observed by HESS [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/dark-matter-origin-of-the-gamma-ray-emission-from-the-galactic-center-observed-by-hess-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/dark-matter-origin-of-the-gamma-ray-emission-from-the-galactic-center-observed-by-hess-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:32:37 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[annihilation]]></category>
		<category><![CDATA[array]]></category>
		<category><![CDATA[cherenkov telescopes]]></category>
		<category><![CDATA[contraction]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[enhancement]]></category>
		<category><![CDATA[Fermi]]></category>
		<category><![CDATA[galactic center]]></category>
		<category><![CDATA[gamma ray emission]]></category>
		<category><![CDATA[hes]]></category>
		<category><![CDATA[morphology]]></category>
		<category><![CDATA[parsec]]></category>
		<category><![CDATA[photon]]></category>
		<category><![CDATA[profile]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[spectrum]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/dark-matter-origin-of-the-gamma-ray-emission-from-the-galactic-center-observed-by-hess-replacement/</guid>
		<description><![CDATA[We show that the gamma ray spectrum observed with the HESS array of Cherenkov telescopes coming from the Galactic Center (GC) region and identified with the source HESS J1745-290, is well fitted by the secondary photons coming from dark matter (DM) annihilation over a diffuse power-law background. The amount of photons and morphology of the [...]]]></description>
			<content:encoded><![CDATA[<p>We show that the gamma ray spectrum observed with the HESS array of Cherenkov telescopes coming from the Galactic Center (GC) region and identified with the source HESS J1745-290, is well fitted by the secondary photons coming from dark matter (DM) annihilation over a diffuse power-law background. The amount of photons and morphology of the signal localized within a region of few parsecs, require compressed DM profiles as those resulting from baryonic contraction, which offer $\sim 10^3$ enhancements in the signal over DM alone simulations. The fitted background from HESS data is consistent with recent Fermi-LAT observations of the same region.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/dark-matter-origin-of-the-gamma-ray-emission-from-the-galactic-center-observed-by-hess-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Multi-wavelength study of the Be/X-ray binary MXB 0656-072 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/multi-wavelength-study-of-the-bex-ray-binary-mxb-0656-072-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/multi-wavelength-study-of-the-bex-ray-binary-mxb-0656-072-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:32:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[cyclotron resonance]]></category>
		<category><![CDATA[density region]]></category>
		<category><![CDATA[energy absorption]]></category>
		<category><![CDATA[iron line]]></category>
		<category><![CDATA[keV]]></category>
		<category><![CDATA[low density]]></category>
		<category><![CDATA[low energy]]></category>
		<category><![CDATA[mass ejection]]></category>
		<category><![CDATA[mxb]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[orbital period]]></category>
		<category><![CDATA[photometric]]></category>
		<category><![CDATA[rxte asm]]></category>
		<category><![CDATA[spectral shape]]></category>
		<category><![CDATA[spectroscopic data]]></category>
		<category><![CDATA[variability]]></category>
		<category><![CDATA[wavelength]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/multi-wavelength-study-of-the-bex-ray-binary-mxb-0656-072-replacement/</guid>
		<description><![CDATA[We present and analyze the optical photometric and spectroscopic data of the Be/X-ray binary MXB 0656-072 from 2006 to 2009. A 101.2-day orbital period is found, for the first time, from the present public X-ray data(Swift/BAT and RXTE/ASM). The anti-correlation between the H$\alpha$ emission and the $UBV$ brightness of MXB 0656$-$072 during our 2007 observations [...]]]></description>
			<content:encoded><![CDATA[<p>We present and analyze the optical photometric and spectroscopic data of the Be/X-ray binary MXB 0656-072 from 2006 to 2009. A 101.2-day orbital period is found, for the first time, from the present public X-ray data(Swift/BAT and RXTE/ASM). The anti-correlation between the H$\alpha$ emission and the $UBV$ brightness of MXB 0656$-$072 during our 2007 observations indicates that a mass ejection event took place in the system. After the mass ejection, a low-density region might develop around the Oe star. With the outward motion of the circumstellar disk, the outer part of the disk interacted with the neutron star around its periastron passage and a series of the X-ray outbursts were triggered between MJD 54350 and MJD 54850. The PCA&#8211;HEXTE spectra during the 2007-2008 X-ray outbursts could be well fitted by a cut-off power law with low energy absorption, together with an iron line around 6.4 keV, and a broad cyclotron resonance feature around 30 keV. The same variability of the soft and hard X-ray colors in 2.3-21 keV indicated that there were no overall changes in the spectral shape during the X-ray outbursts, which might be only connected with the changes of the mass-accretion rate onto the neutron star.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/multi-wavelength-study-of-the-bex-ray-binary-mxb-0656-072-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A First Search for coincident Gravitational Waves and High Energy Neutrinos using LIGO, Virgo and ANTARES data from 2007 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/a-first-search-for-coincident-gravitational-waves-and-high-energy-neutrinos-using-ligo-virgo-and-antares-data-from-2007-replacement/</link>
		<comments>http://voxcharta.org/2012/05/17/a-first-search-for-coincident-gravitational-waves-and-high-energy-neutrinos-using-ligo-virgo-and-antares-data-from-2007-replacement/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:31:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[antares]]></category>
		<category><![CDATA[astronomy]]></category>
		<category><![CDATA[collapse events]]></category>
		<category><![CDATA[core collapse]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[energy neutrino]]></category>
		<category><![CDATA[first science]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[hidden sources]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[ligo]]></category>
		<category><![CDATA[line configuration]]></category>
		<category><![CDATA[merger]]></category>
		<category><![CDATA[messengers]]></category>
		<category><![CDATA[neutrino event]]></category>
		<category><![CDATA[neutrino telescope]]></category>
		<category><![CDATA[virgo]]></category>
		<category><![CDATA[wave signals]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/a-first-search-for-coincident-gravitational-waves-and-high-energy-neutrinos-using-ligo-virgo-and-antares-data-from-2007-replacement/</guid>
		<description><![CDATA[We present the results of the first search for gravitational wave bursts associated with high energy neutrinos. Together, these messengers could reveal new, hidden sources that are not observed by conventional photon astronomy, particularly at high energy. Our search uses neutrinos detected by the underwater neutrino telescope ANTARES in its 5 line configuration during the [...]]]></description>
			<content:encoded><![CDATA[<p>We present the results of the first search for gravitational wave bursts associated with high energy neutrinos. Together, these messengers could reveal new, hidden sources that are not observed by conventional photon astronomy, particularly at high energy. Our search uses neutrinos detected by the underwater neutrino telescope ANTARES in its 5 line configuration during the period January &#8211; September 2007, which coincided with the fifth and first science runs of LIGO and Virgo, respectively. The LIGO-Virgo data were analysed for candidate gravitational-wave signals coincident in time and direction with the neutrino events. No significant coincident events were observed. We place limits on the density of joint high energy neutrino &#8211; gravitational wave emission events in the local universe, and compare them with densities of merger and core-collapse events.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/a-first-search-for-coincident-gravitational-waves-and-high-energy-neutrinos-using-ligo-virgo-and-antares-data-from-2007-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Neutrinos And Cosmic Rays From Gamma Ray Bursts [Replacement]</title>
		<link>http://voxcharta.org/2012/05/17/neutrinos-and-cosmic-rays-from-gamma-ray-bursts-replacement-2/</link>
		<comments>http://voxcharta.org/2012/05/17/neutrinos-and-cosmic-rays-from-gamma-ray-bursts-replacement-2/#comments</comments>
		<pubDate>Fri, 18 May 2012 00:31:25 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[collaboration]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[energy neutrino]]></category>
		<category><![CDATA[fireball]]></category>
		<category><![CDATA[gamma ray burst]]></category>
		<category><![CDATA[grbs]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[main source]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/17/neutrinos-and-cosmic-rays-from-gamma-ray-bursts-replacement-2/</guid>
		<description><![CDATA[The upper limit on the flux of ultra high energy neutrinos from gamma-ray bursts (GRBs) that was reported recently by the IceCube collaboration contradicts predictions based on the Fireball model of GRBs, but does not exclude GRBs as a main source of ultra-high energy cosmic rays.
]]></description>
			<content:encoded><![CDATA[<p>The upper limit on the flux of ultra high energy neutrinos from gamma-ray bursts (GRBs) that was reported recently by the IceCube collaboration contradicts predictions based on the Fireball model of GRBs, but does not exclude GRBs as a main source of ultra-high energy cosmic rays.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/17/neutrinos-and-cosmic-rays-from-gamma-ray-bursts-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>An X-ray Survey of Colliding Wind Binaries</title>
		<link>http://voxcharta.org/2012/05/16/an-x-ray-survey-of-colliding-wind-binaries/</link>
		<comments>http://voxcharta.org/2012/05/16/an-x-ray-survey-of-colliding-wind-binaries/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:54:18 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[Chandra]]></category>
		<category><![CDATA[keV]]></category>
		<category><![CDATA[magellanic cloud]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[model parameter]]></category>
		<category><![CDATA[Newton]]></category>
		<category><![CDATA[order of magnitude]]></category>
		<category><![CDATA[primaries]]></category>
		<category><![CDATA[satellite]]></category>
		<category><![CDATA[short period]]></category>
		<category><![CDATA[soft x]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[system characteristics]]></category>
		<category><![CDATA[wolf]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/an-x-ray-survey-of-colliding-wind-binaries/</guid>
		<description><![CDATA[We have compiled a list of 35 O+O binaries and 86 Wolf-Rayet binaries in the Milky Way and Magellanic clouds detected with the {\it Chandra}, {\it XMM-Newton} and {\it ROSAT} satellites to probe the connection between their X-ray properties % ($L_{\rm X}$, $L_{\rm X}/L_{\rm bol}$ and $kT$) and their system characteristics. Of the Wolf-Rayet binaries [...]]]></description>
			<content:encoded><![CDATA[<p>We have compiled a list of 35 O+O binaries and 86 Wolf-Rayet binaries in the Milky Way and Magellanic clouds detected with the {\it Chandra}, {\it XMM-Newton} and {\it ROSAT} satellites to probe the connection between their X-ray properties % ($L_{\rm X}$, $L_{\rm X}/L_{\rm bol}$ and $kT$) and their system characteristics. Of the Wolf-Rayet binaries with published model parameters, all have log LX &gt; 32, kT &gt; 1 keV and log Lx/Lbol &gt; -7. The most X-ray luminous W-R binaries are typically very long period systems. The WR binaries show a nearly four-order of magnitude spread in X-ray luminosity, even among among systems with very similar W-R primaries. Among the O+O binaries, short-period systems have soft X-ray spectra and longer period systems show harder X-ray spectra again with a large spread in Lx/Lbol.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/an-x-ray-survey-of-colliding-wind-binaries/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Electron-positron plasma in GRBs and in cosmology</title>
		<link>http://voxcharta.org/2012/05/16/electron-positron-plasma-in-grbs-and-in-cosmology/</link>
		<comments>http://voxcharta.org/2012/05/16/electron-positron-plasma-in-grbs-and-in-cosmology/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:53:57 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration phase]]></category>
		<category><![CDATA[admixture]]></category>
		<category><![CDATA[analogy]]></category>
		<category><![CDATA[cosmic microwave background]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[deceleration]]></category>
		<category><![CDATA[early universe]]></category>
		<category><![CDATA[electron]]></category>
		<category><![CDATA[electron positron]]></category>
		<category><![CDATA[gamma ray burst]]></category>
		<category><![CDATA[grb sources]]></category>
		<category><![CDATA[grbs]]></category>
		<category><![CDATA[helium]]></category>
		<category><![CDATA[light element]]></category>
		<category><![CDATA[microwave background radiation]]></category>
		<category><![CDATA[neutral hydrogen]]></category>
		<category><![CDATA[outflow]]></category>
		<category><![CDATA[photon]]></category>
		<category><![CDATA[proton]]></category>
		<category><![CDATA[thermal acceleration]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/electron-positron-plasma-in-grbs-and-in-cosmology/</guid>
		<description><![CDATA[Electron-positron plasma is believed to play imporant role both in the early Universe and in sources of Gamma-Ray Bursts (GRBs). We focus on analogy and difference between physical conditions of electron-positron plasma in the early Universe and in sources of GRBs. We discuss a) dynamical differences, namely thermal acceleration of the outflow in GRB sources [...]]]></description>
			<content:encoded><![CDATA[<p>Electron-positron plasma is believed to play imporant role both in the early Universe and in sources of Gamma-Ray Bursts (GRBs). We focus on analogy and difference between physical conditions of electron-positron plasma in the early Universe and in sources of GRBs. We discuss a) dynamical differences, namely thermal acceleration of the outflow in GRB sources vs cosmological deceleration; b) nuclear composition differences as synthesis of light elements in the early Universe and possible destruction of heavy elements in GRB plasma; c) different physical conditions during last scattering of photons by electrons. Only during the acceleration phase of the optically thick electron-positron plasma comoving observer may find it similar to the early Universe. This similarity breaks down during the coasting phase. Reprocessing of nuclear abundances may likely take place in GRB sources. Heavy nuclear elements are then destroyed, resulting mainly in protons with small admixture of helium. Unlike the primordial plasma which recombines to form neutral hydrogen, and emits the Cosmic Microwave Background Radiation, GRB plasma does not cool down enough to recombine.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/electron-positron-plasma-in-grbs-and-in-cosmology/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Dark matter transport properties and rapidly rotating neutron stars</title>
		<link>http://voxcharta.org/2012/05/16/dark-matter-transport-properties-and-rapidly-rotating-neutron-stars/</link>
		<comments>http://voxcharta.org/2012/05/16/dark-matter-transport-properties-and-rapidly-rotating-neutron-stars/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:52:41 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[attractive places]]></category>
		<category><![CDATA[collective oscillations]]></category>
		<category><![CDATA[coriolis force]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[free path]]></category>
		<category><![CDATA[massive particle]]></category>
		<category><![CDATA[matter transport]]></category>
		<category><![CDATA[mode oscillations]]></category>
		<category><![CDATA[modes]]></category>
		<category><![CDATA[neutron star matter]]></category>
		<category><![CDATA[rotating neutron star]]></category>
		<category><![CDATA[rotating stars]]></category>
		<category><![CDATA[shear viscosity]]></category>
		<category><![CDATA[thermal conductivity]]></category>
		<category><![CDATA[transport properties]]></category>
		<category><![CDATA[wimp]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/dark-matter-transport-properties-and-rapidly-rotating-neutron-stars/</guid>
		<description><![CDATA[Neutron stars are attractive places to look for dark matter because their high densities allow repeated interactions. Weakly interacting massive particles (WIMPs) may scatter efficiently in the core or in the crust of a neutron star. In this paper we focus on WIMP contributions to transport properties, such as shear viscosity or thermal conductivity, because [...]]]></description>
			<content:encoded><![CDATA[<p>Neutron stars are attractive places to look for dark matter because their high densities allow repeated interactions. Weakly interacting massive particles (WIMPs) may scatter efficiently in the core or in the crust of a neutron star. In this paper we focus on WIMP contributions to transport properties, such as shear viscosity or thermal conductivity, because these can be greatly enhanced by long mean free paths. We speculate that WIMPs increase the shear viscosity of neutron star matter and help stabilize r-mode oscillations. These are collective oscillations where the restoring force is the Coriolis force. At present r-modes are thought to be unstable in many observed rapidly rotating stars. If WIMPs stabilize the r-modes, this would allow neutron stars to spin rapidly. This likely requires WIMP-nucleon cross sections near present experimental limits and an appropriate density of WIMPs in neutron stars.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/dark-matter-transport-properties-and-rapidly-rotating-neutron-stars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Constraining the Bulk Lorentz Factor of GRB Outflow in the Magnetic-dominated Jet Model</title>
		<link>http://voxcharta.org/2012/05/16/constraining-the-bulk-lorentz-factor-of-grb-outflow-in-the-magnetic-dominated-jet-model/</link>
		<comments>http://voxcharta.org/2012/05/16/constraining-the-bulk-lorentz-factor-of-grb-outflow-in-the-magnetic-dominated-jet-model/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:50:53 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[coast phase]]></category>
		<category><![CDATA[expansion phase]]></category>
		<category><![CDATA[grbs]]></category>
		<category><![CDATA[jet model]]></category>
		<category><![CDATA[lorentz factor]]></category>
		<category><![CDATA[minimum values]]></category>
		<category><![CDATA[optical depth]]></category>
		<category><![CDATA[outflow]]></category>
		<category><![CDATA[photon]]></category>
		<category><![CDATA[single zone]]></category>
		<category><![CDATA[time delay]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/constraining-the-bulk-lorentz-factor-of-grb-outflow-in-the-magnetic-dominated-jet-model/</guid>
		<description><![CDATA[Recent observations by Fermi-LAT showed that there are delayed arrival of GeV photons relative to the onset of MeV photons in some GRBs. In order to avoid a large optical depth, minimum values of Lorentz factor have been estimated to be higher than 1000 in some brightest bursts. In this paper, we present a detailed [...]]]></description>
			<content:encoded><![CDATA[<p>Recent observations by Fermi-LAT showed that there are delayed arrival of GeV photons relative to the onset of MeV photons in some GRBs. In order to avoid a large optical depth, minimum values of Lorentz factor have been estimated to be higher than 1000 in some brightest bursts. In this paper, we present a detailed calculation of the time delay between the MeV and GeV photons in the framework of the magnetic-dominated jet model. We find that the time delay strongly depends on the terminal bulk Lorentz factor of the jet. Inspired by this fact, we use this model to calculate the Lorentz factors of four Fermi bursts. The results show that the Lorentz factors are much lower than that obtained from &#8220;single-zone&#8221; scenario. The short GRB 090510 has a minimal Lorentz factor 385, while the three long GRBs have almost the same Lorentz factors, with an average value near 260. Another interesting feature is that, for long GRBs, GeV photons are emitted after the Lorentz factor saturates. For short GRBs, however, MeV and GeV photons are emitted at the same phase, i.e, either at the expansion phase or at the coast phase.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/constraining-the-bulk-lorentz-factor-of-grb-outflow-in-the-magnetic-dominated-jet-model/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Spectral analysis of the gamma-ray background near the dwarf Milky Way satellite Segue 1: Improved limits on the cross section of neutralino dark matter annihilation</title>
		<link>http://voxcharta.org/2012/05/16/spectral-analysis-of-the-gamma-ray-background-near-the-dwarf-milky-way-satellite-segue-1-improved-limits-on-the-cross-section-of-neutralino-dark-matter-annihilation/</link>
		<comments>http://voxcharta.org/2012/05/16/spectral-analysis-of-the-gamma-ray-background-near-the-dwarf-milky-way-satellite-segue-1-improved-limits-on-the-cross-section-of-neutralino-dark-matter-annihilation/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:49:09 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[angular extent]]></category>
		<category><![CDATA[annihilation]]></category>
		<category><![CDATA[cross section]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[gamma ray data]]></category>
		<category><![CDATA[indirect detection]]></category>
		<category><![CDATA[likelihood analysis]]></category>
		<category><![CDATA[Milky Way]]></category>
		<category><![CDATA[ray observations]]></category>
		<category><![CDATA[satellite galaxy]]></category>
		<category><![CDATA[spectral analysis]]></category>
		<category><![CDATA[uncertainty]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/spectral-analysis-of-the-gamma-ray-background-near-the-dwarf-milky-way-satellite-segue-1-improved-limits-on-the-cross-section-of-neutralino-dark-matter-annihilation/</guid>
		<description><![CDATA[The indirect detection of dark matter requires that dark matter annihilation products be discriminated from conventional astrophysical backgrounds. Here, we re-analyze GeV-band gamma-ray observations of the prominent Milky Way dwarf satellite galaxy Segue 1, for which the expected astrophysical background is minimal. We explicitly account for the angular extent of the conservatively expected gamma-ray signal [...]]]></description>
			<content:encoded><![CDATA[<p>The indirect detection of dark matter requires that dark matter annihilation products be discriminated from conventional astrophysical backgrounds. Here, we re-analyze GeV-band gamma-ray observations of the prominent Milky Way dwarf satellite galaxy Segue 1, for which the expected astrophysical background is minimal. We explicitly account for the angular extent of the conservatively expected gamma-ray signal and keep the uncertainty in the dark-matter profile external to the likelihood analysis of the gamma-ray data.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/spectral-analysis-of-the-gamma-ray-background-near-the-dwarf-milky-way-satellite-segue-1-improved-limits-on-the-cross-section-of-neutralino-dark-matter-annihilation/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Hadron-Quark Crossover and Massive Hybrid Stars with Strangeness [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/16/hadron-quark-crossover-and-massive-hybrid-stars-with-strangeness-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/16/hadron-quark-crossover-and-massive-hybrid-stars-with-strangeness-cross-listing/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:48:52 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[conclusion]]></category>
		<category><![CDATA[crossover region]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[equation of state]]></category>
		<category><![CDATA[hadronic matter]]></category>
		<category><![CDATA[hybrid stars]]></category>
		<category><![CDATA[hyperon]]></category>
		<category><![CDATA[mass of neutron]]></category>
		<category><![CDATA[maximum mass]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[nuclear density]]></category>
		<category><![CDATA[strangeness]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/hadron-quark-crossover-and-massive-hybrid-stars-with-strangeness-cross-listing/</guid>
		<description><![CDATA[On the basis of a smooth crossover from the hadronic matter with hyperons to quark matter with strangeness, we show that the maximum mass of neutron stars with quark matter core can be larger than those without quark matter core. This is in contrast to the conventional softening of equation of state due to exotic [...]]]></description>
			<content:encoded><![CDATA[<p>On the basis of a smooth crossover from the hadronic matter with hyperons to quark matter with strangeness, we show that the maximum mass of neutron stars with quark matter core can be larger than those without quark matter core. This is in contrast to the conventional softening of equation of state due to exotic components at high density. Essential conditions to reach our conclusion are (i) the crossover takes place at relatively low densities, i.e., (2 &#8211; 4) times the normal nuclear density, and (ii) the quark matter is strongly interacting in the crossover region. By these, the pressure of the system can be greater than that of purely hadronic matter in the crossover region and leads to the maximum mass greater than 2 solar mass. Several implications of this result to the nuclear incompressibility, the hyperon mixing, and the neutrino cooling are also remarked.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/hadron-quark-crossover-and-massive-hybrid-stars-with-strangeness-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>On the Cosmic Ray Muon Hypothesis for DAMA [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/16/on-the-cosmic-ray-muon-hypothesis-for-dama-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/16/on-the-cosmic-ray-muon-hypothesis-for-dama-cross-listing/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:46:34 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[dark matter search]]></category>
		<category><![CDATA[hypothesis]]></category>
		<category><![CDATA[low energy]]></category>
		<category><![CDATA[modulation]]></category>
		<category><![CDATA[muon flux]]></category>
		<category><![CDATA[variation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/on-the-cosmic-ray-muon-hypothesis-for-dama-cross-listing/</guid>
		<description><![CDATA[The DAMA dark matter search experiment observes a statistically significant percent-level variation of its low-energy count rate with a period of one year. In this note we recall some of the arguments which challenge the hypothesis that the cosmic ray induced underground muon flux can be the origin of the modulation. In addition, we provide [...]]]></description>
			<content:encoded><![CDATA[<p>The DAMA dark matter search experiment observes a statistically significant percent-level variation of its low-energy count rate with a period of one year. In this note we recall some of the arguments which challenge the hypothesis that the cosmic ray induced underground muon flux can be the origin of the modulation. In addition, we provide new comments on recent works on this subject.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/on-the-cosmic-ray-muon-hypothesis-for-dama-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Science Drivers for AGN Observations with the Cherenkov Telescope Array</title>
		<link>http://voxcharta.org/2012/05/16/science-drivers-for-agn-observations-with-the-cherenkov-telescope-array/</link>
		<comments>http://voxcharta.org/2012/05/16/science-drivers-for-agn-observations-with-the-cherenkov-telescope-array/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:45:09 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[array]]></category>
		<category><![CDATA[atmospheric cherenkov telescopes]]></category>
		<category><![CDATA[cta]]></category>
		<category><![CDATA[ebl]]></category>
		<category><![CDATA[invariance principle]]></category>
		<category><![CDATA[jet formation]]></category>
		<category><![CDATA[lorentz invariance]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[photon energy]]></category>
		<category><![CDATA[qualitative overview]]></category>
		<category><![CDATA[related science]]></category>
		<category><![CDATA[relativistic jet]]></category>
		<category><![CDATA[science drivers]]></category>
		<category><![CDATA[science topics]]></category>
		<category><![CDATA[substantial contribution]]></category>
		<category><![CDATA[telescope array]]></category>
		<category><![CDATA[tev gamma rays]]></category>
		<category><![CDATA[VERITAS]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/science-drivers-for-agn-observations-with-the-cherenkov-telescope-array/</guid>
		<description><![CDATA[The current generation of Imaging Atmospheric Cherenkov Telescopes (IACTs), including the H.E.S.S., MAGIC, and VERITAS telescope arrays, have made substantial contributions to our knowledge about the structure and composition of the highly relativistic jets from Active Galactic Nuclei (AGNs). In this paper, we discuss some of the outstanding scientific questions and give a qualitative overview [...]]]></description>
			<content:encoded><![CDATA[<p>The current generation of Imaging Atmospheric Cherenkov Telescopes (IACTs), including the H.E.S.S., MAGIC, and VERITAS telescope arrays, have made substantial contributions to our knowledge about the structure and composition of the highly relativistic jets from Active Galactic Nuclei (AGNs). In this paper, we discuss some of the outstanding scientific questions and give a qualitative overview of AGN related science topics which will be explored with the next-generation Cherenkov Telescope Array (CTA). CTA is expected to further constrain the structure and make-up of jets, and thus, to constrain models of jet formation, acceleration, and collimation. Furthermore, being the brightest well-established extragalactic sources of TeV {\gamma}- rays, AGNs can be used to probe the EBL, intergalactic magnetic fields, and the validity of the Lorentz Invariance principle at high photon energies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/science-drivers-for-agn-observations-with-the-cherenkov-telescope-array/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Discovery of the Optical/Ultraviolet/Gamma-ray Counterpart to the Eclipsing Millisecond Pulsar J1816+4510</title>
		<link>http://voxcharta.org/2012/05/16/discovery-of-the-opticalultravioletgamma-ray-counterpart-to-the-eclipsing-millisecond-pulsar-j18164510/</link>
		<comments>http://voxcharta.org/2012/05/16/discovery-of-the-opticalultravioletgamma-ray-counterpart-to-the-eclipsing-millisecond-pulsar-j18164510/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:44:56 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[coincidence]]></category>
		<category><![CDATA[counterpart]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[efficiency]]></category>
		<category><![CDATA[frequency radio]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[green bank telescope]]></category>
		<category><![CDATA[low frequency]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[mass companions]]></category>
		<category><![CDATA[millisecond pulsar]]></category>
		<category><![CDATA[minimum companion mass]]></category>
		<category><![CDATA[orbital period]]></category>
		<category><![CDATA[pulsars]]></category>
		<category><![CDATA[pulsation]]></category>
		<category><![CDATA[radio survey]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/discovery-of-the-opticalultravioletgamma-ray-counterpart-to-the-eclipsing-millisecond-pulsar-j18164510/</guid>
		<description><![CDATA[The energetic, eclipsing millisecond pulsar J1816+4510 was recently discovered in a low-frequency radio survey with the Green Bank Telescope. With an orbital period of 8.7 hr and minimum companion mass of 0.16 Msun it appears to belong to an increasingly important class of pulsars that are ablating their low-mass companions. We report the discovery of [...]]]></description>
			<content:encoded><![CDATA[<p>The energetic, eclipsing millisecond pulsar J1816+4510 was recently discovered in a low-frequency radio survey with the Green Bank Telescope. With an orbital period of 8.7 hr and minimum companion mass of 0.16 Msun it appears to belong to an increasingly important class of pulsars that are ablating their low-mass companions. We report the discovery of the gamma-ray counterpart to this pulsar, and present a likely optical/ultraviolet counterpart as well. Using the radio ephemeris we detect pulsations in the unclassified gamma-ray source 2FGL J1816.5+4511, implying an efficiency of ~25% in converting the pulsar&#8217;s spin-down luminosity into gamma-rays and adding PSR J1816+4510 to the large number of millisecond pulsars detected by Fermi. The likely optical/UV counterpart was identified through position coincidence (15,000 K it would be among the brightest and hottest of low-mass pulsar companions, and appears qualitatively different from other eclipsing pulsar systems. In particular, current data suggest that it is a factor of two larger than most white dwarfs of its mass, but a factor of four smaller than its Roche lobe. We discuss possible reasons for its high temperature and odd size, and suggest that it recently underwent a violent episode of mass loss. Regardless of origin, its brightness and the relative unimportance of irradiation make it an ideal target for a mass, and hence a neutron star mass, determination.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/discovery-of-the-opticalultravioletgamma-ray-counterpart-to-the-eclipsing-millisecond-pulsar-j18164510/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>X-ray emission from star-forming galaxies &#8211; II. Hot interstellar medium</title>
		<link>http://voxcharta.org/2012/05/16/x-ray-emission-from-star-forming-galaxies-ii-hot-interstellar-medium/</link>
		<comments>http://voxcharta.org/2012/05/16/x-ray-emission-from-star-forming-galaxies-ii-hot-interstellar-medium/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:44:03 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[apparent luminosity]]></category>
		<category><![CDATA[compact source]]></category>
		<category><![CDATA[core collapse supernovae]]></category>
		<category><![CDATA[diffuse emission]]></category>
		<category><![CDATA[host galaxy]]></category>
		<category><![CDATA[interstellar medium]]></category>
		<category><![CDATA[mechanical energy]]></category>
		<category><![CDATA[order of magnitude]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[sfr]]></category>
		<category><![CDATA[source of energy]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[systematic effects]]></category>
		<category><![CDATA[thermal emission]]></category>
		<category><![CDATA[thermal energy]]></category>
		<category><![CDATA[type galaxy]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/x-ray-emission-from-star-forming-galaxies-ii-hot-interstellar-medium/</guid>
		<description><![CDATA[We study the emission from the hot interstellar medium in a sample of nearby late type galaxies defined in the Paper I. Our sample covers a broad range of star formation rates, from ~0.1 Msun/yr to ~17 Msun/yr and stellar masses, from ~3&#215;10^8 Msun to ~6&#215;10^10 Msun. We take special care of systematic effects and [...]]]></description>
			<content:encoded><![CDATA[<p>We study the emission from the hot interstellar medium in a sample of nearby late type galaxies defined in the Paper I. Our sample covers a broad range of star formation rates, from ~0.1 Msun/yr to ~17 Msun/yr and stellar masses, from ~3&#215;10^8 Msun to ~6&#215;10^10 Msun. We take special care of systematic effects and contamination from bright and faint compact sources. We find that in all galaxies at least one optically thin thermal emission component is present in the unresolved emission, with the average temperature of = 0.24 keV. In about ~1/3 of galaxies, a second, higher temperature component is required, with the = 0.71 keV. Although statistically significant variations in temperature between galaxies are present, we did not find any meaningful trends with the stellar mass or star formation rate of the host galaxy. The apparent luminosity of the diffuse emission in the 0.5-2 keV band linearly correlates with the star formation rate with the scale factor of Lx/SFR\dim6.3&#215;10^38 erg/s per Msun/yr, of which about ~45% is likely produced by faint compact sources of various types. We attempt to estimate the bolometric luminosity of the gas and and obtained results differing by an order of magnitude, log(Lbol/SFR)\sim39-40, depending on whether intrinsic absorption in star-forming galaxies was allowed or not. Our theoretically most accurate, but in practice the most model dependent result for the intrinsic bolometric luminosity of ISM is Lbol/SFR\sim1.5&#215;10^40 erg/s per Msun/yr. Assuming that core collapse supernovae are the main source of energy, it implies that \epsilon_SN\sim5&#215;10^-2 (E_SN/10^51)^-1 of mechanical energy of supernovae is converted into thermal energy of ISM.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/x-ray-emission-from-star-forming-galaxies-ii-hot-interstellar-medium/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Multi-wavelength Observations of the Type IIb Supernova 2009mg</title>
		<link>http://voxcharta.org/2012/05/16/multi-wavelength-observations-of-the-type-iib-supernova-2009mg/</link>
		<comments>http://voxcharta.org/2012/05/16/multi-wavelength-observations-of-the-type-iib-supernova-2009mg/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:42:13 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[decay rate]]></category>
		<category><![CDATA[ejecta]]></category>
		<category><![CDATA[galaxy eso]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[mass distribution]]></category>
		<category><![CDATA[mass loss]]></category>
		<category><![CDATA[minor differences]]></category>
		<category><![CDATA[observational properties]]></category>
		<category><![CDATA[progenitor]]></category>
		<category><![CDATA[prototype]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[temporal index]]></category>
		<category><![CDATA[type iib]]></category>
		<category><![CDATA[u band]]></category>
		<category><![CDATA[upturn]]></category>
		<category><![CDATA[wavelength]]></category>
		<category><![CDATA[xrt]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/multi-wavelength-observations-of-the-type-iib-supernova-2009mg/</guid>
		<description><![CDATA[We present Swift UVOT and XRT observations, and visual wavelength spectroscopy of the Type IIb supernova (SN) 2009mg, discovered in the Sb galaxy ESO 121-G26. The observational properties of SN 2009mg are compared to the prototype Type IIb SNe 1993J and 2008ax, with which we find many similarities. However, minor differences are discernible including SN [...]]]></description>
			<content:encoded><![CDATA[<p>We present Swift UVOT and XRT observations, and visual wavelength spectroscopy of the Type IIb supernova (SN) 2009mg, discovered in the Sb galaxy ESO 121-G26. The observational properties of SN 2009mg are compared to the prototype Type IIb SNe 1993J and 2008ax, with which we find many similarities. However, minor differences are discernible including SN 2009mg not exhibiting an initial fast decline or u-band upturn as observed in the comparison objects, and its rise to maximum is somewhat slower leading to slightly broader light curves. The late-time temporal index of SN 2009mg, determined from 40 days post-explosion, is consistent with the decay rate of SN 1993J, but inconsistent with the decay of 56Co. This suggests leakage of gamma-rays out of the ejecta and a stellar mass on the small side of the mass distribution. Our XRT non-detection provides an upper limit on the mass-loss rate of the progenitor of &lt;1.5&#215;10^-5 Msun per yr. Modelling of the SN light curve indicates a kinetic energy of 0.15 (+0.02,-0.13) x10^51 erg, an ejecta mass of 0.56(+0.10,-0.26) Msun and a 56Ni mass of 0.10\pm0.01 Msun.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/multi-wavelength-observations-of-the-type-iib-supernova-2009mg/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Tests of the universality of free fall for strongly self-gravitating bodies with radio pulsars [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/16/tests-of-the-universality-of-free-fall-for-strongly-self-gravitating-bodies-with-radio-pulsars-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/16/tests-of-the-universality-of-free-fall-for-strongly-self-gravitating-bodies-with-radio-pulsars-cross-listing/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:41:56 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[binary system]]></category>
		<category><![CDATA[binding energy]]></category>
		<category><![CDATA[equivalence principle]]></category>
		<category><![CDATA[extreme difference]]></category>
		<category><![CDATA[future prospect]]></category>
		<category><![CDATA[globular cluster]]></category>
		<category><![CDATA[measurement precision]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[orbital eccentricity]]></category>
		<category><![CDATA[orbital motion]]></category>
		<category><![CDATA[phenomenon]]></category>
		<category><![CDATA[precise measurement]]></category>
		<category><![CDATA[probabilistic considerations]]></category>
		<category><![CDATA[pulsar data]]></category>
		<category><![CDATA[radiation]]></category>
		<category><![CDATA[radio pulsar]]></category>
		<category><![CDATA[types of tests]]></category>
		<category><![CDATA[universality]]></category>
		<category><![CDATA[variation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/tests-of-the-universality-of-free-fall-for-strongly-self-gravitating-bodies-with-radio-pulsars-cross-listing/</guid>
		<description><![CDATA[In this paper, we review tests of the strong equivalence principle (SEP) derived from binary pulsar data. The extreme difference in binding energy between both components and the precise measurement of the orbital motion provided by pulsar timing allow the only current precision SEP tests for strongly self-gravitating bodies. We start by highlighting why such [...]]]></description>
			<content:encoded><![CDATA[<p>In this paper, we review tests of the strong equivalence principle (SEP) derived from binary pulsar data. The extreme difference in binding energy between both components and the precise measurement of the orbital motion provided by pulsar timing allow the only current precision SEP tests for strongly self-gravitating bodies. We start by highlighting why such tests are conceptually important. We then review previous work where limits on SEP violation are obtained with an ensemble of wide binary systems with small eccentricity orbits. Then we propose a new SEP violation test based on the measurement of the variation of the orbital eccentricity de/dt. This new method has the following advantages: a) unlike previous methods it is not based on probabilistic considerations, b) it can make a direct detection of SEP violation, c) the measurement of de/dt is not contaminated by any known external effects, which implies that this SEP test is only restricted by the measurement precision of de/dt. In the final part of the review, we conceptually compare the SEP test with the test for dipolar radiation damping, a phenomenon closely related to SEP violation, and speculate on future prospects by new types of tests in globular clusters and future triple systems.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/tests-of-the-universality-of-free-fall-for-strongly-self-gravitating-bodies-with-radio-pulsars-cross-listing/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>Origin of the GeV Emission During the X-ray Flaring Activity in GRB 100728A [Replacement]</title>
		<link>http://voxcharta.org/2012/05/16/origin-of-the-gev-emission-during-the-x-ray-flaring-activity-in-grb-100728a-replacement/</link>
		<comments>http://voxcharta.org/2012/05/16/origin-of-the-gev-emission-during-the-x-ray-flaring-activity-in-grb-100728a-replacement/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:38:52 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[flare]]></category>
		<category><![CDATA[forward shock]]></category>
		<category><![CDATA[inverse compton]]></category>
		<category><![CDATA[photon]]></category>
		<category><![CDATA[relativistic electron]]></category>
		<category><![CDATA[scattering effect]]></category>
		<category><![CDATA[scenarios]]></category>
		<category><![CDATA[spectral property]]></category>
		<category><![CDATA[spectrum]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/origin-of-the-gev-emission-during-the-x-ray-flaring-activity-in-grb-100728a-replacement/</guid>
		<description><![CDATA[Recently, Fermi-LAT detected GeV emission during the X-ray flaring activity in GRB 100728A. We study various scenarios for its origin. The hard spectrum of the GeV emission favors the external inverse-Compton origin in which X-ray flare photons are up-scattered by relativistic electrons in the external forward shock. This external IC scenario, with anisotropic scattering effect [...]]]></description>
			<content:encoded><![CDATA[<p>Recently, Fermi-LAT detected GeV emission during the X-ray flaring activity in GRB 100728A. We study various scenarios for its origin. The hard spectrum of the GeV emission favors the external inverse-Compton origin in which X-ray flare photons are up-scattered by relativistic electrons in the external forward shock. This external IC scenario, with anisotropic scattering effect taken into account, can reproduce the temporal and spectral properties of the GeV emission in GRB 100728A.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/origin-of-the-gev-emission-during-the-x-ray-flaring-activity-in-grb-100728a-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Deep Crustal Heating in a Multicomponent Accreted Neutron Star Crust [Replacement]</title>
		<link>http://voxcharta.org/2012/05/16/deep-crustal-heating-in-a-multicomponent-accreted-neutron-star-crust-replacement/</link>
		<comments>http://voxcharta.org/2012/05/16/deep-crustal-heating-in-a-multicomponent-accreted-neutron-star-crust-replacement/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:37:14 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[composition]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[electron]]></category>
		<category><![CDATA[emission]]></category>
		<category><![CDATA[energy change]]></category>
		<category><![CDATA[liquid droplet]]></category>
		<category><![CDATA[mass model]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[nuclear mass]]></category>
		<category><![CDATA[nuclei]]></category>
		<category><![CDATA[nucleosynthesis]]></category>
		<category><![CDATA[reaction pathways]]></category>
		<category><![CDATA[shell]]></category>
		<category><![CDATA[statistical equilibrium model]]></category>
		<category><![CDATA[symmetry]]></category>
		<category><![CDATA[transition]]></category>
		<category><![CDATA[uncertainty]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/deep-crustal-heating-in-a-multicomponent-accreted-neutron-star-crust-replacement/</guid>
		<description><![CDATA[A quasi-statistical equilibrium model is constructed to simulate the multicomponent composition of the crust of an accreting neutron star. The ashes of rp-process nucleosynthesis are driven by accretion through a series of electron captures, neutron emissions, and pycnonuclear fusions up to densities near the transition between the neutron star crust and core. A liquid droplet [...]]]></description>
			<content:encoded><![CDATA[<p>A quasi-statistical equilibrium model is constructed to simulate the multicomponent composition of the crust of an accreting neutron star. The ashes of rp-process nucleosynthesis are driven by accretion through a series of electron captures, neutron emissions, and pycnonuclear fusions up to densities near the transition between the neutron star crust and core. A liquid droplet model which includes nuclear shell effects is used to provide nuclear masses far from stability. Reaction pathways are determined consistently with the nuclear mass model. The nuclear symmetry energy is an important uncertainty in the masses of the exotic nuclei in the inner crust and varying the symmetry energy changes the amount of deep crustal heating by as much as a factor of two.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/deep-crustal-heating-in-a-multicomponent-accreted-neutron-star-crust-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Growth of magnetic fields in accreting millisecond pulsars: the case of J1823-3021A [Replacement]</title>
		<link>http://voxcharta.org/2012/05/16/growth-of-magnetic-fields-in-accreting-millisecond-pulsars-the-case-of-j1823-3021a-replacement/</link>
		<comments>http://voxcharta.org/2012/05/16/growth-of-magnetic-fields-in-accreting-millisecond-pulsars-the-case-of-j1823-3021a-replacement/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:36:51 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[collaboration]]></category>
		<category><![CDATA[diffusion]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[enhancement]]></category>
		<category><![CDATA[external magnetic field]]></category>
		<category><![CDATA[first evidence]]></category>
		<category><![CDATA[internal magnetic field]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[millisecond pulsar]]></category>
		<category><![CDATA[modes]]></category>
		<category><![CDATA[pulsation]]></category>
		<category><![CDATA[radius]]></category>
		<category><![CDATA[rotation period]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/growth-of-magnetic-fields-in-accreting-millisecond-pulsars-the-case-of-j1823-3021a-replacement/</guid>
		<description><![CDATA[The Fermi LAT collaboration has recently reported the discovery of the pulsations of the $\gamma$ ray pulsar J1823-3021A with a luminosity which is the highest observed to date for any millisecond pulsar (MSP). This large luminosity implies a large spin down rate $\dot P$ and therefore a large magnetic field which seems to be incompatible [...]]]></description>
			<content:encoded><![CDATA[<p>The Fermi LAT collaboration has recently reported the discovery of the pulsations of the $\gamma$ ray pulsar J1823-3021A with a luminosity which is the highest observed to date for any millisecond pulsar (MSP). This large luminosity implies a large spin down rate $\dot P$ and therefore a large magnetic field which seems to be incompatible with the observed short rotation period $P$. A possible explanation for the observed $P$ and $\dot P$ is to assume a very small radius for the star but it turns out that this interpretation requires rather extreme astrophysical conditions. Here we show that the data can be explained by considering the increase of the external magnetic field due to the diffusion of an internal magnetic field generated by r-modes during mass accretion. Our analysis offers a first evidence of the strong enhancement of the internal magnetic field due to the r-modes, what has been proposed in several papers. Moreover, the diffusion of the internal magnetic field provides a new evolutionary path for millisecond pulsars.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/growth-of-magnetic-fields-in-accreting-millisecond-pulsars-the-case-of-j1823-3021a-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>General Relativistic Simulations of Magnetized Plasmas around Merging Supermassive Black Holes [Replacement]</title>
		<link>http://voxcharta.org/2012/05/16/general-relativistic-simulations-of-magnetized-plasmas-around-merging-supermassive-black-holes-replacement/</link>
		<comments>http://voxcharta.org/2012/05/16/general-relativistic-simulations-of-magnetized-plasmas-around-merging-supermassive-black-holes-replacement/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:35:31 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[amplification]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[counterpart]]></category>
		<category><![CDATA[electromagnetic signal]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[hole binaries]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetic field strength]]></category>
		<category><![CDATA[merger]]></category>
		<category><![CDATA[orders of magnitude]]></category>
		<category><![CDATA[plasma]]></category>
		<category><![CDATA[possible emission]]></category>
		<category><![CDATA[regime]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[supermassive black hole]]></category>
		<category><![CDATA[whisky]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/general-relativistic-simulations-of-magnetized-plasmas-around-merging-supermassive-black-holes-replacement/</guid>
		<description><![CDATA[Coalescing supermassive black hole binaries are produced by the mergers of galaxies and are the most powerful sources of gravitational waves accessible to space-based gravitational observatories. Some such mergers may occur in the presence of matter and magnetic fields and hence generate an electromagnetic counterpart. In this Letter, we present the first general relativistic simulations [...]]]></description>
			<content:encoded><![CDATA[<p>Coalescing supermassive black hole binaries are produced by the mergers of galaxies and are the most powerful sources of gravitational waves accessible to space-based gravitational observatories. Some such mergers may occur in the presence of matter and magnetic fields and hence generate an electromagnetic counterpart. In this Letter, we present the first general relativistic simulations of magnetized plasma around merging supermassive black holes using the general relativistic magnetohydrodynamic code Whisky. By considering different magnetic field strengths, going from non-magnetically dominated to magnetically dominated regimes, we explore how magnetic fields affect the dynamics of the plasma and the possible emission of electromagnetic signals. In particular we observe a total amplification of the magnetic field of ~2 orders of magnitude which is driven by the accretion onto the binary and that leads to much stronger electromagnetic signals, more than a factor of 10^4 larger than comparable calculations done in the force-free regime where such amplifications are not possible.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/general-relativistic-simulations-of-magnetized-plasmas-around-merging-supermassive-black-holes-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A new low magnetic field magnetar: the 2011 outburst of Swift J1822.3-1606 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/16/a-new-low-magnetic-field-magnetar-the-2011-outburst-of-swift-j1822-3-1606-replacement/</link>
		<comments>http://voxcharta.org/2012/05/16/a-new-low-magnetic-field-magnetar-the-2011-outburst-of-swift-j1822-3-1606-replacement/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:34:53 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[dipolar]]></category>
		<category><![CDATA[gbt]]></category>
		<category><![CDATA[gran telescopio canarias]]></category>
		<category><![CDATA[green bank telescope]]></category>
		<category><![CDATA[kyr]]></category>
		<category><![CDATA[magnetar]]></category>
		<category><![CDATA[optical emission]]></category>
		<category><![CDATA[order of magnitude]]></category>
		<category><![CDATA[outburst]]></category>
		<category><![CDATA[quiescent state]]></category>
		<category><![CDATA[Ray Bursts]]></category>
		<category><![CDATA[rosat observations]]></category>
		<category><![CDATA[rxte]]></category>
		<category><![CDATA[spectral evolution]]></category>
		<category><![CDATA[suzaku]]></category>
		<category><![CDATA[thermal evolution]]></category>
		<category><![CDATA[time span]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xmm newton]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/a-new-low-magnetic-field-magnetar-the-2011-outburst-of-swift-j1822-3-1606-replacement/</guid>
		<description><![CDATA[We report on the long term X-ray monitoring with Swift, RXTE, Suzaku, Chandra and XMM-Newton of the outburst of the newly discovered magnetar Swift J1822.3-1606 (SGR 1822-1606), from the first observations soon after the detection of the short X-ray bursts which led to its discovery, through the first stages of its outburst decay (covering the [...]]]></description>
			<content:encoded><![CDATA[<p>We report on the long term X-ray monitoring with Swift, RXTE, Suzaku, Chandra and XMM-Newton of the outburst of the newly discovered magnetar Swift J1822.3-1606 (SGR 1822-1606), from the first observations soon after the detection of the short X-ray bursts which led to its discovery, through the first stages of its outburst decay (covering the time-span from July 2011, until end of April 2012). We also report on archival ROSAT observations which witnessed the source during its likely quiescent state, and on upper limits on Swift J1822.3-1606&#8217;s radio-pulsed and optical emission during outburst, with the Green Bank Telescope (GBT) and the Gran Telescopio Canarias (GTC), respectively. Our X-ray timing analysis finds the source rotating with a period of P=8.43772016(2) s and a period derivative \dot{P}=8.3(2)x10^{-14} s s^{-1} , which entails an inferred dipolar surface magnetic field of B~2.7&#215;10^{13} G at the equator. This measurement makes Swift J1822.3-1606 the second lowest magnetic field magnetar (after SGR 0418+5729; Rea et al. 2010). Following the flux and spectral evolution from the beginning of the outburst, we find that the flux decreased by about an order of magnitude, with a subtle softening of the spectrum, both typical of the outburst decay of magnetars. By modeling the secular thermal evolution of Swift J1822.3-1606, we find that the observed timing properties of the source, as well as its quiescent X-ray luminosity, can be reproduced if it was born with a poloidal and crustal toroidal fields of B_{p}~1.5&#215;10^{14} G and B_{tor}~7&#215;10^{14} G, respectively, and if its current age is ~550 kyr.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/a-new-low-magnetic-field-magnetar-the-2011-outburst-of-swift-j1822-3-1606-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Diskoseismology and QPOs Confront Black Hole Spin [Replacement]</title>
		<link>http://voxcharta.org/2012/05/16/diskoseismology-and-qpos-confront-black-hole-spin-replacement/</link>
		<comments>http://voxcharta.org/2012/05/16/diskoseismology-and-qpos-confront-black-hole-spin-replacement/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:32:53 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absence]]></category>
		<category><![CDATA[accretion disk]]></category>
		<category><![CDATA[angular momentum]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[circular orbit]]></category>
		<category><![CDATA[continuum]]></category>
		<category><![CDATA[determinations]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[oscillation]]></category>
		<category><![CDATA[periodic oscillation]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/diskoseismology-and-qpos-confront-black-hole-spin-replacement/</guid>
		<description><![CDATA[We compare the determinations of the angular momentum of stellar mass black holes via the continuum and line methods with those from diskoseismology. The assumption being tested is that one of the QPOs (quasi-periodic oscillations) in each binary X-ray source is produced by the fundamental g-mode. This should be the most robust and visible normal [...]]]></description>
			<content:encoded><![CDATA[<p>We compare the determinations of the angular momentum of stellar mass black holes via the continuum and line methods with those from diskoseismology. The assumption being tested is that one of the QPOs (quasi-periodic oscillations) in each binary X-ray source is produced by the fundamental g-mode. This should be the most robust and visible normal mode of oscillation of the accretion disk, and therefore its absence should rule out diskoseismology as the origin of QPOs. The comparisons are consistent with the second highest frequency QPO being produced by this g-mode, but are not consistent with models in which one QPO frequency is that of the innermost stable circular orbit.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/diskoseismology-and-qpos-confront-black-hole-spin-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>GRB 091208B: First Detection of the Optical Polarization in Early Forward Shock Emission of a Gamma-Ray Burst Afterglow [Replacement]</title>
		<link>http://voxcharta.org/2012/05/16/grb-091208b-first-detection-of-the-optical-polarization-in-early-forward-shock-emission-of-a-gamma-ray-burst-afterglow-replacement-2/</link>
		<comments>http://voxcharta.org/2012/05/16/grb-091208b-first-detection-of-the-optical-polarization-in-early-forward-shock-emission-of-a-gamma-ray-burst-afterglow-replacement-2/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:32:34 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[angle]]></category>
		<category><![CDATA[decay]]></category>
		<category><![CDATA[emission region]]></category>
		<category><![CDATA[forward shock]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[optical light curve]]></category>
		<category><![CDATA[plasma]]></category>
		<category><![CDATA[polarization]]></category>
		<category><![CDATA[skin depth]]></category>
		<category><![CDATA[temporal change]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/grb-091208b-first-detection-of-the-optical-polarization-in-early-forward-shock-emission-of-a-gamma-ray-burst-afterglow-replacement-2/</guid>
		<description><![CDATA[We report that the optical polarization in the afterglow of GRB 091208B is measured at t = 149 &#8211; 706 s after the burst trigger, and the polarization degree is P = 10.4% +/- 2.5%. The optical light curve at this time shows a power-law decay with index -0.75 +/- 0.02, which is interpreted as [...]]]></description>
			<content:encoded><![CDATA[<p>We report that the optical polarization in the afterglow of GRB 091208B is measured at t = 149 &#8211; 706 s after the burst trigger, and the polarization degree is P = 10.4% +/- 2.5%. The optical light curve at this time shows a power-law decay with index -0.75 +/- 0.02, which is interpreted as the forward shock synchrotron emission, and thus this is the first detection of the early-time optical polarization in the forward shock (rather than that in the reverse shock reported by Steele et al. (2009). This detection disfavors the afterglow model in which the magnetic fields in the emission region are random on the plasma skin depth scales, such as amplified by the plasma instabilities, e.g., Weibel instability. We suggest that the fields are amplified by the magnetohydrodynamic instabilities, which would be tested by future observations of the temporal changes of the polarization degrees and angles for other bursts.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/grb-091208b-first-detection-of-the-optical-polarization-in-early-forward-shock-emission-of-a-gamma-ray-burst-afterglow-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Neutrinos And Cosmic Rays From Gamma Ray Bursts [Replacement]</title>
		<link>http://voxcharta.org/2012/05/16/neutrinos-and-cosmic-rays-from-gamma-ray-bursts-replacement/</link>
		<comments>http://voxcharta.org/2012/05/16/neutrinos-and-cosmic-rays-from-gamma-ray-bursts-replacement/#comments</comments>
		<pubDate>Thu, 17 May 2012 00:31:14 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[collaboration]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[energy neutrino]]></category>
		<category><![CDATA[fireball]]></category>
		<category><![CDATA[gamma ray burst]]></category>
		<category><![CDATA[grbs]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[main source]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/16/neutrinos-and-cosmic-rays-from-gamma-ray-bursts-replacement/</guid>
		<description><![CDATA[The upper limit on the flux of ultra high energy neutrinos from gamma-ray bursts (GRBs) that was reported recently by the IceCube collaboration contradicts predictions based on the Fireball model of GRBs, but does not exclude GRBs as a main source of ultra-high energy cosmic rays.
]]></description>
			<content:encoded><![CDATA[<p>The upper limit on the flux of ultra high energy neutrinos from gamma-ray bursts (GRBs) that was reported recently by the IceCube collaboration contradicts predictions based on the Fireball model of GRBs, but does not exclude GRBs as a main source of ultra-high energy cosmic rays.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/16/neutrinos-and-cosmic-rays-from-gamma-ray-bursts-replacement/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 optically unbiased GRB host (TOUGH) survey. I. Survey design and catalogs</title>
		<link>http://voxcharta.org/2012/05/15/the-optically-unbiased-grb-host-tough-survey-i-survey-design-and-catalogs/</link>
		<comments>http://voxcharta.org/2012/05/15/the-optically-unbiased-grb-host-tough-survey-i-survey-design-and-catalogs/#comments</comments>
		<pubDate>Wed, 16 May 2012 01:06:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[alpha emission]]></category>
		<category><![CDATA[completeness]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[energy properties]]></category>
		<category><![CDATA[gamma ray burst]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[host galaxy]]></category>
		<category><![CDATA[lyman]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[optical afterglow]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[selection criteria]]></category>
		<category><![CDATA[statistical study]]></category>
		<category><![CDATA[survey design]]></category>
		<category><![CDATA[swift grb]]></category>
		<category><![CDATA[Telescope]]></category>
		<category><![CDATA[tracers]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/the-optically-unbiased-grb-host-tough-survey-i-survey-design-and-catalogs/</guid>
		<description><![CDATA[Long-duration gamma-ray bursts (GRBs) are powerful tracers of star-forming galaxies at a very wide range of redshifts. We have defined a homogeneous subsample of 69 Swift GRB-selected galaxies. Special attention has been devoted to making the sample optically unbiased through simple and well-defined selection criteria based on the high-energy properties of the bursts and their [...]]]></description>
			<content:encoded><![CDATA[<p>Long-duration gamma-ray bursts (GRBs) are powerful tracers of star-forming galaxies at a very wide range of redshifts. We have defined a homogeneous subsample of 69 Swift GRB-selected galaxies. Special attention has been devoted to making the sample optically unbiased through simple and well-defined selection criteria based on the high-energy properties of the bursts and their positions on the sky. Thanks to our extensive follow-up observations, this sample has now achieved a comparatively high degree of redshift completeness, and thus provides a legacy sample, useful for statistical studies of GRBs and their host galaxies. In this paper we present the survey design and summarize the results of our observing program conducted at the ESO Very Large Telescope aimed at obtaining the most basic properties of galaxies in this sample, including a catalog of R and K magnitudes and redshifts. We detect the host galaxies for 80 % of the GRBs in the sample, although only 42 % Ks-band detections, which confirms that GRB-selected host galaxies are generally blue. The sample is not uniformly blue, however, with two extremely red objects detected. Moreover, galaxies hosting GRBs with no optical afterglows, whose identification therefore relies on X-ray localisations, are significantly brighter and redder than those with an optical afterglow. Our spectroscopic campaign has resulted in 77 % now having redshift measurements, with a median redshift of 2.14 +- 0.18. TOUGH alone consists of 17 detected z &gt; 2 Swift GRB host galaxies suitable for individual and statistical studies. Seven hosts have detections of the Ly-alpha emission line and we can exclude an early indication that Ly-alpha emission is ubiquitous among GRB hosts, but confirm that Ly-alpha is stronger in GRB-selected galaxies than in flux-limited samples of Lyman break galaxies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/the-optically-unbiased-grb-host-tough-survey-i-survey-design-and-catalogs/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>The Central Engine Structure of 3C120: Evidence for a Retrograde Black Hole or a Refilling Accretion Disk</title>
		<link>http://voxcharta.org/2012/05/15/the-central-engine-structure-of-3c120-evidence-for-a-retrograde-black-hole-or-a-refilling-accretion-disk/</link>
		<comments>http://voxcharta.org/2012/05/15/the-central-engine-structure-of-3c120-evidence-for-a-retrograde-black-hole-or-a-refilling-accretion-disk/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:56:14 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion disk]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[circular orbit]]></category>
		<category><![CDATA[confidence level]]></category>
		<category><![CDATA[hxd]]></category>
		<category><![CDATA[inner radius]]></category>
		<category><![CDATA[inner regions]]></category>
		<category><![CDATA[instabilities]]></category>
		<category><![CDATA[iron line]]></category>
		<category><![CDATA[isco]]></category>
		<category><![CDATA[k line]]></category>
		<category><![CDATA[line feature]]></category>
		<category><![CDATA[line radio]]></category>
		<category><![CDATA[radio emission]]></category>
		<category><![CDATA[radio galaxy 3c120]]></category>
		<category><![CDATA[reanalysis]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xis]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/the-central-engine-structure-of-3c120-evidence-for-a-retrograde-black-hole-or-a-refilling-accretion-disk/</guid>
		<description><![CDATA[The broad-line radio galaxy 3C120 is a powerful source of both X-ray and radio emission including superluminal jet outflows. We report on our reanalysis of 160 ks of Suzaku data taken in 2006, previously examined by Kataoka et al. (2007). Spectral fits to the XIS and HXD/PIN data over a range of 0.7-45 keV reveal [...]]]></description>
			<content:encoded><![CDATA[<p>The broad-line radio galaxy 3C120 is a powerful source of both X-ray and radio emission including superluminal jet outflows. We report on our reanalysis of 160 ks of Suzaku data taken in 2006, previously examined by Kataoka et al. (2007). Spectral fits to the XIS and HXD/PIN data over a range of 0.7-45 keV reveal a well-defined iron K line complex with a narrow Ka core and relativistically broadened features consistent with emission from the inner regions of the accretion disk. Furthermore, the inner region of the disk appears to be truncated with an inner radius of r_in = 11.7^{+3.5}_{-5.2} r_g. If we assume that fluorescent iron line features terminate at the inner-most stable circular orbit (ISCO), we measure a black hole spin of a  0.8) can be ruled out at the 99% confidence level. Alternatively, the disk may be truncated well outside of the ISCO of a rapid prograde hole. The most compelling scenario is the possibility that the inner regions of the disk were destroyed/ejected by catastrophic instabilities just prior to the time these observations were made.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/the-central-engine-structure-of-3c120-evidence-for-a-retrograde-black-hole-or-a-refilling-accretion-disk/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Understanding X-ray reflection emissivity profiles in AGN: Locating the X-ray source</title>
		<link>http://voxcharta.org/2012/05/15/understanding-x-ray-reflection-emissivity-profiles-in-agn-locating-the-x-ray-source/</link>
		<comments>http://voxcharta.org/2012/05/15/understanding-x-ray-reflection-emissivity-profiles-in-agn-locating-the-x-ray-source/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:54:28 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion disc]]></category>
		<category><![CDATA[AGN]]></category>
		<category><![CDATA[constant power]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[general relativity]]></category>
		<category><![CDATA[geometry]]></category>
		<category><![CDATA[illumination pattern]]></category>
		<category><![CDATA[inner regions]]></category>
		<category><![CDATA[point source]]></category>
		<category><![CDATA[processing unit]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[ray tracing]]></category>
		<category><![CDATA[relativistic effects]]></category>
		<category><![CDATA[relativistic ray]]></category>
		<category><![CDATA[reverberation time]]></category>
		<category><![CDATA[source location]]></category>
		<category><![CDATA[trajectory]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/understanding-x-ray-reflection-emissivity-profiles-in-agn-locating-the-x-ray-source/</guid>
		<description><![CDATA[The illumination pattern (or emissivity profile) of the accretion disc due to the reflection of X-rays in AGN can be understood in terms of relativistic effects on the rays propagating from a source in a corona surrounding the central black hole, both on their trajectories and on the accretion disc itself. Theoretical emissivity profiles due [...]]]></description>
			<content:encoded><![CDATA[<p>The illumination pattern (or emissivity profile) of the accretion disc due to the reflection of X-rays in AGN can be understood in terms of relativistic effects on the rays propagating from a source in a corona surrounding the central black hole, both on their trajectories and on the accretion disc itself. Theoretical emissivity profiles due to isotropic point sources as well as simple extended geometries are computed in general relativistic ray tracing simulations performed on graphics processing units (GPUs). Such simulations assuming only general relativity naturally explain the accretion disc emissivity profiles determined from relativistically broadened emission lines which fall off steeply (with power law indices of between 6 and 8) over the inner regions of the disc, then flattening off to almost a constant before tending to a constant power law of index 3 over the outer disc. Simulations for a variety of source locations, extents and geometries show how the emissivity profiles depend on these properties, and when combined with reverberation time lags allow the location and extent of the primary X-ray source to be constrained. Comparing the emissivity profile determined from the broadened iron K emission line in spectra of 1H 0707-495 obtained in January 2008 to theoretical emissivity profiles and applying constraints from reverberation lags suggest that there exists an extended region of primary X-ray emission located as low as 2rg above the accretion disc, extending outwards to a radius of around 30rg.</p>
]]></content:encoded>
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		<title>Tidal acceleration of black holes and superradiance [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/15/tidal-acceleration-of-black-holes-and-superradiance-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/15/tidal-acceleration-of-black-holes-and-superradiance-cross-listing/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:54:14 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration]]></category>
		<category><![CDATA[binaries]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[consequence]]></category>
		<category><![CDATA[degrees of freedom]]></category>
		<category><![CDATA[dipole moment]]></category>
		<category><![CDATA[earth moon]]></category>
		<category><![CDATA[event horizon]]></category>
		<category><![CDATA[general relativity]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[guise]]></category>
		<category><![CDATA[hinge]]></category>
		<category><![CDATA[imprints]]></category>
		<category><![CDATA[moon distance]]></category>
		<category><![CDATA[orders of magnitude]]></category>
		<category><![CDATA[polarization]]></category>
		<category><![CDATA[synchronous rotation]]></category>
		<category><![CDATA[tidal effect]]></category>
		<category><![CDATA[wave observations]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/tidal-acceleration-of-black-holes-and-superradiance-cross-listing/</guid>
		<description><![CDATA[Tidal effects have long ago locked the Moon in synchronous rotation with the Earth and progressively increase the Earth-Moon distance. This &#8220;tidal acceleration&#8221; hinges on dissipation. Binaries containing black holes may also be tidally accelerated, dissipation being caused by the event horizon &#8211; a flexible, viscous one-way membrane. In fact, this process is known for [...]]]></description>
			<content:encoded><![CDATA[<p>Tidal effects have long ago locked the Moon in synchronous rotation with the Earth and progressively increase the Earth-Moon distance. This &#8220;tidal acceleration&#8221; hinges on dissipation. Binaries containing black holes may also be tidally accelerated, dissipation being caused by the event horizon &#8211; a flexible, viscous one-way membrane. In fact, this process is known for many years under a different guise: superradiance. In General Relativity, tidal acceleration is obscured by gravitational-wave emission. However, when coupling to light scalar degrees of freedom is allowed, an induced dipole moment produces a &#8220;polarization acceleration&#8221;, which might be orders of magnitude stronger than tidal quadrupolar effects. Consequences for optical and gravitational-wave observations are intriguing and it is not impossible that imprints of such mechanism have already been observed.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
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		<title>Beaming and rapid variability of high-energy radiation from relativistic pair plasma reconnection</title>
		<link>http://voxcharta.org/2012/05/15/beaming-and-rapid-variability-of-high-energy-radiation-from-relativistic-pair-plasma-reconnection/</link>
		<comments>http://voxcharta.org/2012/05/15/beaming-and-rapid-variability-of-high-energy-radiation-from-relativistic-pair-plasma-reconnection/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:51:05 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[angular distribution]]></category>
		<category><![CDATA[anisotropy]]></category>
		<category><![CDATA[cell simulation]]></category>
		<category><![CDATA[crab nebula]]></category>
		<category><![CDATA[dimensional particle]]></category>
		<category><![CDATA[doppler]]></category>
		<category><![CDATA[electron positron]]></category>
		<category><![CDATA[energetic particle]]></category>
		<category><![CDATA[energy radiation]]></category>
		<category><![CDATA[external observer]]></category>
		<category><![CDATA[fast time]]></category>
		<category><![CDATA[flare]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[high energy astrophysics]]></category>
		<category><![CDATA[line of sight]]></category>
		<category><![CDATA[photon]]></category>
		<category><![CDATA[plasma]]></category>
		<category><![CDATA[signature]]></category>
		<category><![CDATA[synchrotron emission]]></category>
		<category><![CDATA[time variability]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/beaming-and-rapid-variability-of-high-energy-radiation-from-relativistic-pair-plasma-reconnection/</guid>
		<description><![CDATA[We report on the first study of angular distributions of energetic particles and radiation generated in relativistic collisionless electron-positron pair plasma reconnection, using two-dimensional particle-in-cell simulations. We discover a strong anisotropy of the particles accelerated by reconnection and the associated strong beaming of their radiation. The focusing of particles and radiation increases with their energy; [...]]]></description>
			<content:encoded><![CDATA[<p>We report on the first study of angular distributions of energetic particles and radiation generated in relativistic collisionless electron-positron pair plasma reconnection, using two-dimensional particle-in-cell simulations. We discover a strong anisotropy of the particles accelerated by reconnection and the associated strong beaming of their radiation. The focusing of particles and radiation increases with their energy; in this sense, this &#8220;kinetic beaming&#8221; effect differs fundamentally from the relativistic Doppler beaming usually invoked in high-energy astrophysics, in which all photons are focused and boosted achromatically. We also present, for the first time, the modeling of the synchrotron emission as seen by an external observer during the reconnection process. The lightcurves exhibit super-fast time variability, comprising several bright symmetric bursts lasting about one tenth the light-crossing time of the system. The rapid variability in observed radiation is caused by the energetic beam of particles sweeping across the line of sight. This radiative signature can account for the brightness and variability of the gamma-ray flares in the Crab Nebula and in blazars.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
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		<title>Observational signatures of sub-photospheric radiation mediated shocks in the prompt phase of GRBs</title>
		<link>http://voxcharta.org/2012/05/15/observational-signatures-of-sub-photospheric-radiation-mediated-shocks-in-the-prompt-phase-of-grbs/</link>
		<comments>http://voxcharta.org/2012/05/15/observational-signatures-of-sub-photospheric-radiation-mediated-shocks-in-the-prompt-phase-of-grbs/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:50:26 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[characteristic scale]]></category>
		<category><![CDATA[collisionless shocks]]></category>
		<category><![CDATA[compton]]></category>
		<category><![CDATA[geometry]]></category>
		<category><![CDATA[grbs]]></category>
		<category><![CDATA[magnitude]]></category>
		<category><![CDATA[observational signature]]></category>
		<category><![CDATA[optical depth]]></category>
		<category><![CDATA[outflow]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[photosphere]]></category>
		<category><![CDATA[properties of radiation]]></category>
		<category><![CDATA[shape]]></category>
		<category><![CDATA[shock transition]]></category>
		<category><![CDATA[slope]]></category>
		<category><![CDATA[spectrum]]></category>
		<category><![CDATA[temperature profile]]></category>
		<category><![CDATA[thomson]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/observational-signatures-of-sub-photospheric-radiation-mediated-shocks-in-the-prompt-phase-of-grbs/</guid>
		<description><![CDATA[A shock that form below the photosphere of a GRB outflow is mediated by Compton scattering of radiation advected into the shock by the upstream fluid. The characteristic scale of such a shock, a few Thomson depths, is larger than any kinetic scale involved by several orders of magnitudes, hence, unlike collisionless shocks, radiation mediated [...]]]></description>
			<content:encoded><![CDATA[<p>A shock that form below the photosphere of a GRB outflow is mediated by Compton scattering of radiation advected into the shock by the upstream fluid. The characteristic scale of such a shock, a few Thomson depths, is larger than any kinetic scale involved by several orders of magnitudes, hence, unlike collisionless shocks, radiation mediated shocks cannot accelerate particles to non-thermal energies. The spectrum emitted from a shock that breaks out of the photosphere of a GRB jet, reflects the temperature profile downstream of the shock, with a possible contribution at the highest energies from the shock transition layer itself. We study the properties of radiation mediated shocks that form during the prompt phase of GRBs, and compute the time integrated spectrum emitted by the shocked fluid following shock breakout. We show that for shocks that form just below the photosphere, at optical depths $\tau\simlt10$, the emitted spectrum has a Wien shape. The time integrated spectrum emitted from shocks that form at moderate optical depths is modified by adiabatic cooling. Typically, it exhibits a thermal peak with a power law extension that depends on the geometry of the unshocked jet, with $\nu F_\nu\propto\nu^{-1/2}$ for a conical jet, and a steeper slope for a collimating jet. At large optical depths, $\tau\simgt10^3$, thermalization processes affect the shape of the emitted spectrum.</p>
]]></content:encoded>
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		<title>A New Code for Proto-Neutron Star Evolution</title>
		<link>http://voxcharta.org/2012/05/15/a-new-code-for-proto-neutron-star-evolution/</link>
		<comments>http://voxcharta.org/2012/05/15/a-new-code-for-proto-neutron-star-evolution/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:49:56 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[approximation]]></category>
		<category><![CDATA[diffusion]]></category>
		<category><![CDATA[driven wind]]></category>
		<category><![CDATA[eddington]]></category>
		<category><![CDATA[electron]]></category>
		<category><![CDATA[emission]]></category>
		<category><![CDATA[equilibrium]]></category>
		<category><![CDATA[existence]]></category>
		<category><![CDATA[formal solution]]></category>
		<category><![CDATA[multi group]]></category>
		<category><![CDATA[neutrino]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[nucleosynthesis]]></category>
		<category><![CDATA[previous results]]></category>
		<category><![CDATA[proto]]></category>
		<category><![CDATA[relativistic boltzmann equation]]></category>
		<category><![CDATA[spectral evolution]]></category>
		<category><![CDATA[star evolution]]></category>
		<category><![CDATA[timescale]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/a-new-code-for-proto-neutron-star-evolution/</guid>
		<description><![CDATA[A new code for following the evolution and emissions of proto-neutron stars during the first minute of their lives is developed and tested. The code is one dimensional, fully implicit, and general relativistic. Multi-group, multi-flavor neutrino transport is incorporated that makes use of variable Eddington factors obtained from a formal solution of the static general [...]]]></description>
			<content:encoded><![CDATA[<p>A new code for following the evolution and emissions of proto-neutron stars during the first minute of their lives is developed and tested. The code is one dimensional, fully implicit, and general relativistic. Multi-group, multi-flavor neutrino transport is incorporated that makes use of variable Eddington factors obtained from a formal solution of the static general relativistic Boltzmann equation with linearized scattering terms. The timescales of neutrino emission and spectral evolution obtained using the new code are broadly consistent with previous results. Unlike other recent calculations, however, the new code predicts that the neutrino-driven wind will be characterized, at least for part of its existence, by a neutron excess. This change, potentially consequential for nucleosynthesis in the wind, is due to an improved treatment of the charged-current interactions of electron flavored neutrinos and anti-neutrinos with nucleons. A comparison is also made between the results obtained using either variable Eddington factors or simple equilibrium flux-limited diffusion. The latter approximation, which has been frequently used in previous studies of proto-neutron star cooling, accurately describes the total neutrino luminosities (to within 10%) for most of the evolution, until the proto-neutron star becomes optically thin.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
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		<title>The influence of fallback discs on the spectral and timing properties of neutron stars</title>
		<link>http://voxcharta.org/2012/05/15/the-influence-of-fallback-discs-on-the-spectral-and-timing-properties-of-neutron-stars/</link>
		<comments>http://voxcharta.org/2012/05/15/the-influence-of-fallback-discs-on-the-spectral-and-timing-properties-of-neutron-stars/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:47:44 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[consequence]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[Monte Carlo]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[population]]></category>
		<category><![CDATA[pulsars]]></category>
		<category><![CDATA[quantitative difference]]></category>
		<category><![CDATA[spectral property]]></category>
		<category><![CDATA[supernova explosion]]></category>
		<category><![CDATA[synthesis]]></category>
		<category><![CDATA[time period]]></category>
		<category><![CDATA[torque]]></category>
		<category><![CDATA[younger ones]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/the-influence-of-fallback-discs-on-the-spectral-and-timing-properties-of-neutron-stars/</guid>
		<description><![CDATA[Fallback discs around neutron stars (NSs) are believed to be an expected outcome of supernova explosions. Here we investigate the consequences of such a common outcome for the timing and spectral properties of the associated NS population, using Monte Carlo population synthesis models. We find that the long-term torque exerted by the fallback disc can [...]]]></description>
			<content:encoded><![CDATA[<p>Fallback discs around neutron stars (NSs) are believed to be an expected outcome of supernova explosions. Here we investigate the consequences of such a common outcome for the timing and spectral properties of the associated NS population, using Monte Carlo population synthesis models. We find that the long-term torque exerted by the fallback disc can substantially influence the late-time period distribution, but with quantitative differences which depend on whether the initial spin distribution is dominated by slow or fast pulsars. For the latter, a single-peaked initial spin distribution becomes bimodal at later times. Timing ages tend to underestimate the real age of older pulsars, and overestimate the age of younger ones. Braking indices cluster in the range 1.5 &lt;~ n &lt;~ 3 for slow-born pulsars, and -0.5 &lt;~ n &lt;~ 5 for fast-born pulsars, with the younger objects found predominantly below n &lt;~ 3. Large values of n, while not common, are possible, and associated with torque transitions in the NS+disc system. The 0.1-10 keV thermal luminosity of the NS+disc system is found to be generally dominated by the disc emission at early times, t &lt;~ 10^3 yr, but this declines faster than the thermal surface emission of the NS. Depending on the initial parameters, there can be occasional periods in which some NSs switch from the propeller to the accretion phase, increasing their luminosity up to the Eddington limit for ~ 10^3-10^4 years.</p>
]]></content:encoded>
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		<title>A Dirac right-handed sneutrino dark matter and its signature in the gamma-ray lines [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/15/a-dirac-right-handed-sneutrino-dark-matter-and-its-signature-in-the-gamma-ray-lines-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/15/a-dirac-right-handed-sneutrino-dark-matter-and-its-signature-in-the-gamma-ray-lines-cross-listing/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:47:14 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[annihilation]]></category>
		<category><![CDATA[coupling constants]]></category>
		<category><![CDATA[cross section]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[dirac]]></category>
		<category><![CDATA[fermion]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[higgs field]]></category>
		<category><![CDATA[lepton]]></category>
		<category><![CDATA[line signal]]></category>
		<category><![CDATA[massive particle]]></category>
		<category><![CDATA[neutrino]]></category>
		<category><![CDATA[relic density]]></category>
		<category><![CDATA[signature]]></category>
		<category><![CDATA[yukawa couplings]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/a-dirac-right-handed-sneutrino-dark-matter-and-its-signature-in-the-gamma-ray-lines-cross-listing/</guid>
		<description><![CDATA[We show that a Dirac right-handed scalar neutrino can be weakly interacting massive particle in the neutrinophilic Higgs model. When the additional Higgs fields couple only to the leptonic sector through neutrino Yukawa couplings, the right number of relic density of dark matter can be obtained from thermal freeze-out of the dark matter annihilation into [...]]]></description>
			<content:encoded><![CDATA[<p>We show that a Dirac right-handed scalar neutrino can be weakly interacting massive particle in the neutrinophilic Higgs model. When the additional Higgs fields couple only to the leptonic sector through neutrino Yukawa couplings, the right number of relic density of dark matter can be obtained from thermal freeze-out of the dark matter annihilation into charged leptons and neutrinos. At present, this annihilation is suppressed by the velocity of dark matter. However one-loop annihilation cross section into $\gamma\gamma$ can be larger than that of the helicity suppressed annihilation into fermions, because relevant coupling constants are different. Hence, gamma-ray line signal which might have been observed in the Fermi-LAT is also able to be explained by its annihilation.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/a-dirac-right-handed-sneutrino-dark-matter-and-its-signature-in-the-gamma-ray-lines-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A relativistic iron emission line from the neutron star low-mass X-ray binary GX 3+1</title>
		<link>http://voxcharta.org/2012/05/15/a-relativistic-iron-emission-line-from-the-neutron-star-low-mass-x-ray-binary-gx-31/</link>
		<comments>http://voxcharta.org/2012/05/15/a-relativistic-iron-emission-line-from-the-neutron-star-low-mass-x-ray-binary-gx-31/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:44:51 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion disk]]></category>
		<category><![CDATA[alpha emission]]></category>
		<category><![CDATA[burster]]></category>
		<category><![CDATA[component model]]></category>
		<category><![CDATA[disk inclination]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[energy features]]></category>
		<category><![CDATA[epic pn]]></category>
		<category><![CDATA[iron line]]></category>
		<category><![CDATA[keV]]></category>
		<category><![CDATA[line feature]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[mass x]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[pile up]]></category>
		<category><![CDATA[residuals]]></category>
		<category><![CDATA[spectroscopic study]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xmm newton]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/a-relativistic-iron-emission-line-from-the-neutron-star-low-mass-x-ray-binary-gx-31/</guid>
		<description><![CDATA[We present the results of a spectroscopic study of the Fe K{\alpha} emission of the persistent neutron-star atoll low-mass X-ray binary and type I X-ray burster GX 3+1 with the EPIC-PN on board XMM-Newton. The source shows a flux modulation over several years and we observed it during its fainter phase, which corresponds to an [...]]]></description>
			<content:encoded><![CDATA[<p>We present the results of a spectroscopic study of the Fe K{\alpha} emission of the persistent neutron-star atoll low-mass X-ray binary and type I X-ray burster GX 3+1 with the EPIC-PN on board XMM-Newton. The source shows a flux modulation over several years and we observed it during its fainter phase, which corresponds to an X-ray luminosity of Lx~10^37 ergs/s. When fitted with a two-component model, the X-ray spectrum shows broad residuals at \sim6-7 keV that can be ascribed to an iron K{\alpha} fluorescence line. In addition, lower energy features are observed at \sim3.3 keV, \sim3.9 keV and might originate from Ar XVIII and Ca XIX. The broad iron line feature is well fitted with a relativistically smeared profile. This result is robust against possible systematics caused by instrumental pile-up effects. Assuming that the line is produced by reflection from the inner accretion disk, we infer an inner disk radius of \sim25 Rg and a disk inclination of 35{\deg} &lt; i &lt; 44{\deg}.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/a-relativistic-iron-emission-line-from-the-neutron-star-low-mass-x-ray-binary-gx-31/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Electrodynamics of Massless Charges with Application to Pulsars</title>
		<link>http://voxcharta.org/2012/05/15/electrodynamics-of-massless-charges-with-application-to-pulsars/</link>
		<comments>http://voxcharta.org/2012/05/15/electrodynamics-of-massless-charges-with-application-to-pulsars/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:43:35 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[adequate theory]]></category>
		<category><![CDATA[dissipative dynamical system]]></category>
		<category><![CDATA[electrodynamics]]></category>
		<category><![CDATA[electromagnetic field]]></category>
		<category><![CDATA[emc]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[numerical calculation]]></category>
		<category><![CDATA[pulsar theory]]></category>
		<category><![CDATA[spectra]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/electrodynamics-of-massless-charges-with-application-to-pulsars/</guid>
		<description><![CDATA[Electromagnetic field together with zero-mass charges moving in this field form a well-behaved semi-dissipative dynamical system &#8212; Electrodynamics of Massless Charges (EMC). We give equations of EMC, argue that EMC is an adequate theory for calculating pulsar magnetospheres, give an illustrative numerical calculation (showing that bolometric luminosity of an aligned rotator is approximately equal to [...]]]></description>
			<content:encoded><![CDATA[<p>Electromagnetic field together with zero-mass charges moving in this field form a well-behaved semi-dissipative dynamical system &#8212; Electrodynamics of Massless Charges (EMC). We give equations of EMC, argue that EMC is an adequate theory for calculating pulsar magnetospheres, give an illustrative numerical calculation (showing that bolometric luminosity of an aligned rotator is approximately equal to half the spin-down power). EMC looks like a portion of the full pulsar theory that will resolve the already calculated bolometric luminosity into light curves and spectra.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/electrodynamics-of-massless-charges-with-application-to-pulsars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Tidal effects in binary neutron star coalescence [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/15/tidal-effects-in-binary-neutron-star-coalescence-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/15/tidal-effects-in-binary-neutron-star-coalescence-cross-listing/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:41:10 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accurate simulation]]></category>
		<category><![CDATA[accurate tool]]></category>
		<category><![CDATA[amplification]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[body model]]></category>
		<category><![CDATA[calibration]]></category>
		<category><![CDATA[coalescence]]></category>
		<category><![CDATA[consequence]]></category>
		<category><![CDATA[free parameter]]></category>
		<category><![CDATA[gravitational waveforms]]></category>
		<category><![CDATA[inaccuracy]]></category>
		<category><![CDATA[inclusion]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[numerical data]]></category>
		<category><![CDATA[numerical relativity simulations]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[tidal effect]]></category>
		<category><![CDATA[uncertainty]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/tidal-effects-in-binary-neutron-star-coalescence-cross-listing/</guid>
		<description><![CDATA[We compare dynamics and waveforms from binary neutron star coalescence as computed by new long-term ($\sim 10 $ orbits) numerical relativity simulations and by the tidal effective-one-body (EOB) model including analytical tidal corrections up to second post-Newtonian order (2PN). The current analytical knowledge encoded in the tidal EOB model is found to be sufficient to [...]]]></description>
			<content:encoded><![CDATA[<p>We compare dynamics and waveforms from binary neutron star coalescence as computed by new long-term ($\sim 10 $ orbits) numerical relativity simulations and by the tidal effective-one-body (EOB) model including analytical tidal corrections up to second post-Newtonian order (2PN). The current analytical knowledge encoded in the tidal EOB model is found to be sufficient to reproduce the numerical data up to contact and within their uncertainties. Remarkably, no calibration of any tidal EOB free parameters is required, beside those already fitted to binary black holes data. The inclusion of 2PN tidal corrections minimizes the differences with the numerical data, but it is not possible to significantly distinguish them from the leading-order tidal contribution. The presence of a relevant amplification of tidal effects is likely to be excluded, although it can appear as a consequence of numerical inaccuracies. We conclude that the tidally-completed effective-one-body model provides nowadays the most advanced and accurate tool for modelling gravitational waveforms from binary neutron star inspiral up to contact. This work also points out the importance of extensive tests to assess the uncertainties of the numerical data, and the potential need of new numerical strategies to perform accurate simulations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/tidal-effects-in-binary-neutron-star-coalescence-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Fermi~I particle acceleration in converging flows mediated by magnetic reconnection</title>
		<link>http://voxcharta.org/2012/05/15/fermii-particle-acceleration-in-converging-flows-mediated-by-magnetic-reconnection/</link>
		<comments>http://voxcharta.org/2012/05/15/fermii-particle-acceleration-in-converging-flows-mediated-by-magnetic-reconnection/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:38:27 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration mechanism]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[characteristic size]]></category>
		<category><![CDATA[electron]]></category>
		<category><![CDATA[energy distribution]]></category>
		<category><![CDATA[innermost region]]></category>
		<category><![CDATA[jets]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetic reconnection]]></category>
		<category><![CDATA[mean free path]]></category>
		<category><![CDATA[obstacle]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[particle acceleration]]></category>
		<category><![CDATA[particle energy]]></category>
		<category><![CDATA[polarity]]></category>
		<category><![CDATA[probability]]></category>
		<category><![CDATA[regime]]></category>
		<category><![CDATA[scenarios]]></category>
		<category><![CDATA[shock acceleration]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/fermii-particle-acceleration-in-converging-flows-mediated-by-magnetic-reconnection/</guid>
		<description><![CDATA[Converging flows with strong magnetic fields of different polarity can accelerate particles through magnetic reconnection. If the particle mean free path is larger than the thickness of the reconnection layer, but much smaller than the entire reconnection structure, the particle will mostly interact with the incoming flows potentially with a very low escape probability. We [...]]]></description>
			<content:encoded><![CDATA[<p>Converging flows with strong magnetic fields of different polarity can accelerate particles through magnetic reconnection. If the particle mean free path is larger than the thickness of the reconnection layer, but much smaller than the entire reconnection structure, the particle will mostly interact with the incoming flows potentially with a very low escape probability. We explore, in general and also in some specific scenarios, the possibility of particles being accelerated in a magnetic reconnection layer by interacting only with the incoming flows. We characterize converging flows undergoing magnetic reconnection, and derive analytical estimates for the particle energy distribution, acceleration rate, and maximum energies achievable in these flows. We also discuss a possible scenario, based on jets dominated by magnetic fields of changing polarity, in which this mechanism may operate. The proposed acceleration mechanism operates if the thickness of the reconnection layer is much smaller than its transversal characteristic size, and the magnetic field has a disordered component. Synchrotron losses may prevent electrons from entering in this acceleration regime. The acceleration rate should be faster, and the energy distribution of particles harder, than in standard diffusive shock acceleration. The interaction of obstacles with the innermost region of jets in active galactic nuclei and microquasars may be suitable sites for particle acceleration in converging flows.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/fermii-particle-acceleration-in-converging-flows-mediated-by-magnetic-reconnection/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Neutrinos And Cosmic Rays From Gamma Ray Bursts</title>
		<link>http://voxcharta.org/2012/05/15/neutrinos-and-cosmic-rays-from-gamma-ray-bursts/</link>
		<comments>http://voxcharta.org/2012/05/15/neutrinos-and-cosmic-rays-from-gamma-ray-bursts/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:37:37 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[collaboration]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[energy neutrino]]></category>
		<category><![CDATA[fireball]]></category>
		<category><![CDATA[gamma ray burst]]></category>
		<category><![CDATA[grbs]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[main source]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/neutrinos-and-cosmic-rays-from-gamma-ray-bursts/</guid>
		<description><![CDATA[The upper limit on the flux of ultra high energy neutrinos from gamma-ray bursts (GRBs) that was reported recently by the IceCube collaboration contradicts predictions based on the Fireball model of GRBs, but does not exclude GRBs as a main source of ultra-high energy cosmic rays.
]]></description>
			<content:encoded><![CDATA[<p>The upper limit on the flux of ultra high energy neutrinos from gamma-ray bursts (GRBs) that was reported recently by the IceCube collaboration contradicts predictions based on the Fireball model of GRBs, but does not exclude GRBs as a main source of ultra-high energy cosmic rays.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/neutrinos-and-cosmic-rays-from-gamma-ray-bursts/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Diffuse Galactic Gamma Rays at intermediate and high latitudes. I. Constraints on the ISM properties [Replacement]</title>
		<link>http://voxcharta.org/2012/05/15/diffuse-galactic-gamma-rays-at-intermediate-and-high-latitudes-i-constraints-on-the-ism-properties-replacement/</link>
		<comments>http://voxcharta.org/2012/05/15/diffuse-galactic-gamma-rays-at-intermediate-and-high-latitudes-i-constraints-on-the-ism-properties-replacement/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:36:07 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[conventional assumption]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[crs]]></category>
		<category><![CDATA[dark matter detection]]></category>
		<category><![CDATA[diffusion]]></category>
		<category><![CDATA[distributions]]></category>
		<category><![CDATA[dragon code]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[gamma ray emission]]></category>
		<category><![CDATA[gas distribution]]></category>
		<category><![CDATA[helium spectra]]></category>
		<category><![CDATA[high latitudes]]></category>
		<category><![CDATA[ism]]></category>
		<category><![CDATA[mev]]></category>
		<category><![CDATA[propagation]]></category>
		<category><![CDATA[proton]]></category>
		<category><![CDATA[unprecedented accuracy]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/diffuse-galactic-gamma-rays-at-intermediate-and-high-latitudes-i-constraints-on-the-ism-properties-replacement/</guid>
		<description><![CDATA[We study the high latitude (&#124;b&#124;&#62;10) diffuse gamma-ray emission in the Galaxy in light of the recently published data from the Fermi collaboration at energies between 100 MeV and 100 GeV. The unprecedented accuracy in these measurements allows to probe and constrain the properties of sources and propagation of cosmic rays (CRs) in the Galaxy, [...]]]></description>
			<content:encoded><![CDATA[<p>We study the high latitude (|b|&gt;10) diffuse gamma-ray emission in the Galaxy in light of the recently published data from the Fermi collaboration at energies between 100 MeV and 100 GeV. The unprecedented accuracy in these measurements allows to probe and constrain the properties of sources and propagation of cosmic rays (CRs) in the Galaxy, as well as confirming conventional assumptions made on the interstellar medium (ISM). Using the publicly available DRAGON code, that has been shown to reproduce local measurements of CRs, we study assumptions made in the literature on HI and H2 gas distributions in the ISM, and non spatially uniform models of diffusion in the Galaxy. By performing a combined analysis of CR and gamma-ray spectra, we derive constraints on the properties of the ISM gas distribution and the vertical scale height of galactic CR diffusion, which may have implications also on indirect Dark Matter detection. We also discuss some of the possible interpretations of the break at ~230 GV in CR protons and helium spectra, recently observed by PAMELA and their impact on gamma-rays.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/diffuse-galactic-gamma-rays-at-intermediate-and-high-latitudes-i-constraints-on-the-ism-properties-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Testing the Origin of High-Energy Cosmic Rays [Replacement]</title>
		<link>http://voxcharta.org/2012/05/15/testing-the-origin-of-high-energy-cosmic-rays-replacement/</link>
		<comments>http://voxcharta.org/2012/05/15/testing-the-origin-of-high-energy-cosmic-rays-replacement/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:35:42 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accurate measurement]]></category>
		<category><![CDATA[anisotropy]]></category>
		<category><![CDATA[clue]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[crs]]></category>
		<category><![CDATA[gamma ray emission]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[high energy astrophysics]]></category>
		<category><![CDATA[nuclei]]></category>
		<category><![CDATA[nucleon]]></category>
		<category><![CDATA[pamela]]></category>
		<category><![CDATA[proton]]></category>
		<category><![CDATA[ratios]]></category>
		<category><![CDATA[scenarios]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectral feature]]></category>
		<category><![CDATA[spectrum]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/testing-the-origin-of-high-energy-cosmic-rays-replacement/</guid>
		<description><![CDATA[Recent accurate measurements of cosmic-ray (CR) protons and nuclei by ATIC-2, CREAM, and PAMELA reveal: a) unexpected spectral hardening in the spectra of CR species above a few hundred GeV per nucleon, b) a harder spectrum of He compared to protons, and c) softening of the CR spectra just below the break energy. These newly-discovered [...]]]></description>
			<content:encoded><![CDATA[<p>Recent accurate measurements of cosmic-ray (CR) protons and nuclei by ATIC-2, CREAM, and PAMELA reveal: a) unexpected spectral hardening in the spectra of CR species above a few hundred GeV per nucleon, b) a harder spectrum of He compared to protons, and c) softening of the CR spectra just below the break energy. These newly-discovered features may offer a clue to the origin of the observed high-energy Galactic CRs. We discuss possible interpretations of these spectral features and make predictions for the secondary CR fluxes and secondary to primary ratios, anisotropy of CRs, and diffuse Galactic {\gamma}-ray emission in different phenomenological scenarios. Our predictions can be tested by currently running or near-future high-energy astrophysics experiments.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/testing-the-origin-of-high-energy-cosmic-rays-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Cosmic Rays during BBN as Origin of Lithium Problem [Replacement]</title>
		<link>http://voxcharta.org/2012/05/15/cosmic-rays-during-bbn-as-origin-of-lithium-problem-replacement-4/</link>
		<comments>http://voxcharta.org/2012/05/15/cosmic-rays-during-bbn-as-origin-of-lithium-problem-replacement-4/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:35:21 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abundance]]></category>
		<category><![CDATA[acceleration mechanism]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[bbn]]></category>
		<category><![CDATA[big bang nucleosynthesis]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[early universe]]></category>
		<category><![CDATA[further study]]></category>
		<category><![CDATA[Lithium]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[numerical calculation]]></category>
		<category><![CDATA[open question]]></category>
		<category><![CDATA[order of magnitude]]></category>
		<category><![CDATA[parameter space]]></category>
		<category><![CDATA[spectrum]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/cosmic-rays-during-bbn-as-origin-of-lithium-problem-replacement-4/</guid>
		<description><![CDATA[There may be non-thermal cosmic rays during big-bang nucleosynthesis (BBN) epoch (dubbed as BBNCRs). This paper investigated whether such BBNCRs can be the origin of Lithium problem or not. It can be expected that BBNCRs flux will be small in order to keep the success of standard BBN (SBBN). With favorable assumptions on the BBNCR [...]]]></description>
			<content:encoded><![CDATA[<p>There may be non-thermal cosmic rays during big-bang nucleosynthesis (BBN) epoch (dubbed as BBNCRs). This paper investigated whether such BBNCRs can be the origin of Lithium problem or not. It can be expected that BBNCRs flux will be small in order to keep the success of standard BBN (SBBN). With favorable assumptions on the BBNCR spectrum between 0.09 &#8212; 4 MeV, our numerical calculation showed that extra contributions from BBNCRs can account for the $^7$Li abundance successfully. However $^6$Li abundance is only lifted an order of magnitude, which is still much lower than the observed value. As the deuteron abundance is very sensitive to the spectrum choice of BBNCRs, the allowed parameter space for the spectrum is strictly constrained. We should emphasize that the acceleration mechanism for BBNCRs in the early universe is still an open question. For example, strong turbulent magnetic field is probably the solution to the problem. Whether such a mechanism can provide the required spectrum deserves further studies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/cosmic-rays-during-bbn-as-origin-of-lithium-problem-replacement-4/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<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>Cosmic-ray-induced ionization in molecular clouds adjacent to supernova remnants &#8211; Tracing the hadronic origin of GeV gamma radiation [Replacement]</title>
		<link>http://voxcharta.org/2012/05/15/cosmic-ray-induced-ionization-in-molecular-clouds-adjacent-to-supernova-remnants-tracing-the-hadronic-origin-of-gev-gamma-radiation-replacement/</link>
		<comments>http://voxcharta.org/2012/05/15/cosmic-ray-induced-ionization-in-molecular-clouds-adjacent-to-supernova-remnants-tracing-the-hadronic-origin-of-gev-gamma-radiation-replacement/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:34:31 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration]]></category>
		<category><![CDATA[bremsstrahlung]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[gamma radiation]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[molecular cloud]]></category>
		<category><![CDATA[nuclei]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[photon energy]]></category>
		<category><![CDATA[shock]]></category>
		<category><![CDATA[supernova remnant]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/cosmic-ray-induced-ionization-in-molecular-clouds-adjacent-to-supernova-remnants-tracing-the-hadronic-origin-of-gev-gamma-radiation-replacement/</guid>
		<description><![CDATA[Energetic gamma rays (GeV to TeV photon energy) have been detected toward several supernova remnants (SNR) associated with molecular clouds. If the gamma rays are produced mainly by hadronic processes rather than leptonic processes like bremsstrahlung, then the flux of energetic cosmic ray (CR) nuclei (&#62;1 GeV) required to produce the gamma rays can be [...]]]></description>
			<content:encoded><![CDATA[<p>Energetic gamma rays (GeV to TeV photon energy) have been detected toward several supernova remnants (SNR) associated with molecular clouds. If the gamma rays are produced mainly by hadronic processes rather than leptonic processes like bremsstrahlung, then the flux of energetic cosmic ray (CR) nuclei (&gt;1 GeV) required to produce the gamma rays can be inferred at the site where the particles are accelerated in SNR shocks. It is of great interest to understand the acceleration of the CR of lower energy (&lt;1 GeV) accompanying the energetic component. These particles of lower energy are most effective in ionizing interstellar gas, leaving an observable imprint on the interstellar ion chemistry. A correlation of energetic gamma radiation with enhanced interstellar ionization can thus support the hadronic origin of the gamma rays and constrain the acceleration of ionizing CR in SNR. We propose a method to test the hadronic origin of GeV gamma rays from SNR associated with a molecular cloud. We use observational gamma ray data for each of these SNR known, modeling the observations to obtain the underlying proton spectrum assuming that the gamma rays are produced by pion decay. Assuming that the acceleration mechanism does not only produce high energy protons, but also low energy protons, this proton spectrum at the source is then used to calculate the ionization rate of the molecular cloud. Ionized molecular hydrogen triggers a chemical network forming molecular ions. The relaxation of these ions results in characteristic line emission, which can be predicted. We show that the ionization rate for at least two objects is more than an order of magnitude above Galactic average for molecular clouds, hinting at an enhanced formation rate of molecular ions. There will be interesting opportunities to measure crucial molecular ions in the infrared and submillimeter-wave parts of the spectrum.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/cosmic-ray-induced-ionization-in-molecular-clouds-adjacent-to-supernova-remnants-tracing-the-hadronic-origin-of-gev-gamma-radiation-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The XMM-Newton Slew view of IGRJ17361-4441: a transient in the globular cluster NGC 6388 [Replacement]</title>
		<link>http://voxcharta.org/2012/05/15/the-xmm-newton-slew-view-of-igrj17361-4441-a-transient-in-the-globular-cluster-ngc-6388-replacement/</link>
		<comments>http://voxcharta.org/2012/05/15/the-xmm-newton-slew-view-of-igrj17361-4441-a-transient-in-the-globular-cluster-ngc-6388-replacement/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:33:37 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[center of gravity]]></category>
		<category><![CDATA[Chandra]]></category>
		<category><![CDATA[cluster ngc]]></category>
		<category><![CDATA[globular cluster]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[integral satellite]]></category>
		<category><![CDATA[observation]]></category>
		<category><![CDATA[observatory]]></category>
		<category><![CDATA[rxte]]></category>
		<category><![CDATA[slew]]></category>
		<category><![CDATA[spectral parameters]]></category>
		<category><![CDATA[spectral variations]]></category>
		<category><![CDATA[spectrum]]></category>
		<category><![CDATA[swift]]></category>
		<category><![CDATA[target]]></category>
		<category><![CDATA[xmm newton]]></category>
		<category><![CDATA[xrt]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/the-xmm-newton-slew-view-of-igrj17361-4441-a-transient-in-the-globular-cluster-ngc-6388-replacement/</guid>
		<description><![CDATA[IGRJ17361-4441 is a hard transient recently observed by the INTEGRAL satellite. The source, close to the center of gravity of the globular cluster NGC 6388, quickly became the target of follow-up observations conducted by the Chandra, Swift/XRT and RXTE observatories. Here, we concentrate in particular on a set of observations conducted by the XMM-Newton satellite [...]]]></description>
			<content:encoded><![CDATA[<p>IGRJ17361-4441 is a hard transient recently observed by the INTEGRAL satellite. The source, close to the center of gravity of the globular cluster NGC 6388, quickly became the target of follow-up observations conducted by the Chandra, Swift/XRT and RXTE observatories. Here, we concentrate in particular on a set of observations conducted by the XMM-Newton satellite during two slews, in order to get the spectral information of the source and search for spectral variations. The spectral parameters determined by the recent XMM-Newton slew observations were compared to the previously known results. The maximum unabsorbed $X$-ray flux in the 0.5-10 keV band as detected by the XMM-Newton slew observations is $\simeq 4.5\times 10^{-11}$ erg cm$^{-2}$ s$^{-1}$, i.e. consistent with that observed by the Swift/XRT satellite 15 days earlier. The spectrum seems to be marginally consistent ($\Gamma\simeq 0.93-1.63$) with that derived from the previous high energy observation.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/the-xmm-newton-slew-view-of-igrj17361-4441-a-transient-in-the-globular-cluster-ngc-6388-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>
		</item>
		<item>
		<title>AGN Physics with the Cherenkov Telescope Array [Replacement]</title>
		<link>http://voxcharta.org/2012/05/15/agn-physics-with-the-cherenkov-telescope-array-replacement/</link>
		<comments>http://voxcharta.org/2012/05/15/agn-physics-with-the-cherenkov-telescope-array-replacement/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:32:35 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[cherenkov telescopes]]></category>
		<category><![CDATA[cta]]></category>
		<category><![CDATA[energy coverage]]></category>
		<category><![CDATA[energy gamma rays]]></category>
		<category><![CDATA[energy range]]></category>
		<category><![CDATA[extragalactic background light]]></category>
		<category><![CDATA[extragalactic sources]]></category>
		<category><![CDATA[extrapolation]]></category>
		<category><![CDATA[Fermi]]></category>
		<category><![CDATA[gap]]></category>
		<category><![CDATA[international consortium]]></category>
		<category><![CDATA[lorentz invariance]]></category>
		<category><![CDATA[preparatory phase]]></category>
		<category><![CDATA[radio galaxy]]></category>
		<category><![CDATA[science case]]></category>
		<category><![CDATA[southern hemisphere]]></category>
		<category><![CDATA[spectral feature]]></category>
		<category><![CDATA[telescope array]]></category>
		<category><![CDATA[tev sources]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/agn-physics-with-the-cherenkov-telescope-array-replacement/</guid>
		<description><![CDATA[The Cherenkov Telescope Array (CTA), currently in its Preparatory Phase, will be the first open observatory for very high energy gamma-rays from galactic and extragalactic sources. The international consortium behind CTA is preparing the construction of two large arrays of Cherenkov telescopes in the Northern and Southern Hemispheres with a performance that will be significantly [...]]]></description>
			<content:encoded><![CDATA[<p>The Cherenkov Telescope Array (CTA), currently in its Preparatory Phase, will be the first open observatory for very high energy gamma-rays from galactic and extragalactic sources. The international consortium behind CTA is preparing the construction of two large arrays of Cherenkov telescopes in the Northern and Southern Hemispheres with a performance that will be significantly improved compared to the current generation of arrays.   Its increased sensitivity and energy range will give CTA access to a large population of Active Galactic Nuclei (AGN) not yet detected at very high energies and provide much more details on known TeV sources. While the low end of the CTA energy coverage will close the current gap with the Fermi-LAT band, its high energy coverage will open a new window on the sky and help us understand the intrinsic shape of the hardest blazar spectra.   We outline the current status of CTA and discuss the science case for AGN physics with the observatory. Predictions for source detections based on extrapolations of Fermi-LAT spectra are discussed. An overview is given of prospects for the detection of extended emission from radio galaxies, of rapid variability, and spectral features. The observation of AGN with CTA will also improve current constraints on the distribution of the extragalactic background light, the strength of the intergalactic magnetic field and Lorentz invariance violation.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/agn-physics-with-the-cherenkov-telescope-array-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>130 GeV dark matter and the Fermi gamma-ray line [Replacement]</title>
		<link>http://voxcharta.org/2012/05/15/130-gev-dark-matter-and-the-fermi-gamma-ray-line-replacement/</link>
		<comments>http://voxcharta.org/2012/05/15/130-gev-dark-matter-and-the-fermi-gamma-ray-line-replacement/#comments</comments>
		<pubDate>Wed, 16 May 2012 00:32:25 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[center of the galaxy]]></category>
		<category><![CDATA[coupling]]></category>
		<category><![CDATA[cross section]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[gamma gamma]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[hadronic jets]]></category>
		<category><![CDATA[higgs boson]]></category>
		<category><![CDATA[Lambda]]></category>
		<category><![CDATA[nucleon]]></category>
		<category><![CDATA[particle physics]]></category>
		<category><![CDATA[photon]]></category>
		<category><![CDATA[physics model]]></category>
		<category><![CDATA[pion]]></category>
		<category><![CDATA[qcd]]></category>
		<category><![CDATA[relic density]]></category>
		<category><![CDATA[section 24]]></category>
		<category><![CDATA[standard model]]></category>
		<category><![CDATA[tentative evidence]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/15/130-gev-dark-matter-and-the-fermi-gamma-ray-line-replacement/</guid>
		<description><![CDATA[Based on tentative evidence for a peak in the Fermi gamma-ray spectrum originating from near the center of the galaxy, it has been suggested that dark matter of mass ~130 GeV is annihilating directly into photons with a cross section ~24 times smaller than that needed for the thermal relic density. We propose a simple [...]]]></description>
			<content:encoded><![CDATA[<p>Based on tentative evidence for a peak in the Fermi gamma-ray spectrum originating from near the center of the galaxy, it has been suggested that dark matter of mass ~130 GeV is annihilating directly into photons with a cross section ~24 times smaller than that needed for the thermal relic density. We propose a simple particle physics model in which the DM is a scalar X, with a coupling lambda_X X^2|S|^2 to a scalar multiplet S carrying electric charge, which allows for XX -&gt; gamma gamma at one loop due to the virtual S. We predict a second monochromatic photon peak at 114 GeV due to XX -&gt; gamma Z. The S should be colored under a hidden sector SU(N) or QCD to confine the charged relic S. The analogous coupling lambda_h h^2 |S|^2 to the Higgs boson can naturally increase the partial width for h -&gt; gamma gamma by an amount comparable to its standard model value, as suggested by recent measurements from CMS. Due to the hidden sector SU(N) (or QCD), S binds to its antiparticle to form S-pions, which will be pair-produced in colliders and then decay predominantly to XX, hh (or hadronic jets) and subdominantly to gamma gamma. The cross section for X on nucleons is in marginal conflict with the Xenon100 upper limit, suggesting that it should be discovered soon by direct detection.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/15/130-gev-dark-matter-and-the-fermi-gamma-ray-line-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Fermi LAT Search for Dark Matter in Gamma-ray Lines and the Inclusive Photon Spectrum</title>
		<link>http://voxcharta.org/2012/05/14/fermi-lat-search-for-dark-matter-in-gamma-ray-lines-and-the-inclusive-photon-spectrum/</link>
		<comments>http://voxcharta.org/2012/05/14/fermi-lat-search-for-dark-matter-in-gamma-ray-lines-and-the-inclusive-photon-spectrum/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:49:45 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[annihilation]]></category>
		<category><![CDATA[background flux]]></category>
		<category><![CDATA[cosmic ray data]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[decay]]></category>
		<category><![CDATA[explanations]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[lifetime]]></category>
		<category><![CDATA[matter particle]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[pamela]]></category>
		<category><![CDATA[photon spectrum]]></category>
		<category><![CDATA[sky]]></category>
		<category><![CDATA[spectral line]]></category>
		<category><![CDATA[telescope data]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/fermi-lat-search-for-dark-matter-in-gamma-ray-lines-and-the-inclusive-photon-spectrum/</guid>
		<description><![CDATA[Dark matter particle annihilation or decay can produce monochromatic gamma-ray lines and contribute to the diffuse gamma-ray background. Flux upper limits are presented for gamma-ray spectral lines from 7 to 200 GeV and for the diffuse gamma-ray background from 4.8 GeV to 264 GeV obtained from two years of Fermi Large Area Telescope data integrated [...]]]></description>
			<content:encoded><![CDATA[<p>Dark matter particle annihilation or decay can produce monochromatic gamma-ray lines and contribute to the diffuse gamma-ray background. Flux upper limits are presented for gamma-ray spectral lines from 7 to 200 GeV and for the diffuse gamma-ray background from 4.8 GeV to 264 GeV obtained from two years of Fermi Large Area Telescope data integrated over most of the sky. We give cross section upper limits and decay lifetime lower limits for dark matter models that produce gamma-ray lines or contribute to the diffuse spectrum, including models proposed as explanations of the PAMELA and Fermi cosmic-ray data.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/fermi-lat-search-for-dark-matter-in-gamma-ray-lines-and-the-inclusive-photon-spectrum/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A New Sample of Candidate Intermediate-Mass Black Holes Selected by X-ray Variability</title>
		<link>http://voxcharta.org/2012/05/14/a-new-sample-of-candidate-intermediate-mass-black-holes-selected-by-x-ray-variability/</link>
		<comments>http://voxcharta.org/2012/05/14/a-new-sample-of-candidate-intermediate-mass-black-holes-selected-by-x-ray-variability/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:47:59 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[eddington]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[positive correlation]]></category>
		<category><![CDATA[ratios]]></category>
		<category><![CDATA[serendipitous]]></category>
		<category><![CDATA[soft x]]></category>
		<category><![CDATA[source catalogue]]></category>
		<category><![CDATA[spectral analysis]]></category>
		<category><![CDATA[variability]]></category>
		<category><![CDATA[variance]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xmm newton]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/a-new-sample-of-candidate-intermediate-mass-black-holes-selected-by-x-ray-variability/</guid>
		<description><![CDATA[We present the results of X-ray variability and spectral analysis of a sample of 15 new candidates for active galactic nuclei with relatively low-mass black holes (BHs). They are selected from the Second XMM-Newton Serendipitous Source Catalogue based on strong variability quantified by normalized excess variances. Their BH masses are estimated to be 1.1-6.6&#215;10^6 M_solar [...]]]></description>
			<content:encoded><![CDATA[<p>We present the results of X-ray variability and spectral analysis of a sample of 15 new candidates for active galactic nuclei with relatively low-mass black holes (BHs). They are selected from the Second XMM-Newton Serendipitous Source Catalogue based on strong variability quantified by normalized excess variances. Their BH masses are estimated to be 1.1-6.6&#215;10^6 M_solar by using a correlation between excess variance and BH mass. Seven sources have estimated BH masses smaller than 2&#215;10^6 M_solar, which are in the range for intermediate-mass black holes. Eddington ratios of sources with known redshifts range from 0.07 to 0.46 and the mean Eddington ratio is 0.24. These results imply that some of our sources are growing supermassive black holes, which are expected to have relatively low masses with high Eddington ratios. X-ray photon indices of the 15 sources are in the range of ~0.57-2.57, and 5 among them have steep (&gt;2) photon indices, which are the range for narrow-line Seyfert 1s. Soft X-ray excess is seen in 12 sources, and is expressed by a blackbody model with kT~83-294 eV. We derive a correlation between X-ray photon indices and Eddington ratios, and find that the X-ray photon indices of about a half of our sources are flatter than the positive correlation suggested previously.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/a-new-sample-of-candidate-intermediate-mass-black-holes-selected-by-x-ray-variability/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A Candidate Active Galactic Nucleus with a Pure Soft Thermal X-ray Spectrum</title>
		<link>http://voxcharta.org/2012/05/14/a-candidate-active-galactic-nucleus-with-a-pure-soft-thermal-x-ray-spectrum/</link>
		<comments>http://voxcharta.org/2012/05/14/a-candidate-active-galactic-nucleus-with-a-pure-soft-thermal-x-ray-spectrum/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:47:48 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[binaries]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[eddington]]></category>
		<category><![CDATA[galactic nucleus]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[keV]]></category>
		<category><![CDATA[low energy]]></category>
		<category><![CDATA[signal to noise]]></category>
		<category><![CDATA[signal to noise ratio]]></category>
		<category><![CDATA[soft x]]></category>
		<category><![CDATA[source catalogue]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectral regime]]></category>
		<category><![CDATA[spectral variability]]></category>
		<category><![CDATA[thermal emission]]></category>
		<category><![CDATA[time interval]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xmm]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/a-candidate-active-galactic-nucleus-with-a-pure-soft-thermal-x-ray-spectrum/</guid>
		<description><![CDATA[We report the discovery of a candidate active galactic nucleus (AGN), 2XMM J123103.2+110648 at z = 0.13, with an X-ray spectrum represented purely by soft thermal emission reminiscent of Galactic black hole (BH) binaries in the disk-dominated state. This object was found in the second XMM serendipitous source catalogue as a highly variable X-ray source. [...]]]></description>
			<content:encoded><![CDATA[<p>We report the discovery of a candidate active galactic nucleus (AGN), 2XMM J123103.2+110648 at z = 0.13, with an X-ray spectrum represented purely by soft thermal emission reminiscent of Galactic black hole (BH) binaries in the disk-dominated state. This object was found in the second XMM serendipitous source catalogue as a highly variable X-ray source. In three separate observations, its X-ray spectrum can be represented either by a multicolor disk blackbody model with an inner temperature of kT_in~0.16-0.21 keV or a Wien spectrum Comptonized by an optically thick plasma with kT~0.14-0.18 keV. The soft X-ray luminosity in the 0.5&#8211;2 keV band is estimated to be (1.6-3.8)x10^42 erg/s. Hard emission above ~2 keV is not detected. The ratio of the soft to hard emission is the strongest among AGNs observed thus far. Spectra selected in high/low flux time intervals are examined in order to study spectral variability. In the second observation with the highest signal-to-noise ratio, the low energy (below 0.7 keV) spectral regime flattens when the flux is high, while the shape of the high energy part (1-1.7 keV) remains unchanged. This behavior is qualitatively consistent with being caused by strong Comptonization. Both the strong soft excess and spectral change consistent with Comptonization in the X-ray spectrum imply that the Eddington ratio is large, which requires a small BH mass (smaller than ~10^5M_solar.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/a-candidate-active-galactic-nucleus-with-a-pure-soft-thermal-x-ray-spectrum/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Charged-current weak interaction processes in hot and dense matter and its impact on the spectra of neutrinos emitted from proto-neutron star cooling</title>
		<link>http://voxcharta.org/2012/05/14/charged-current-weak-interaction-processes-in-hot-and-dense-matter-and-its-impact-on-the-spectra-of-neutrinos-emitted-from-proto-neutron-star-cooling/</link>
		<comments>http://voxcharta.org/2012/05/14/charged-current-weak-interaction-processes-in-hot-and-dense-matter-and-its-impact-on-the-spectra-of-neutrinos-emitted-from-proto-neutron-star-cooling/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:47:11 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[antineutrino]]></category>
		<category><![CDATA[boltzmann]]></category>
		<category><![CDATA[core collapse supernova]]></category>
		<category><![CDATA[dense matter]]></category>
		<category><![CDATA[driven wind]]></category>
		<category><![CDATA[electron neutrino]]></category>
		<category><![CDATA[equation of state]]></category>
		<category><![CDATA[flavors]]></category>
		<category><![CDATA[interaction processes]]></category>
		<category><![CDATA[neutrino interaction]]></category>
		<category><![CDATA[neutrino transport]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[nucleosynthesis]]></category>
		<category><![CDATA[radiation hydrodynamics]]></category>
		<category><![CDATA[spectral changes]]></category>
		<category><![CDATA[spectral differences]]></category>
		<category><![CDATA[substantial impact]]></category>
		<category><![CDATA[weak interaction]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/charged-current-weak-interaction-processes-in-hot-and-dense-matter-and-its-impact-on-the-spectra-of-neutrinos-emitted-from-proto-neutron-star-cooling/</guid>
		<description><![CDATA[We have performed three-flavor Boltzmann neutrino transport radiation hydrodynamics simulations covering a period of 3 s after the formation of a protoneutron star in a core-collapse supernova explosion. Our results show that a treatment of charged-current neutrino interactions in hot and dense matter as suggested by Reddy et al. [Phys. Rev. D 58, 013009 (1998)] [...]]]></description>
			<content:encoded><![CDATA[<p>We have performed three-flavor Boltzmann neutrino transport radiation hydrodynamics simulations covering a period of 3 s after the formation of a protoneutron star in a core-collapse supernova explosion. Our results show that a treatment of charged-current neutrino interactions in hot and dense matter as suggested by Reddy et al. [Phys. Rev. D 58, 013009 (1998)] has a strong impact on the luminosities and spectra of the emitted neutrinos. When compared with simulations that neglect mean field effects on the neutrino opacities, we find that the luminosities of all neutrino flavors are reduced while the spectral differences between electron neutrino and antineutrino are increased. Their magnitude depends on the equation of state and in particular on the symmetry energy at sub-nuclear densities. These modifications reduce the proton-to-nucleon ratio of the outflow, increasing slightly their entropy. They are expected to have a substantial impact on the nucleosynthesis in neutrino-driven winds, even though they do not result in conditions that favor an r-process. Contrarily to previous findings, our simulations show that the spectra of electron neutrinos remain substantially different from those of other (anti)neutrino flavors during the entire deleptonization phase of the protoneutron star. The obtained luminosity and spectral changes are also expected to have important consequences for neutrino flavor oscillations and neutrino detection on Earth.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/charged-current-weak-interaction-processes-in-hot-and-dense-matter-and-its-impact-on-the-spectra-of-neutrinos-emitted-from-proto-neutron-star-cooling/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>New insights into the Be/X-ray binary system MXB 0656-072</title>
		<link>http://voxcharta.org/2012/05/14/new-insights-into-the-bex-ray-binary-system-mxb-0656-072/</link>
		<comments>http://voxcharta.org/2012/05/14/new-insights-into-the-bex-ray-binary-system-mxb-0656-072/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:45:43 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[archive data]]></category>
		<category><![CDATA[binary system]]></category>
		<category><![CDATA[giant type]]></category>
		<category><![CDATA[high mass]]></category>
		<category><![CDATA[hydrodynamic instability]]></category>
		<category><![CDATA[mass x]]></category>
		<category><![CDATA[new insights]]></category>
		<category><![CDATA[optical counterpart]]></category>
		<category><![CDATA[optical spectra]]></category>
		<category><![CDATA[optical spectroscopy]]></category>
		<category><![CDATA[orbital period]]></category>
		<category><![CDATA[peculiar feature]]></category>
		<category><![CDATA[periodicity]]></category>
		<category><![CDATA[physical regions]]></category>
		<category><![CDATA[pulsation]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[spectral parameters]]></category>
		<category><![CDATA[times10]]></category>
		<category><![CDATA[transient nature]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/new-insights-into-the-bex-ray-binary-system-mxb-0656-072/</guid>
		<description><![CDATA[The X-ray transient MXB 0656-072 is a poorly studied member of high-mass X-ray binaries. Based on the transient nature of the X-ray emission, the detection of pulsations, and the early-type companion, it has been classified as a Be X-ray binary (Be/XRB). However, the flaring activity covering a large fraction of a giant outburst is somehow [...]]]></description>
			<content:encoded><![CDATA[<p>The X-ray transient MXB 0656-072 is a poorly studied member of high-mass X-ray binaries. Based on the transient nature of the X-ray emission, the detection of pulsations, and the early-type companion, it has been classified as a Be X-ray binary (Be/XRB). However, the flaring activity covering a large fraction of a giant outburst is somehow peculiar. Our goal is to investigate the multiwavelength variability of the high-mass X-ray binary MXB 0656-072. We carry out optical spectroscopy and analyse all RXTE archive data, performing a detailed X-ray colour, spectral, and timing analysis of both normal (type-I) and giant (type-II) outbursts from MXB 0656-072. From optical spectroscopy, we classify the optical counterpart as a O9.5Ve star, confirming its Be nature. From the study of type-I outbursts we unveil a \sim100 days periodicity, most likely associated with the orbital period of the system. Balmer lines in emission in the optical spectra, long-term X-ray variability, and the spin period / orbital period relation, are fully consistent with the system being a Be/XRB. The peculiar feature that characterises the type-II outburst is flaring activity, which occurs during the whole outburst peak, before a smoother decay. We interpret it in terms of magneto-hydrodynamic instability. We explored for the first time the aperiodic X-ray variability of the system, finding a correlation of the central frequency and rms of the main timing component with luminosity, which extends up to a &#8220;saturation&#8221; flux of 1\times10^-8 erg cm^2 s^-1 . A correlation between timing and spectral parameters was also found, pointing to an interconnection between the two physical regions responsible for both phenomenologies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/new-insights-into-the-bex-ray-binary-system-mxb-0656-072/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Signs of magnetic accretion in X-ray pulsars</title>
		<link>http://voxcharta.org/2012/05/14/signs-of-magnetic-accretion-in-x-ray-pulsars/</link>
		<comments>http://voxcharta.org/2012/05/14/signs-of-magnetic-accretion-in-x-ray-pulsars/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:45:33 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[binary system]]></category>
		<category><![CDATA[mass transfer]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[pulsars]]></category>
		<category><![CDATA[radius]]></category>
		<category><![CDATA[signs]]></category>
		<category><![CDATA[torque]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/signs-of-magnetic-accretion-in-x-ray-pulsars/</guid>
		<description><![CDATA[The spin-down mechanism of accreting neutron stars is discussed with an application to one of the best studied X-ray pulsars GX 301-2. We show that the maximum possible spin-down torque applied to a neutron star from the accretion flow can be evaluated as $K_{\rm sd}^{\rm (t)} = \mu^2/(r_{\rm m} r_{\rm cor})^{3/2}$. The spin-down rate of [...]]]></description>
			<content:encoded><![CDATA[<p>The spin-down mechanism of accreting neutron stars is discussed with an application to one of the best studied X-ray pulsars GX 301-2. We show that the maximum possible spin-down torque applied to a neutron star from the accretion flow can be evaluated as $K_{\rm sd}^{\rm (t)} = \mu^2/(r_{\rm m} r_{\rm cor})^{3/2}$. The spin-down rate of the neutron star in GX 301-2 can be explained provided the magnetospheric radius of the neutron star is smaller than its canonical value. We calculate the magnetospheric radius considering the mass-transfer in the binary system in the frame of the magnetic accretion scenario suggested by V.F. Shvartsman. The spin-down rate of the neutron star expected within this approach is in a good agreement with that derived from observations of GX 301-2.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/signs-of-magnetic-accretion-in-x-ray-pulsars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>On the spectral shape of radiation due to Inverse Compton Scattering close to the maximum cut-off</title>
		<link>http://voxcharta.org/2012/05/14/on-the-spectral-shape-of-radiation-due-to-inverse-compton-scattering-close-to-the-maximum-cut-off/</link>
		<comments>http://voxcharta.org/2012/05/14/on-the-spectral-shape-of-radiation-due-to-inverse-compton-scattering-close-to-the-maximum-cut-off/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:44:44 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[approximation]]></category>
		<category><![CDATA[electron distribution]]></category>
		<category><![CDATA[expression]]></category>
		<category><![CDATA[inverse compton]]></category>
		<category><![CDATA[klein nishina]]></category>
		<category><![CDATA[parent electrons]]></category>
		<category><![CDATA[photon]]></category>
		<category><![CDATA[radiation]]></category>
		<category><![CDATA[regime]]></category>
		<category><![CDATA[spectral shape]]></category>
		<category><![CDATA[spectrum]]></category>
		<category><![CDATA[target]]></category>
		<category><![CDATA[thomson]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/on-the-spectral-shape-of-radiation-due-to-inverse-compton-scattering-close-to-the-maximum-cut-off/</guid>
		<description><![CDATA[The spectral shape of radiation due to Inverse Compton Scattering is analyzed, in the Thomson and the Klein-Nishina regime, for electron distributions with exponential cut-off. We derive analytical, asymptotic expressions for the spectrum close to the maximum cut-off region. We consider monoenergetic, Planckian and Synchrotron photons as target photon fields. These approximations provide a direct [...]]]></description>
			<content:encoded><![CDATA[<p>The spectral shape of radiation due to Inverse Compton Scattering is analyzed, in the Thomson and the Klein-Nishina regime, for electron distributions with exponential cut-off. We derive analytical, asymptotic expressions for the spectrum close to the maximum cut-off region. We consider monoenergetic, Planckian and Synchrotron photons as target photon fields. These approximations provide a direct link between the distribution of parent electrons and the up-scattered spectrum at the cut-off region.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/on-the-spectral-shape-of-radiation-due-to-inverse-compton-scattering-close-to-the-maximum-cut-off/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A fully covariant mean-field dynamo closure for numerical 3+1 resistive GRMHD</title>
		<link>http://voxcharta.org/2012/05/14/a-fully-covariant-mean-field-dynamo-closure-for-numerical-31-resistive-grmhd/</link>
		<comments>http://voxcharta.org/2012/05/14/a-fully-covariant-mean-field-dynamo-closure-for-numerical-31-resistive-grmhd/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:44:20 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion disk]]></category>
		<category><![CDATA[analytical solution]]></category>
		<category><![CDATA[astrophysics]]></category>
		<category><![CDATA[classical theory]]></category>
		<category><![CDATA[dynamo action]]></category>
		<category><![CDATA[dynamo processes]]></category>
		<category><![CDATA[energy phenomena]]></category>
		<category><![CDATA[finite difference scheme]]></category>
		<category><![CDATA[global dynamics]]></category>
		<category><![CDATA[gravitational field]]></category>
		<category><![CDATA[hole accretion]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetization]]></category>
		<category><![CDATA[mhd]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[numerical scheme]]></category>
		<category><![CDATA[numerical test]]></category>
		<category><![CDATA[physical processes]]></category>
		<category><![CDATA[resistivity]]></category>
		<category><![CDATA[zanna]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/a-fully-covariant-mean-field-dynamo-closure-for-numerical-31-resistive-grmhd/</guid>
		<description><![CDATA[The powerful high-energy phenomena typically encountered in astrophysics invariably involve physical engines, like neutron stars and black hole accretion disks, characterized by a combination of highly magnetized plasmas, strong gravitational fields, and relativistic motions. In recent years numerical schemes for General Relativistic MHD (GRMHD) have been developed to model the multidimensional dynamics of such systems, [...]]]></description>
			<content:encoded><![CDATA[<p>The powerful high-energy phenomena typically encountered in astrophysics invariably involve physical engines, like neutron stars and black hole accretion disks, characterized by a combination of highly magnetized plasmas, strong gravitational fields, and relativistic motions. In recent years numerical schemes for General Relativistic MHD (GRMHD) have been developed to model the multidimensional dynamics of such systems, including the possibility of an evolving spacetime. Such schemes have been also extended beyond the ideal limit including the effects of resistivity, in an attempt to model dissipative physical processes acting on small scales (sub-grid effects) over the global dynamics. Along the same lines, magnetic fields could be amplified by the presence of turbulent dynamo processes, as often invoked to explain the high values of magnetization required in accretion disks and neutron stars. Here we present, for the first time, a further extension to include the possibility of a mean-field dynamo action within the framework of numerical 3+1 (resistive) GRMHD. A fully covariant dynamo closure is proposed, in analogy with the classical theory, assuming a simple alpha-effect in the comoving frame. Its implementation into a finite-difference scheme for GRMHD in dynamical spacetimes [the X-ECHO code: (Bucciantini and Del Zanna 2011)] is described, and a set of numerical test is presented and compared with analytical solutions wherever possible.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/a-fully-covariant-mean-field-dynamo-closure-for-numerical-31-resistive-grmhd/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A First Search for coincident Gravitational Waves and High Energy Neutrinos using LIGO, Virgo and ANTARES data from 2007</title>
		<link>http://voxcharta.org/2012/05/14/a-first-search-for-coincident-gravitational-waves-and-high-energy-neutrinos-using-ligo-virgo-and-antares-data-from-2007/</link>
		<comments>http://voxcharta.org/2012/05/14/a-first-search-for-coincident-gravitational-waves-and-high-energy-neutrinos-using-ligo-virgo-and-antares-data-from-2007/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:41:42 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[antares]]></category>
		<category><![CDATA[astronomy]]></category>
		<category><![CDATA[collapse events]]></category>
		<category><![CDATA[core collapse]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[energy neutrino]]></category>
		<category><![CDATA[first science]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[hidden sources]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[ligo]]></category>
		<category><![CDATA[line configuration]]></category>
		<category><![CDATA[merger]]></category>
		<category><![CDATA[messengers]]></category>
		<category><![CDATA[neutrino event]]></category>
		<category><![CDATA[neutrino telescope]]></category>
		<category><![CDATA[virgo]]></category>
		<category><![CDATA[wave signals]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/a-first-search-for-coincident-gravitational-waves-and-high-energy-neutrinos-using-ligo-virgo-and-antares-data-from-2007/</guid>
		<description><![CDATA[We present the results of the first search for gravitational wave bursts associated with high energy neutrinos. Together, these messengers could reveal new, hidden sources that are not observed by conventional photon astronomy, particularly at high energy. Our search uses neutrinos detected by the underwater neutrino telescope ANTARES in its 5 line configuration during the [...]]]></description>
			<content:encoded><![CDATA[<p>We present the results of the first search for gravitational wave bursts associated with high energy neutrinos. Together, these messengers could reveal new, hidden sources that are not observed by conventional photon astronomy, particularly at high energy. Our search uses neutrinos detected by the underwater neutrino telescope ANTARES in its 5 line configuration during the period January &#8211; September 2007, which coincided with the fifth and first science runs of LIGO and Virgo, respectively. The LIGO-Virgo data were analysed for candidate gravitational-wave signals coincident in time and direction with the neutrino events. No significant coincident events were observed. We place limits on the density of joint high energy neutrino &#8211; gravitational wave emission events in the local universe, and compare them with densities of merger and core-collapse events.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/a-first-search-for-coincident-gravitational-waves-and-high-energy-neutrinos-using-ligo-virgo-and-antares-data-from-2007/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>IGR J12319-0749: evidence for another extreme blazar found with INTEGRAL</title>
		<link>http://voxcharta.org/2012/05/14/igr-j12319-0749-evidence-for-another-extreme-blazar-found-with-integral/</link>
		<comments>http://voxcharta.org/2012/05/14/igr-j12319-0749-evidence-for-another-extreme-blazar-found-with-integral/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:41:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion disk]]></category>
		<category><![CDATA[AGN]]></category>
		<category><![CDATA[blazar]]></category>
		<category><![CDATA[broad band]]></category>
		<category><![CDATA[cm 2]]></category>
		<category><![CDATA[compton peak]]></category>
		<category><![CDATA[gamma ray band]]></category>
		<category><![CDATA[hole 2]]></category>
		<category><![CDATA[imager]]></category>
		<category><![CDATA[integral satellite]]></category>
		<category><![CDATA[massive black hole]]></category>
		<category><![CDATA[ray observations]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[rest frame]]></category>
		<category><![CDATA[solar mass]]></category>
		<category><![CDATA[spectral energy distribution]]></category>
		<category><![CDATA[variability]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xrt]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/igr-j12319-0749-evidence-for-another-extreme-blazar-found-with-integral/</guid>
		<description><![CDATA[We report on the identification of a new soft gamma-ray source, IGR J12319-0749, detected with the IBIS imager on board the INTEGRAL satellite. The source, which has an observed 20-100 keV flux of ~8.3 x 10^{-12} erg cm^{-2} s^{-1}, is spatially coincident with an AGN at redshift z=3.12. The broad-band continuum, obtained by combining XRT [...]]]></description>
			<content:encoded><![CDATA[<p>We report on the identification of a new soft gamma-ray source, IGR J12319-0749, detected with the IBIS imager on board the INTEGRAL satellite. The source, which has an observed 20-100 keV flux of ~8.3 x 10^{-12} erg cm^{-2} s^{-1}, is spatially coincident with an AGN at redshift z=3.12. The broad-band continuum, obtained by combining XRT and IBIS data, is flat (Gamma ~ 1.3) with evidence for a spectral break around 25 keV (100 keV in the source rest frame). X-ray observations indicate flux variability which is further supported by a comparison with a previous ROSAT measurement. IGR J12319-0749 is also a radio emitting object likely characterized by a flat spectrum and high radio loudness; optically it is a broad-line emitting object with a massive black hole (2.8 x 10^{9}$ solar masses) at its center. The source Spectral Energy Distribution is similar to another high redshift blazar, 225155+2217 at z=3.668: both objects are bright, with a large accretion disk luminosity and a Compton peak located in the hard X-ray/soft gamma-ray band. IGR J12319-0749 is likely the second most distant blazar detected so far by INTEGRAL.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/igr-j12319-0749-evidence-for-another-extreme-blazar-found-with-integral/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>General Properties of Fermi/LAT Active Galactic Nuclei</title>
		<link>http://voxcharta.org/2012/05/14/general-properties-of-fermilat-active-galactic-nuclei/</link>
		<comments>http://voxcharta.org/2012/05/14/general-properties-of-fermilat-active-galactic-nuclei/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:40:48 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[blazar]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[lacs]]></category>
		<category><![CDATA[population]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/general-properties-of-fermilat-active-galactic-nuclei/</guid>
		<description><![CDATA[The Second Catalog of Blazars and other Active Galactic Nuclei detected by the Fermi/LAT (2LAC) includes about 1100 sources, 886 of which comprise the Clean Sample. The general properties of the different populations of sources classified according to the strength of their emission lines (FSRQs, BL Lacs) or the estimated position of the synchrotron peak [...]]]></description>
			<content:encoded><![CDATA[<p>The Second Catalog of Blazars and other Active Galactic Nuclei detected by the Fermi/LAT (2LAC) includes about 1100 sources, 886 of which comprise the Clean Sample. The general properties of the different populations of sources classified according to the strength of their emission lines (FSRQs, BL Lacs) or the estimated position of the synchrotron peak are reviewed.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/general-properties-of-fermilat-active-galactic-nuclei/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>Limits to the fraction of high-energy photon emitting gamma-ray bursts</title>
		<link>http://voxcharta.org/2012/05/14/limits-to-the-fraction-of-high-energy-photon-emitting-gamma-ray-bursts/</link>
		<comments>http://voxcharta.org/2012/05/14/limits-to-the-fraction-of-high-energy-photon-emitting-gamma-ray-bursts/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:39:55 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accurate reference]]></category>
		<category><![CDATA[angular resolution]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[data suggests that]]></category>
		<category><![CDATA[energy photons]]></category>
		<category><![CDATA[extrapolation]]></category>
		<category><![CDATA[fraction]]></category>
		<category><![CDATA[gamma ray burst]]></category>
		<category><![CDATA[grbs]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[image co]]></category>
		<category><![CDATA[mev]]></category>
		<category><![CDATA[photon emission]]></category>
		<category><![CDATA[ray space]]></category>
		<category><![CDATA[reference point]]></category>
		<category><![CDATA[space telescope]]></category>
		<category><![CDATA[two instruments]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/limits-to-the-fraction-of-high-energy-photon-emitting-gamma-ray-bursts/</guid>
		<description><![CDATA[After almost 4 years of operation, the two instruments onboard the Fermi Gamma-ray Space Telescope have shown that the number of gamma-ray bursts with high energy photon emission above 100 MeV cannot exceed roughly 9% of the total number of all such events, at least at the present detection limits. In a recent paper (Zheng [...]]]></description>
			<content:encoded><![CDATA[<p>After almost 4 years of operation, the two instruments onboard the Fermi Gamma-ray Space Telescope have shown that the number of gamma-ray bursts with high energy photon emission above 100 MeV cannot exceed roughly 9% of the total number of all such events, at least at the present detection limits. In a recent paper (Zheng et al. 2012c), we found that GRBs with photons detected in the Large Area Telescope (LAT) have a surprisingly broad distribution with respect to the photon number above background. Extrapolation of our empirical fit to numbers of photons below our quoted detection limit suggests that the overall rate of such events could be determined by standard image co-adding techniques. In this case, we have taken advantage of the excellent angular resolution of the Swift mission to provide accurate reference points for 79 GRB events which have eluded any previous correlations with high energy photons. We find a small but significant signal. Guided by the power law fit obtained previously for the number distribution of GRBs, the data suggests that only a small fraction of GRBs are sources of high energy photons.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/limits-to-the-fraction-of-high-energy-photon-emitting-gamma-ray-bursts/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Radio Searches of Fermi LAT Sources and Blind Search Pulsars: The Fermi Pulsar Search Consortium</title>
		<link>http://voxcharta.org/2012/05/14/radio-searches-of-fermi-lat-sources-and-blind-search-pulsars-the-fermi-pulsar-search-consortium/</link>
		<comments>http://voxcharta.org/2012/05/14/radio-searches-of-fermi-lat-sources-and-blind-search-pulsars-the-fermi-pulsar-search-consortium/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:39:04 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[black widow]]></category>
		<category><![CDATA[blind search]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[frequency search]]></category>
		<category><![CDATA[galactic disk]]></category>
		<category><![CDATA[gamma ray sources]]></category>
		<category><![CDATA[international collaboration]]></category>
		<category><![CDATA[msp]]></category>
		<category><![CDATA[new radio]]></category>
		<category><![CDATA[observers]]></category>
		<category><![CDATA[promising candidate]]></category>
		<category><![CDATA[pulsar candidates]]></category>
		<category><![CDATA[pulsars]]></category>
		<category><![CDATA[pulsation]]></category>
		<category><![CDATA[radio astronomers]]></category>
		<category><![CDATA[radio search]]></category>
		<category><![CDATA[radio telescope]]></category>
		<category><![CDATA[source population]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[variability]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/radio-searches-of-fermi-lat-sources-and-blind-search-pulsars-the-fermi-pulsar-search-consortium/</guid>
		<description><![CDATA[We present a summary of the Fermi Pulsar Search Consortium (PSC), an international collaboration of radio astronomers and members of the Large Area Telescope (LAT) collaboration, whose goal is to organize radio follow-up observations of Fermi pulsars and pulsar candidates among the LAT gamma-ray source population. The PSC includes pulsar observers with expertise using the [...]]]></description>
			<content:encoded><![CDATA[<p>We present a summary of the Fermi Pulsar Search Consortium (PSC), an international collaboration of radio astronomers and members of the Large Area Telescope (LAT) collaboration, whose goal is to organize radio follow-up observations of Fermi pulsars and pulsar candidates among the LAT gamma-ray source population. The PSC includes pulsar observers with expertise using the world&#8217;s largest radio telescopes that together cover the full sky. We have performed very deep observations of all 35 pulsars discovered in blind frequency searches of the LAT data, resulting in the discovery of radio pulsations from four of them. We have also searched over 300 LAT gamma-ray sources that do not have strong associations with known gamma-ray emitting source classes and have pulsar-like spectra and variability characteristics. These searches have led to the discovery of a total of 43 new radio millisecond pulsars (MSPs) and four normal pulsars. These discoveries greatly increase the known population of MSPs in the Galactic disk, more than double the known population of so-called `black widow&#8217; pulsars, and contain many promising candidates for inclusion in pulsar timing arrays.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/radio-searches-of-fermi-lat-sources-and-blind-search-pulsars-the-fermi-pulsar-search-consortium/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Gravitational Asynchronous Machine</title>
		<link>http://voxcharta.org/2012/05/14/the-gravitational-asynchronous-machine/</link>
		<comments>http://voxcharta.org/2012/05/14/the-gravitational-asynchronous-machine/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:37:57 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astrophysics]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[consensus]]></category>
		<category><![CDATA[phenomena]]></category>
		<category><![CDATA[relativistic jet]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/the-gravitational-asynchronous-machine/</guid>
		<description><![CDATA[How relativistic jets are generated is one of the hottest topics of the modern astrophysics. Several theories have been proposed to explain the wide variety of observed phenomena, but none seems to catch the general consensus, although the mechanism proposed for black holes in 1977 by Blandford &#38; Znajek (BZ) deserves some favor. In the [...]]]></description>
			<content:encoded><![CDATA[<p>How relativistic jets are generated is one of the hottest topics of the modern astrophysics. Several theories have been proposed to explain the wide variety of observed phenomena, but none seems to catch the general consensus, although the mechanism proposed for black holes in 1977 by Blandford &amp; Znajek (BZ) deserves some favor. In the following essay, I study some relatively unexplored features in the black hole/jet/disk feedback as derived from the application of the BZ theory.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/the-gravitational-asynchronous-machine/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Evaluation of the discovery potential of an underwater Mediterranean neutrino telescope taking into account the estimated directional resolution and energy of the reconstructed tracks [Replacement]</title>
		<link>http://voxcharta.org/2012/05/14/evaluation-of-the-discovery-potential-of-an-underwater-mediterranean-neutrino-telescope-taking-into-account-the-estimated-directional-resolution-and-energy-of-the-reconstructed-tracks-replacement/</link>
		<comments>http://voxcharta.org/2012/05/14/evaluation-of-the-discovery-potential-of-an-underwater-mediterranean-neutrino-telescope-taking-into-account-the-estimated-directional-resolution-and-energy-of-the-reconstructed-tracks-replacement/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:35:07 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[capability]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[estimation]]></category>
		<category><![CDATA[neutrino telescope]]></category>
		<category><![CDATA[search method]]></category>
		<category><![CDATA[significant improvement]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/evaluation-of-the-discovery-potential-of-an-underwater-mediterranean-neutrino-telescope-taking-into-account-the-estimated-directional-resolution-and-energy-of-the-reconstructed-tracks-replacement/</guid>
		<description><![CDATA[We report on the development of search methods for point-like and extended neutrino sources, utilizing the tracking and energy estimation capabilities of an underwater, Very Large Volume Neutrino Telescope (VLVnT). We demonstrate that the developed techniques offer a significant improvement on the telescope&#8217;s discovery potential. We also present results on the potential of the Mediterranean [...]]]></description>
			<content:encoded><![CDATA[<p>We report on the development of search methods for point-like and extended neutrino sources, utilizing the tracking and energy estimation capabilities of an underwater, Very Large Volume Neutrino Telescope (VLVnT). We demonstrate that the developed techniques offer a significant improvement on the telescope&#8217;s discovery potential. We also present results on the potential of the Mediterranean KM3NeT to discover galactic neutrino sources.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/evaluation-of-the-discovery-potential-of-an-underwater-mediterranean-neutrino-telescope-taking-into-account-the-estimated-directional-resolution-and-energy-of-the-reconstructed-tracks-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The presence of Primordial Gravitational Waves in the Cosmic Microwave Background [Replacement]</title>
		<link>http://voxcharta.org/2012/05/14/the-presence-of-primordial-gravitational-waves-in-the-cosmic-microwave-background-replacement/</link>
		<comments>http://voxcharta.org/2012/05/14/the-presence-of-primordial-gravitational-waves-in-the-cosmic-microwave-background-replacement/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:34:35 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[cosmic microwave background]]></category>
		<category><![CDATA[general relativity]]></category>
		<category><![CDATA[gravitational field]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[radiation]]></category>
		<category><![CDATA[wave length]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/the-presence-of-primordial-gravitational-waves-in-the-cosmic-microwave-background-replacement/</guid>
		<description><![CDATA[The General Relativity affirms that any field is a source of gravitational field, thus one should affirm that the energy of Cosmic Microwave Background (CMB) generated primordial gravitational waves. The present article shows that a gravitational wave with dimensionless amplitude $\sim 10^{-5}$ and large wave length $\sim 10$ megaparsecs shifts temperature of CMB radiation about [...]]]></description>
			<content:encoded><![CDATA[<p>The General Relativity affirms that any field is a source of gravitational field, thus one should affirm that the energy of Cosmic Microwave Background (CMB) generated primordial gravitational waves. The present article shows that a gravitational wave with dimensionless amplitude $\sim 10^{-5}$ and large wave length $\sim 10$ megaparsecs shifts temperature of CMB radiation about of a part in $10^{5}$.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/the-presence-of-primordial-gravitational-waves-in-the-cosmic-microwave-background-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Ultra-high energy cosmic ray correlations with Active Galactic Nuclei in the world dataset [Replacement]</title>
		<link>http://voxcharta.org/2012/05/14/ultra-high-energy-cosmic-ray-correlations-with-active-galactic-nuclei-in-the-world-dataset-replacement/</link>
		<comments>http://voxcharta.org/2012/05/14/ultra-high-energy-cosmic-ray-correlations-with-active-galactic-nuclei-in-the-world-dataset-replacement/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:33:56 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[agasa]]></category>
		<category><![CDATA[arrival direction]]></category>
		<category><![CDATA[blind test]]></category>
		<category><![CDATA[collaboration]]></category>
		<category><![CDATA[consistency]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[energy scale]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[highest energy]]></category>
		<category><![CDATA[hypothesis]]></category>
		<category><![CDATA[pierre auger]]></category>
		<category><![CDATA[random background]]></category>
		<category><![CDATA[subset]]></category>
		<category><![CDATA[world dataset]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/ultra-high-energy-cosmic-ray-correlations-with-active-galactic-nuclei-in-the-world-dataset-replacement/</guid>
		<description><![CDATA[Pierre Auger collaboration have recently put forward the hypothesis that the arrival directions of the highest energy cosmic rays correlate with the subset of local active galactic nuclei (AGN). We perform a blind test of AGN hypothesis using publicly available event sets collected by Yakutsk, AGASA and HiRes experiments. The consistency of the procedure requires [...]]]></description>
			<content:encoded><![CDATA[<p>Pierre Auger collaboration have recently put forward the hypothesis that the arrival directions of the highest energy cosmic rays correlate with the subset of local active galactic nuclei (AGN). We perform a blind test of AGN hypothesis using publicly available event sets collected by Yakutsk, AGASA and HiRes experiments. The consistency of the procedure requires the event energies to be normalized towards the common energy scale. The number of correlating events in resulting data-set is 3 of 21 which is consistent with expected random background.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/ultra-high-energy-cosmic-ray-correlations-with-active-galactic-nuclei-in-the-world-dataset-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Upper Bounds on Asymmetric Dark Matter Self Annihilation Cross Sections [Replacement]</title>
		<link>http://voxcharta.org/2012/05/14/upper-bounds-on-asymmetric-dark-matter-self-annihilation-cross-sections-replacement/</link>
		<comments>http://voxcharta.org/2012/05/14/upper-bounds-on-asymmetric-dark-matter-self-annihilation-cross-sections-replacement/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:33:34 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absence]]></category>
		<category><![CDATA[angle]]></category>
		<category><![CDATA[annihilation]]></category>
		<category><![CDATA[asymmetry]]></category>
		<category><![CDATA[boltzmann equation]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[cross section]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[scenarios]]></category>
		<category><![CDATA[temperature]]></category>
		<category><![CDATA[upper bound]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/upper-bounds-on-asymmetric-dark-matter-self-annihilation-cross-sections-replacement/</guid>
		<description><![CDATA[Most models for asymmetric dark matter allow for dark matter self annihilation processes, which can wash out the asymmetry at temperatures near and below the dark matter mass. We study the coupled set of Boltzmann equations for the symmetric and antisymmetric dark matter number densities, and derive conditions applicable to a large class of models [...]]]></description>
			<content:encoded><![CDATA[<p>Most models for asymmetric dark matter allow for dark matter self annihilation processes, which can wash out the asymmetry at temperatures near and below the dark matter mass. We study the coupled set of Boltzmann equations for the symmetric and antisymmetric dark matter number densities, and derive conditions applicable to a large class of models for the absence of a significant wash-out of an asymmetry. These constraints are applied to various existing scenarios. In the case of left- or right-handed sneutrinos, very large electroweak gaugino masses, or very small mixing angles are required.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/upper-bounds-on-asymmetric-dark-matter-self-annihilation-cross-sections-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>Extra U(1) as natural source of a monochromatic gamma ray line [Replacement]</title>
		<link>http://voxcharta.org/2012/05/14/extra-u1-as-natural-source-of-a-monochromatic-gamma-ray-line-replacement/</link>
		<comments>http://voxcharta.org/2012/05/14/extra-u1-as-natural-source-of-a-monochromatic-gamma-ray-line-replacement/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:33:11 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[chern]]></category>
		<category><![CDATA[coupling]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[gauge]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[heavy fermions]]></category>
		<category><![CDATA[line extensions]]></category>
		<category><![CDATA[natural source]]></category>
		<category><![CDATA[natural values]]></category>
		<category><![CDATA[standard model]]></category>
		<category><![CDATA[Telescope]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/extra-u1-as-natural-source-of-a-monochromatic-gamma-ray-line-replacement/</guid>
		<description><![CDATA[Extensions of the Standard Model with an extra U&#8217;(1) abelian group generically generate terms coming from loops of heavy fermions, leading to three gauge boson couplings, in particular Z&#8217;Z gamma. We show that WMAP data constrains the gauge coupling of the group g_D to values comparable with the electro-weak ones, rather independently of the mass [...]]]></description>
			<content:encoded><![CDATA[<p>Extensions of the Standard Model with an extra U&#8217;(1) abelian group generically generate terms coming from loops of heavy fermions, leading to three gauge boson couplings, in particular Z&#8217;Z gamma. We show that WMAP data constrains the gauge coupling of the group g_D to values comparable with the electro-weak ones, rather independently of the mass of Z&#8217;. Moreover, the model predicts a monochromatic gamma-ray line which can fit a 130 GeV signal at the FERMI telescope for natural values of the Chern-Simons terms and a dark matter mass around 144.5 GeV.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/extra-u1-as-natural-source-of-a-monochromatic-gamma-ray-line-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Hot Electron and Pair Production from the Texas Petawatt Laser Irradiating Thick Gold Targets [Replacement]</title>
		<link>http://voxcharta.org/2012/05/14/hot-electron-and-pair-production-from-the-texas-petawatt-laser-irradiating-thick-gold-targets-replacement/</link>
		<comments>http://voxcharta.org/2012/05/14/hot-electron-and-pair-production-from-the-texas-petawatt-laser-irradiating-thick-gold-targets-replacement/#comments</comments>
		<pubDate>Tue, 15 May 2012 00:33:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cm 2]]></category>
		<category><![CDATA[deconvolution algorithm]]></category>
		<category><![CDATA[direct evidence]]></category>
		<category><![CDATA[electron]]></category>
		<category><![CDATA[energy spectra]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[intensity]]></category>
		<category><![CDATA[magnetic spectrometer]]></category>
		<category><![CDATA[Measurement]]></category>
		<category><![CDATA[mev]]></category>
		<category><![CDATA[pair production]]></category>
		<category><![CDATA[petawatt laser]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[target]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/14/hot-electron-and-pair-production-from-the-texas-petawatt-laser-irradiating-thick-gold-targets-replacement/</guid>
		<description><![CDATA[We present data from electron-positron pair production by an ultra-intense laser incident on solid Au targets with thickness between 1 and 4 mm. The experiment was performed at the Texas Petawatt Laser in July 2011, with intensities on the order of several x1019W.cm-2 and laser energies around 50 J. We discuss the design of an [...]]]></description>
			<content:encoded><![CDATA[<p>We present data from electron-positron pair production by an ultra-intense laser incident on solid Au targets with thickness between 1 and 4 mm. The experiment was performed at the Texas Petawatt Laser in July 2011, with intensities on the order of several x1019W.cm-2 and laser energies around 50 J. We discuss the design of an electron-positron magnetic spectrometer to record the lepton energy spectra ejected from the Au targets. We then present a deconvolution algorithm to extract the lepton energy spectra. We measured hot electron spectra out to &gt; 50 MeV, which show a narrow peak around 10 &#8211; 15 MeV, plus exponential tail consistent with ponderomotive temperature scaling. We did not observe direct evidence of positron production above the background, even though separate gamma-ray measurement hints at the presence of positrons.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/14/hot-electron-and-pair-production-from-the-texas-petawatt-laser-irradiating-thick-gold-targets-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>
		</item>
		<item>
		<title>Residual Cooling and Persistent Star Formation amid AGN Feedback in Abell 2597</title>
		<link>http://voxcharta.org/2012/05/13/residual-cooling-and-persistent-star-formation-amid-agn-feedback-in-abell-2597/</link>
		<comments>http://voxcharta.org/2012/05/13/residual-cooling-and-persistent-star-formation-amid-agn-feedback-in-abell-2597/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:53:54 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[abell]]></category>
		<category><![CDATA[bcg]]></category>
		<category><![CDATA[chandra observation]]></category>
		<category><![CDATA[chandra x ray]]></category>
		<category><![CDATA[cluster galaxy]]></category>
		<category><![CDATA[cold dust]]></category>
		<category><![CDATA[cold gas]]></category>
		<category><![CDATA[cooling flow]]></category>
		<category><![CDATA[dominant contributor]]></category>
		<category><![CDATA[filament]]></category>
		<category><![CDATA[fuv]]></category>
		<category><![CDATA[galactic nucleus]]></category>
		<category><![CDATA[herschel]]></category>
		<category><![CDATA[kiloparsec]]></category>
		<category><![CDATA[previous results]]></category>
		<category><![CDATA[radio lobes]]></category>
		<category><![CDATA[star formation rate]]></category>
		<category><![CDATA[thermal instability]]></category>
		<category><![CDATA[time profile]]></category>
		<category><![CDATA[young stars]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/residual-cooling-and-persistent-star-formation-amid-agn-feedback-in-abell-2597/</guid>
		<description><![CDATA[New Chandra X-ray and Herschel FIR observations enable a multiwavelength study of active galactic nucleus (AGN) heating and intracluster medium (ICM) cooling in the brightest cluster galaxy of Abell 2597. The new Chandra observations reveal the central &#60; 30 kiloparsec X-ray cavity network to be more extensive than previously thought, and associated with enough enthalpy [...]]]></description>
			<content:encoded><![CDATA[<p>New Chandra X-ray and Herschel FIR observations enable a multiwavelength study of active galactic nucleus (AGN) heating and intracluster medium (ICM) cooling in the brightest cluster galaxy of Abell 2597. The new Chandra observations reveal the central &lt; 30 kiloparsec X-ray cavity network to be more extensive than previously thought, and associated with enough enthalpy to theoretically inhibit the inferred classical cooling flow. Nevertheless, we present new evidence, consistent with previous results, that a moderately strong residual cooling flow is persisting at 4%-8% of the classically predicted rates in a spatially structured manner amid the feedback-driven excavation of the X-ray cavity network. New Herschel observations are used to estimate warm and cold dust masses, a lower-limit gas-to-dust ratio, and a star formation rate consistent with previous measurements. The cooling time profile of the ambient X-ray atmosphere is used to map the locations of the observational star formation entropy threshold as well as the theoretical thermal instability threshold. Both lie just outside the &lt; 30 kpc central region permeated by X-ray cavities, and star formation as well as ionized and molecular gas lie interior to both. The young stars are distributed in an elongated region that is aligned with the radio lobes, and their estimated ages are both younger and older than the X-ray cavity network, suggesting both jet-triggered as well as persistent star formation over the current AGN feedback episode. Bright X-ray knots that are coincident with extended Ly-alpha and FUV continuum filaments motivate a discussion of structured cooling from the ambient hot atmosphere along a projected axis that is perpendicular to X-ray cavity and radio axis. We conclude that the cooling ICM is the dominant contributor of the cold gas reservoir fueling star formation and AGN activity in the Abell 2597 BCG.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/residual-cooling-and-persistent-star-formation-amid-agn-feedback-in-abell-2597/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Multiphase Signatures of AGN Feedback in Abell 2597</title>
		<link>http://voxcharta.org/2012/05/13/multiphase-signatures-of-agn-feedback-in-abell-2597/</link>
		<comments>http://voxcharta.org/2012/05/13/multiphase-signatures-of-agn-feedback-in-abell-2597/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:53:32 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bcg]]></category>
		<category><![CDATA[caveat]]></category>
		<category><![CDATA[cavity]]></category>
		<category><![CDATA[chandra x ray]]></category>
		<category><![CDATA[cluster abell]]></category>
		<category><![CDATA[cluster galaxy]]></category>
		<category><![CDATA[cold gas]]></category>
		<category><![CDATA[core cluster]]></category>
		<category><![CDATA[excess gas]]></category>
		<category><![CDATA[filament]]></category>
		<category><![CDATA[galactic nucleus]]></category>
		<category><![CDATA[inner edge]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[observational evidence]]></category>
		<category><![CDATA[radio data]]></category>
		<category><![CDATA[radio source]]></category>
		<category><![CDATA[ray observations]]></category>
		<category><![CDATA[spatial correlation]]></category>
		<category><![CDATA[spectral analysis]]></category>
		<category><![CDATA[spectral maps]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/multiphase-signatures-of-agn-feedback-in-abell-2597/</guid>
		<description><![CDATA[We present new Chandra X-ray observations of the brightest cluster galaxy (BCG) in the cool core cluster Abell 2597. The data reveal an extensive kpc-scale X-ray cavity network as well as a 15 kpc filament of soft-excess gas exhibiting strong spatial correlation with archival VLA radio data. In addition to several possible scenarios, multiwavelength evidence [...]]]></description>
			<content:encoded><![CDATA[<p>We present new Chandra X-ray observations of the brightest cluster galaxy (BCG) in the cool core cluster Abell 2597. The data reveal an extensive kpc-scale X-ray cavity network as well as a 15 kpc filament of soft-excess gas exhibiting strong spatial correlation with archival VLA radio data. In addition to several possible scenarios, multiwavelength evidence may suggest that the filament is associated with multiphase (10^3 &#8211; 10^7 K) gas that has been entrained and dredged-up by the propagating radio source. Stemming from a full spectral analysis, we also present profiles and 2D spectral maps of modeled X-ray temperature, entropy, pressure, and metal abundance. The maps reveal an arc of hot gas which in projection borders the inner edge of a large X-ray cavity. Although limited by strong caveats, we suggest that the hot arc may be (a) due to a compressed rim of cold gas pushed outward by the radio bubble or (b) morphologically and energetically consistent with cavity-driven active galactic nucleus (AGN) heating models invoked to quench cooling flows, in which the enthalpy of a buoyant X-ray cavity is locally thermalized as ambient gas rushes to refill its wake. If confirmed, this would be the first observational evidence for this model.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/multiphase-signatures-of-agn-feedback-in-abell-2597/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Type Ib/c Supernovae with and without Gamma-Ray Bursts</title>
		<link>http://voxcharta.org/2012/05/13/type-ibc-supernovae-with-and-without-gamma-ray-bursts/</link>
		<comments>http://voxcharta.org/2012/05/13/type-ibc-supernovae-with-and-without-gamma-ray-bursts/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:50:16 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[explosion]]></category>
		<category><![CDATA[gamma ray burst]]></category>
		<category><![CDATA[grbs]]></category>
		<category><![CDATA[meta analysis]]></category>
		<category><![CDATA[metallicity]]></category>
		<category><![CDATA[observational study]]></category>
		<category><![CDATA[oxygen]]></category>
		<category><![CDATA[rich environment]]></category>
		<category><![CDATA[SNe]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectroscopic]]></category>
		<category><![CDATA[supernovae]]></category>
		<category><![CDATA[velocities]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/type-ibc-supernovae-with-and-without-gamma-ray-bursts/</guid>
		<description><![CDATA[While the connection between Long Gamma-Ray Bursts (GRBs) and Type Ib/c Supernovae (SNe Ib/c) from stripped stars has been well-established, one key outstanding question is what conditions and factors lead to each kind of explosion in massive stripped stars. One promising line of attack is to investigate what sets apart SNe Ib/c with GRBs from [...]]]></description>
			<content:encoded><![CDATA[<p>While the connection between Long Gamma-Ray Bursts (GRBs) and Type Ib/c Supernovae (SNe Ib/c) from stripped stars has been well-established, one key outstanding question is what conditions and factors lead to each kind of explosion in massive stripped stars. One promising line of attack is to investigate what sets apart SNe Ib/c with GRBs from those without GRBs. Here, I briefly present two observational studies that probe the SN properties and the environmental metallicities of SNe Ib/c (specifically broad-lined SNe Ic) with and without GRBs. I present an analysis of expansion velocities based on published spectra and on the homogeneous spectroscopic CfA data set of over 70 SNe of Types IIb, Ib, Ic and Ic-bl, which triples the world supply of well-observed Stripped SNe. Moreover, I demonstrate that a meta-analysis of the three published SN Ib/c metallicity data sets, when including only values at the SN positions to probe natal oxygen abundances, indicates at very high significance that indeed SNe Ic erupt from more metal-rich environments than SNe Ib, while SNe Ic-bl with GRBs still prefer, on average, more metal-poor sites than those without GRBs.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/type-ibc-supernovae-with-and-without-gamma-ray-bursts/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Increasing the Number of TeV Blazars with Parsec-Scale Kinematics</title>
		<link>http://voxcharta.org/2012/05/13/increasing-the-number-of-tev-blazars-with-parsec-scale-kinematics/</link>
		<comments>http://voxcharta.org/2012/05/13/increasing-the-number-of-tev-blazars-with-parsec-scale-kinematics/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:49:40 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[blazar]]></category>
		<category><![CDATA[epochs]]></category>
		<category><![CDATA[faintness]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[gradient]]></category>
		<category><![CDATA[high frequency]]></category>
		<category><![CDATA[jet properties]]></category>
		<category><![CDATA[jet speed]]></category>
		<category><![CDATA[lorentz factor]]></category>
		<category><![CDATA[measurements]]></category>
		<category><![CDATA[radio jet]]></category>
		<category><![CDATA[radio properties]]></category>
		<category><![CDATA[scale radio]]></category>
		<category><![CDATA[survey]]></category>
		<category><![CDATA[telescopes]]></category>
		<category><![CDATA[tev energy range]]></category>
		<category><![CDATA[very long baseline array]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/increasing-the-number-of-tev-blazars-with-parsec-scale-kinematics/</guid>
		<description><![CDATA[We report on our observations of the parsec-scale radio jet structures of five blazars that have been detected by ground-based TeV gamma-ray telescopes. These five blazars all belong to the class of high-frequency peaked BL Lac objects (HBLs), which are the most common blazar type detected at the TeV energy range. Because of their relative [...]]]></description>
			<content:encoded><![CDATA[<p>We report on our observations of the parsec-scale radio jet structures of five blazars that have been detected by ground-based TeV gamma-ray telescopes. These five blazars all belong to the class of high-frequency peaked BL Lac objects (HBLs), which are the most common blazar type detected at the TeV energy range. Because of their relative faintness in the radio, these HBLs are not well represented in other radio blazar surveys. Our observations consist of five epochs of Very Long Baseline Array (VLBA) imaging from 2006 to 2009, of each of the five blazars 1ES 1101-232, Markarian 180, 1ES 1218+304, PG 1553+113, and H 2356-309, at frequencies from 5 to 22 GHz. Fundamental jet properties, including the apparent jet speeds, that can be measured from these multi-epoch series of VLBA images are presented and compared with other gamma-ray blazars. Confirming prior work, we find that the TeV HBLs have significantly slower apparent jet speeds than radio-selected blazars. Together with other radio properties of the HBL class, this suggests modest Lorentz factors in their parsec-scale radio jets. This in turn suggests some form of Lorentz factor gradient in these jets, since they are likely to have high Lorentz factors in their TeV-emitting regions. The study presented here approximately doubles the number of TeV HBLs with multi-epoch parsec-scale kinematic measurements.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/increasing-the-number-of-tev-blazars-with-parsec-scale-kinematics/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>ATCA monitoring of gamma-ray loud AGN</title>
		<link>http://voxcharta.org/2012/05/13/atca-monitoring-of-gamma-ray-loud-agn/</link>
		<comments>http://voxcharta.org/2012/05/13/atca-monitoring-of-gamma-ray-loud-agn/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:49:05 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[AGN]]></category>
		<category><![CDATA[australia telescope]]></category>
		<category><![CDATA[changes over time]]></category>
		<category><![CDATA[egret]]></category>
		<category><![CDATA[Fermi]]></category>
		<category><![CDATA[gamma ray emission]]></category>
		<category><![CDATA[jets]]></category>
		<category><![CDATA[mechanic]]></category>
		<category><![CDATA[monitoring program]]></category>
		<category><![CDATA[radio spectra]]></category>
		<category><![CDATA[ray space]]></category>
		<category><![CDATA[southern hemisphere]]></category>
		<category><![CDATA[space observatory]]></category>
		<category><![CDATA[spectral index]]></category>
		<category><![CDATA[telescope compact array]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/atca-monitoring-of-gamma-ray-loud-agn/</guid>
		<description><![CDATA[As a critical part of the Tracking Active Galactic Nuclei with Austral Milliarcsecond Interferometry (TANAMI) program, in November 2007 the Australia Telescope Compact Array (ATCA) started monitoring the radio spectra of a sample of southern hemisphere active galactic nuclei (AGN) that were selected as likely candidates for detection (as well as a control sample) by [...]]]></description>
			<content:encoded><![CDATA[<p>As a critical part of the Tracking Active Galactic Nuclei with Austral Milliarcsecond Interferometry (TANAMI) program, in November 2007 the Australia Telescope Compact Array (ATCA) started monitoring the radio spectra of a sample of southern hemisphere active galactic nuclei (AGN) that were selected as likely candidates for detection (as well as a control sample) by the Large Area Telescope (LAT) aboard the Fermi Gamma Ray Space Observatory. The initial sample was chosen based on properties determined from AGN detections by the Energetic Gamma Ray Experiment Telescope (EGRET). Most of the initial sample has been detected by Fermi/LAT and with the addition of new detections the sample has grown to include 226 AGN, 133 of which have data for more than one epoch. For the majority of these AGN, our monitoring program provides the only dynamic radio spectra available. The ATCA receiver suite makes it possible to observe several sources at frequencies between 4.5 and 41 GHz in a few hours, resulting in an excellent measure of spectral index at each epoch. By examining how the spectral index changes over time, we aim to investigate the mechanics of radio and gamma-ray emission from AGN jets.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/atca-monitoring-of-gamma-ray-loud-agn/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Correlation between Peak Energy and Peak Luminosity in Short Gamma-Ray Bursts</title>
		<link>http://voxcharta.org/2012/05/13/correlation-between-peak-energy-and-peak-luminosity-in-short-gamma-ray-bursts/</link>
		<comments>http://voxcharta.org/2012/05/13/correlation-between-peak-energy-and-peak-luminosity-in-short-gamma-ray-bursts/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:48:11 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[dissipation]]></category>
		<category><![CDATA[gamma ray burst]]></category>
		<category><![CDATA[law index]]></category>
		<category><![CDATA[necessary data]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[peak energy]]></category>
		<category><![CDATA[peak luminosity]]></category>
		<category><![CDATA[photosphere]]></category>
		<category><![CDATA[physical constraint]]></category>
		<category><![CDATA[synchrotron radiation]]></category>
		<category><![CDATA[theoretical model]]></category>
		<category><![CDATA[thermal emission]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/correlation-between-peak-energy-and-peak-luminosity-in-short-gamma-ray-bursts/</guid>
		<description><![CDATA[A correlation between the peak luminosity and the peak energy has been found by Yonetoku et al. as $L_{p}\propto E_{p,i}^{2.0}$ for 11 pre-Swift long gamma-ray bursts. In this study, for a greatly expanded sample of 148 long gamma-ray bursts in the Swift era, we find that the correlation still exists, but most likely with a [...]]]></description>
			<content:encoded><![CDATA[<p>A correlation between the peak luminosity and the peak energy has been found by Yonetoku et al. as $L_{p}\propto E_{p,i}^{2.0}$ for 11 pre-Swift long gamma-ray bursts. In this study, for a greatly expanded sample of 148 long gamma-ray bursts in the Swift era, we find that the correlation still exists, but most likely with a slightly different power-law index, i.e., $L_{p}\propto E_{p,i} ^{1.7}$. In addition, we have collected 17 short gamma-ray bursts with necessary data. It is found that the correlation of $L_{p}\propto E_{p,i} ^{1.7}$ also exists for this sample of short events. It is argued that the radiation mechanism of both long and short gamma-ray bursts should be similar, i.e., of quasi-thermal origin caused by the photosphere and the dissipation occurring very near the central engine. Some key parameters of the process are constrained. Our results suggest that the radiation process of both long and short bursts may be dominated by thermal emission, rather than the single synchrotron radiation. This might put strong physical constraints on the theoretical models.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/correlation-between-peak-energy-and-peak-luminosity-in-short-gamma-ray-bursts/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Multiwavelength Astronomy and CTA: X-rays</title>
		<link>http://voxcharta.org/2012/05/13/multiwavelength-astronomy-and-cta-x-rays/</link>
		<comments>http://voxcharta.org/2012/05/13/multiwavelength-astronomy-and-cta-x-rays/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:46:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[astrophysical sources]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[clusters of galaxies]]></category>
		<category><![CDATA[depth investigation]]></category>
		<category><![CDATA[energy particle]]></category>
		<category><![CDATA[energy universe]]></category>
		<category><![CDATA[future x]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[observational result]]></category>
		<category><![CDATA[observatory]]></category>
		<category><![CDATA[ray astronomy]]></category>
		<category><![CDATA[ray observations]]></category>
		<category><![CDATA[rosita]]></category>
		<category><![CDATA[supernova remnant]]></category>
		<category><![CDATA[suzaku]]></category>
		<category><![CDATA[telescope array]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[xmm newton]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/multiwavelength-astronomy-and-cta-x-rays/</guid>
		<description><![CDATA[We discuss how future X-ray instruments which are under development can contribute to our understanding of the non-thermal Universe. Much progress has been made in the field of X-ray Astronomy recently, thanks to the operation of modern X-ray telescopes such as Chandra, XMM-Newton, Suzaku, and Swift, but more in-depth investigation awaits future missions. These future [...]]]></description>
			<content:encoded><![CDATA[<p>We discuss how future X-ray instruments which are under development can contribute to our understanding of the non-thermal Universe. Much progress has been made in the field of X-ray Astronomy recently, thanks to the operation of modern X-ray telescopes such as Chandra, XMM-Newton, Suzaku, and Swift, but more in-depth investigation awaits future missions. These future missions include ASTROSAT, NuStar, e-ROSITA, ASTRO-H and GEMS, which will be realized in the next decade, and also much larger projects such as Athena and LOFT, which have been proposed for the 2020&#8217;s. All of those are expected to bring a variety of novel observational results regarding astrophysical sources of high-energy particles and radiation, i.e. supernova remnants, neutron stars, stellar-mass black holes, active galaxies, and clusters of galaxies among others. The operation of the future X-ray instruments will proceed in parallel with the operation of Fermi-LAT and the Cherenkov Telescope Array. We emphasize that the synergy between the X-ray and gamma-ray observations is particularly important, and that the planned X-ray missions, when in conjunction with the modern gamma-ray observatories, will indeed provide a qualitatively better insight into the high-energy Universe.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/multiwavelength-astronomy-and-cta-x-rays/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Defect formation from defect&#8211;anti-defect annihilations [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/13/defect-formation-from-defect-anti-defect-annihilations-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/13/defect-formation-from-defect-anti-defect-annihilations-cross-listing/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:45:47 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[defect formation]]></category>
		<category><![CDATA[domain wall]]></category>
		<category><![CDATA[topological defects]]></category>
		<category><![CDATA[world volume]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/defect-formation-from-defect-anti-defect-annihilations-cross-listing/</guid>
		<description><![CDATA[We show that when a topological defect with extended world-volume annihilates with an anti-defect, there arise topological defects with dimensions less than those of the original defects by one. Domain wall annihilations create vortices while monopole-string annihilations result in instantons. We find that twisted domain wall rings are vortices, whereas twisted monopole rings are instantons.
]]></description>
			<content:encoded><![CDATA[<p>We show that when a topological defect with extended world-volume annihilates with an anti-defect, there arise topological defects with dimensions less than those of the original defects by one. Domain wall annihilations create vortices while monopole-string annihilations result in instantons. We find that twisted domain wall rings are vortices, whereas twisted monopole rings are instantons.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/defect-formation-from-defect-anti-defect-annihilations-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Knots from wall&#8211;anti-wall annihilations with stretched strings [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/13/knots-from-wall-anti-wall-annihilations-with-stretched-strings-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/13/knots-from-wall-anti-wall-annihilations-with-stretched-strings-cross-listing/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:45:36 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[annihilation]]></category>
		<category><![CDATA[domain wall]]></category>
		<category><![CDATA[knot]]></category>
		<category><![CDATA[stretched strings]]></category>
		<category><![CDATA[vortex]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/knots-from-wall-anti-wall-annihilations-with-stretched-strings-cross-listing/</guid>
		<description><![CDATA[A pair of a domain wall and an anti-domain wall is unstable to decay. We show that when a vortex-string is stretched between the walls, there remains a knot soliton (Hopfion) after the pair annihilation.
]]></description>
			<content:encoded><![CDATA[<p>A pair of a domain wall and an anti-domain wall is unstable to decay. We show that when a vortex-string is stretched between the walls, there remains a knot soliton (Hopfion) after the pair annihilation.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/knots-from-wall-anti-wall-annihilations-with-stretched-strings-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Connection between Radio and Gamma Ray Emission in Fermi/LAT Blazars</title>
		<link>http://voxcharta.org/2012/05/13/the-connection-between-radio-and-gamma-ray-emission-in-fermilat-blazars/</link>
		<comments>http://voxcharta.org/2012/05/13/the-connection-between-radio-and-gamma-ray-emission-in-fermilat-blazars/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:44:23 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bl lacertae objects]]></category>
		<category><![CDATA[emission region]]></category>
		<category><![CDATA[energy peak]]></category>
		<category><![CDATA[external radiation]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[gamma ray emission]]></category>
		<category><![CDATA[gamma ray energy]]></category>
		<category><![CDATA[loudness]]></category>
		<category><![CDATA[negative correlation]]></category>
		<category><![CDATA[peak energy]]></category>
		<category><![CDATA[positive correlation]]></category>
		<category><![CDATA[radiation field]]></category>
		<category><![CDATA[radio gamma]]></category>
		<category><![CDATA[simultaneous data]]></category>
		<category><![CDATA[spectral energy distribution]]></category>
		<category><![CDATA[spectral index]]></category>
		<category><![CDATA[statistic analysis]]></category>
		<category><![CDATA[statistic results]]></category>
		<category><![CDATA[variability]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/the-connection-between-radio-and-gamma-ray-emission-in-fermilat-blazars/</guid>
		<description><![CDATA[We collect the 2LAC and MOJAVE quasi-simultaneous data to investigate the radio-gamma connection of blazars. The cross sample contains 166 sources. The statistic analysis based on this sample confirms positive correlations between these two bands, but the correlations become weaker as the gamma-ray energy increases. The statistic results between various parameters show negative correlations of [...]]]></description>
			<content:encoded><![CDATA[<p>We collect the 2LAC and MOJAVE quasi-simultaneous data to investigate the radio-gamma connection of blazars. The cross sample contains 166 sources. The statistic analysis based on this sample confirms positive correlations between these two bands, but the correlations become weaker as the gamma-ray energy increases. The statistic results between various parameters show negative correlations of gamma-ray photon spectral index with gamma-ray loudness for both FSRQs and BL Lacertae objects, positive correlations of gamma-ray variability index with the gamma-ray loudness for FSRQs, a negative correlation of the gamma-ray variability index with the gamma-ray photon spectral index for FSRQs, and negative correlations of gamma-ray photon spectral index with gamma-ray luminosity for FSRQs. These results suggest that the gamma-ray variability may be due to changes inside the gamma-ray emission region like the injected power, rather than changes in the photon density of the external radiation fields, and the variability amplitude tends to be larger as the gamma-rays are closer to the high energy peak of spectral energy distribution. No correlation of variability index found for BL Lacertae objects implies that variability behavior may differ below and above the peak energy.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/the-connection-between-radio-and-gamma-ray-emission-in-fermilat-blazars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<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>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>
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		<item>
		<title>Neutron star as laboratories for Cosmology</title>
		<link>http://voxcharta.org/2012/05/13/neutron-star-as-laboratories-for-cosmology/</link>
		<comments>http://voxcharta.org/2012/05/13/neutron-star-as-laboratories-for-cosmology/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:38:11 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[annihilation]]></category>
		<category><![CDATA[bbn]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[cosmology]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[deviations]]></category>
		<category><![CDATA[galactic halo]]></category>
		<category><![CDATA[gravitational potential]]></category>
		<category><![CDATA[low density]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[test bench]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/neutron-star-as-laboratories-for-cosmology/</guid>
		<description><![CDATA[Neutron stars can be considered a useful and interesting laboratory for Cosmology. With their deep gravitational potential they may accrete dark matter from the galactic halo and subsequent self-annihilation processes could induce an indirect observable signal this type of matter. In addition, the large densities in the interior of these objects may constitute a test-bench [...]]]></description>
			<content:encoded><![CDATA[<p>Neutron stars can be considered a useful and interesting laboratory for Cosmology. With their deep gravitational potential they may accrete dark matter from the galactic halo and subsequent self-annihilation processes could induce an indirect observable signal this type of matter. In addition, the large densities in the interior of these objects may constitute a test-bench to study hypothesized deviations of fundamental constant values complementary to existing works using constraints at low density from BBN.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/neutron-star-as-laboratories-for-cosmology/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>130 GeV dark matter and the Fermi gamma-ray line [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/13/130-gev-dark-matter-and-the-fermi-gamma-ray-line-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/13/130-gev-dark-matter-and-the-fermi-gamma-ray-line-cross-listing/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:37:18 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[center of the galaxy]]></category>
		<category><![CDATA[coupling]]></category>
		<category><![CDATA[cross section]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[doublet]]></category>
		<category><![CDATA[gamma gamma]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[hadronic jets]]></category>
		<category><![CDATA[higgs boson]]></category>
		<category><![CDATA[Lambda]]></category>
		<category><![CDATA[nucleon]]></category>
		<category><![CDATA[particle physics]]></category>
		<category><![CDATA[photon]]></category>
		<category><![CDATA[physics model]]></category>
		<category><![CDATA[pion]]></category>
		<category><![CDATA[qcd]]></category>
		<category><![CDATA[relic density]]></category>
		<category><![CDATA[section 24]]></category>
		<category><![CDATA[standard model]]></category>
		<category><![CDATA[tentative evidence]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/130-gev-dark-matter-and-the-fermi-gamma-ray-line-cross-listing/</guid>
		<description><![CDATA[Based on tentative evidence for a peak in the Fermi gamma-ray spectrum originating from near the center of the galaxy, it has been suggested that dark matter of mass ~130 GeV is annihilating directly into photons with a cross section ~24 times smaller than that needed for the thermal relic density. We propose a simple [...]]]></description>
			<content:encoded><![CDATA[<p>Based on tentative evidence for a peak in the Fermi gamma-ray spectrum originating from near the center of the galaxy, it has been suggested that dark matter of mass ~130 GeV is annihilating directly into photons with a cross section ~24 times smaller than that needed for the thermal relic density. We propose a simple particle physics model in which the DM is a scalar X, with a coupling lambda_X X^2 |S|^2 to a scalar multiplet S containing a charged component, which allows for XX -&gt; gamma gamma at one loop due to the virtual S^+. We predict a second monochromatic photon peak at 114 GeV due to XX -&gt; gamma Z. The S should be a doublet under SU(2) to satisfy precision electroweak constraints, and colored under a hidden sector SU(N) or QCD to confine the charged relic S^+. We need lambda_X ~ 3 and m_S ~ m_X to get a large enough XX -&gt; gamma Z cross section. The analogous coupling lambda_h h^2 |S|^2 to the Higgs boson can naturally increase the partial width for h -&gt; gamma gamma by an amount comparable to its standard model value, as suggested by recent measurements from CMS. Due to the hidden sector SU(N) (or QCD), S binds to its antiparticle to form S-pions, which will be pair-produced in colliders and then decay predominantly to XX, hh (or hadronic jets) and subdominantly to gamma gamma. The cross section for X on nucleons is in marginal conflict with the Xenon100 upper limit, suggesting that it should be discovered soon by direct detection.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/130-gev-dark-matter-and-the-fermi-gamma-ray-line-cross-listing/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>GRB 100418A: a Long GRB without a Bright Supernova in a High-Metallicity Host Galaxy [Replacement]</title>
		<link>http://voxcharta.org/2012/05/13/grb-100418a-a-long-grb-without-a-bright-supernova-in-a-high-metallicity-host-galaxy-replacement/</link>
		<comments>http://voxcharta.org/2012/05/13/grb-100418a-a-long-grb-without-a-bright-supernova-in-a-high-metallicity-host-galaxy-replacement/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:34:18 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absolute magnitude]]></category>
		<category><![CDATA[afterglow]]></category>
		<category><![CDATA[bright supernova]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[focas]]></category>
		<category><![CDATA[galaxy image]]></category>
		<category><![CDATA[galaxy properties]]></category>
		<category><![CDATA[gcn circulars]]></category>
		<category><![CDATA[host galaxy]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[m star]]></category>
		<category><![CDATA[massive log]]></category>
		<category><![CDATA[metallicity]]></category>
		<category><![CDATA[noise spectrum]]></category>
		<category><![CDATA[point source]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[spectrophotometric observations]]></category>
		<category><![CDATA[supernova sn]]></category>
		<category><![CDATA[time variation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/grb-100418a-a-long-grb-without-a-bright-supernova-in-a-high-metallicity-host-galaxy-replacement/</guid>
		<description><![CDATA[We present results of a search for a supernova (SN) component associated with GRB 100418A at the redshift of 0.624. The field of GRB 100418A was observed with FOCAS on Subaru 8.2m telescope under a photometric condition (seeing 0.3&#8243;-0.4&#8243;) on 2010 May 14 (UT). The date corresponds to 25.6 days after the burst trigger (15.8 [...]]]></description>
			<content:encoded><![CDATA[<p>We present results of a search for a supernova (SN) component associated with GRB 100418A at the redshift of 0.624. The field of GRB 100418A was observed with FOCAS on Subaru 8.2m telescope under a photometric condition (seeing 0.3&#8243;-0.4&#8243;) on 2010 May 14 (UT). The date corresponds to 25.6 days after the burst trigger (15.8 days in the restframe). We did imaging observations in V, Rc, and Ic bands, and two hours of spectrophotometric observations. We got the resolved host galaxy image which elongated 1.6&#8243; (= 11 kpc) from north to south. No point source was detected on the host galaxy. The time variation of Rc-band magnitude shows that the afterglow of GRB 100418A has faded to Rc \sim &gt; 24 without SN like rebrightening, when we compare our measurement to the reports in GCN circulars. We could not identify any SN feature such as broad emission-lines or bumps in our spectrum. Assuming the SN is fainter than the 3{\sigma} noise spectrum of our observation, we estimate the upper limit on the SN absolute magnitude MIc,obs &gt; -17.2 in observer frame Ic-band. This magnitude is comparable to the faintest type Ic SNe. We also estimate host galaxy properties from the spectrum. The host galaxy of GRB 100418A is relatively massive (log M_{star}/M_{sun} = 9.54) compared to typical long GRB host galaxies, and has 12+log(O/H) = 8.75.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/grb-100418a-a-long-grb-without-a-bright-supernova-in-a-high-metallicity-host-galaxy-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Gravitational waves and gamma-ray bursts [Replacement]</title>
		<link>http://voxcharta.org/2012/05/13/gravitational-waves-and-gamma-ray-bursts-replacement/</link>
		<comments>http://voxcharta.org/2012/05/13/gravitational-waves-and-gamma-ray-bursts-replacement/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:33:40 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absence]]></category>
		<category><![CDATA[central source]]></category>
		<category><![CDATA[energy release]]></category>
		<category><![CDATA[gamma ray burst]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[mass objects]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[multi messenger]]></category>
		<category><![CDATA[progenitor]]></category>
		<category><![CDATA[stellar mass]]></category>
		<category><![CDATA[wave observations]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/gravitational-waves-and-gamma-ray-bursts-replacement/</guid>
		<description><![CDATA[Gamma-Ray Bursts are likely associated with a catastrophic energy release in stellar mass objects. Electromagnetic observations provide important, but indirect information on the progenitor. On the other hand, gravitational waves emitted from the central source, carry direct information on its nature. In this context, I give an overview of the multi-messenger study of gamma-ray bursts [...]]]></description>
			<content:encoded><![CDATA[<p>Gamma-Ray Bursts are likely associated with a catastrophic energy release in stellar mass objects. Electromagnetic observations provide important, but indirect information on the progenitor. On the other hand, gravitational waves emitted from the central source, carry direct information on its nature. In this context, I give an overview of the multi-messenger study of gamma-ray bursts that can be carried out by using electromagnetic and gravitational wave observations. I also underline the importance of joint electromagnetic and gravitational wave searches, in the absence of a gamma-ray trigger. Finally, I discuss how multi-messenger observations may probe alternative gamma-ray burst progenitor models, such as the magnetar scenario.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/gravitational-waves-and-gamma-ray-bursts-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>GUT and Supersymmetry at the LHC and in dark matter [Replacement]</title>
		<link>http://voxcharta.org/2012/05/13/gut-and-supersymmetry-at-the-lhc-and-in-dark-matter-replacement/</link>
		<comments>http://voxcharta.org/2012/05/13/gut-and-supersymmetry-at-the-lhc-and-in-dark-matter-replacement/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:32:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[boson mass]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[doublet]]></category>
		<category><![CDATA[electroweak symmetry]]></category>
		<category><![CDATA[energy physics]]></category>
		<category><![CDATA[focal surface]]></category>
		<category><![CDATA[grand unification]]></category>
		<category><![CDATA[hierarchy problem]]></category>
		<category><![CDATA[higgs field]]></category>
		<category><![CDATA[lhc]]></category>
		<category><![CDATA[low energy]]></category>
		<category><![CDATA[natural solution]]></category>
		<category><![CDATA[parameter space]]></category>
		<category><![CDATA[representations]]></category>
		<category><![CDATA[scale model]]></category>
		<category><![CDATA[supersymmetry]]></category>
		<category><![CDATA[triplet]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/gut-and-supersymmetry-at-the-lhc-and-in-dark-matter-replacement/</guid>
		<description><![CDATA[Conventional SO(10) models involve more than one scale for a complete breaking of the GUT symmetry requiring further assumptions on the VEVs of the Higgs fields that enter in the breaking to achieve viable models. Recent works where the breaking can be accomplished at one scale are discussed. These include models with just a pair [...]]]></description>
			<content:encoded><![CDATA[<p>Conventional SO(10) models involve more than one scale for a complete breaking of the GUT symmetry requiring further assumptions on the VEVs of the Higgs fields that enter in the breaking to achieve viable models. Recent works where the breaking can be accomplished at one scale are discussed. These include models with just a pair of $144+\bar{144}$ of Higgs fields. Further extensions of this idea utilizing $560+ \bar{560}$ of Higgs representations allow both the breaking at one scale, as well as accomplish a natural doublet-triplet splitting via the missing partner mechanism. More generally, we discuss the connection of high scale models to low energy physics in the context of supergravity grand unification. Here we discuss a natural solution to the little hierarchy problem and also discuss the implications of the LHC data for supersymmetry. It is shown that the LHC data implies that most of the parameter space of supergravity models consistent with the data lie on the Hyperbolic Branch of radiative breaking of the electroweak symmetry and more specifically on the Focal Surface of the Hyperbolic Branch. A discussion is also given of the implications of recent LHC data on the Higgs boson mass for the discovery of supersymmetry and for the search for dark matter.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/gut-and-supersymmetry-at-the-lhc-and-in-dark-matter-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Revised production cross-section of gamma-rays in p-p collisions with LHC data for the study of TeV gamma-ray astronomy [Replacement]</title>
		<link>http://voxcharta.org/2012/05/13/revised-production-cross-section-of-gamma-rays-in-p-p-collisions-with-lhc-data-for-the-study-of-tev-gamma-ray-astronomy-replacement/</link>
		<comments>http://voxcharta.org/2012/05/13/revised-production-cross-section-of-gamma-rays-in-p-p-collisions-with-lhc-data-for-the-study-of-tev-gamma-ray-astronomy-replacement/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:32:12 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accelerator]]></category>
		<category><![CDATA[center of mass]]></category>
		<category><![CDATA[cms]]></category>
		<category><![CDATA[collisions]]></category>
		<category><![CDATA[cross section]]></category>
		<category><![CDATA[empirical formula]]></category>
		<category><![CDATA[energy range]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[gamma ray astronomy]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[hadron]]></category>
		<category><![CDATA[mass system]]></category>
		<category><![CDATA[mev]]></category>
		<category><![CDATA[pev]]></category>
		<category><![CDATA[projectile]]></category>
		<category><![CDATA[proton]]></category>
		<category><![CDATA[rapidity]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[totem]]></category>
		<category><![CDATA[transverse momentum]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/revised-production-cross-section-of-gamma-rays-in-p-p-collisions-with-lhc-data-for-the-study-of-tev-gamma-ray-astronomy-replacement/</guid>
		<description><![CDATA[We present the production cross-section of gamma-rays based on data of p-p collisions at LHC, revising the previous semi-empirical formula mainly for 1) the inelastic cross-section in p-p collisions, $\sigma_{pp}(E_0)$, and 2) the inclusive gamma-ray spectrum in the forward region, $\sigma_{pp \rightarrow \gamma}(E_0, E_\gamma)$. We find that the previous cross-section gives a significantly softer spectrum [...]]]></description>
			<content:encoded><![CDATA[<p>We present the production cross-section of gamma-rays based on data of p-p collisions at LHC, revising the previous semi-empirical formula mainly for 1) the inelastic cross-section in p-p collisions, $\sigma_{pp}(E_0)$, and 2) the inclusive gamma-ray spectrum in the forward region, $\sigma_{pp \rightarrow \gamma}(E_0, E_\gamma)$. We find that the previous cross-section gives a significantly softer spectrum than found in the data of LHC. In this paper, we focus our interest mainly upon the LHC forward (LHCf) experiment, giving gamma-ray spectra in the very forward region with the pseudo-rapidity $\eta^*$ &gt; 8.8 in the center of mass system (CMS), which have not been reported so far. We also give the pseudo-rapidity distribution of charged hadrons with -3 &lt; $\eta^*$ &lt; 3 obtained by ALICE and TOTEM experiments, both with LHC. We find that the revised cross-section reproduces quite well the accelerator data over the wide energy range from GeV to 30 PeV for projectile protons, corresponding approximately to 100 MeV to 3 PeV for secondary gamma-rays. The production cross-section of gamma-rays produced in the forward region is essential for the study of gamma-ray astronomy, while not important are those produced in the central region in CMS, and of much less importance in the backward. We discuss also the average transverse momentum of gamma-rays, $\bar{p}_{t}$, and the average inelasticity transferred to gamma-rays, $\bar{k}_\gamma^*$, obtaining that the former increases very slowly with $\bar{p}_{t}$ = 100 &#8211; 220 MeV/c for $E_0$ = 1 GeV &#8211; 26 PeV, and the latter is almost independent of $E_0$, with $\bar{k}_\gamma^* \approx 1/6$, while we can not exclude the possibility of a small increase of $\bar{k}_\gamma^*$.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/revised-production-cross-section-of-gamma-rays-in-p-p-collisions-with-lhc-data-for-the-study-of-tev-gamma-ray-astronomy-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Modelling the light curves of PSR B1259-63/LS 2883-II.The effects of anisotropic pulsar wind and Doppler-boosting [Replacement]</title>
		<link>http://voxcharta.org/2012/05/13/modelling-the-light-curves-of-psr-b1259-63ls-2883-ii-the-effects-of-anisotropic-pulsar-wind-and-doppler-boosting-replacement/</link>
		<comments>http://voxcharta.org/2012/05/13/modelling-the-light-curves-of-psr-b1259-63ls-2883-ii-the-effects-of-anisotropic-pulsar-wind-and-doppler-boosting-replacement/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:31:59 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[anisotropy]]></category>
		<category><![CDATA[binary system]]></category>
		<category><![CDATA[bow shock]]></category>
		<category><![CDATA[doppler]]></category>
		<category><![CDATA[eccentric orbit]]></category>
		<category><![CDATA[energy flux]]></category>
		<category><![CDATA[flare]]></category>
		<category><![CDATA[gamma ray observatory]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[orbital period]]></category>
		<category><![CDATA[orbital phase]]></category>
		<category><![CDATA[peak light]]></category>
		<category><![CDATA[photon]]></category>
		<category><![CDATA[psr b1259]]></category>
		<category><![CDATA[termination shock]]></category>
		<category><![CDATA[two peak]]></category>
		<category><![CDATA[wind model]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/modelling-the-light-curves-of-psr-b1259-63ls-2883-ii-the-effects-of-anisotropic-pulsar-wind-and-doppler-boosting-replacement/</guid>
		<description><![CDATA[PSR B1259-63/LS 2883 is a binary system in which a 48-ms pulsar orbits around a Be star in a high eccentric orbit with a long orbital period of about 3.4 yr. It is special for having asymmetric two-peak profiles in both the X-ray and the TeV light curves. Recently, an unexpected GeV flare was detected [...]]]></description>
			<content:encoded><![CDATA[<p>PSR B1259-63/LS 2883 is a binary system in which a 48-ms pulsar orbits around a Be star in a high eccentric orbit with a long orbital period of about 3.4 yr. It is special for having asymmetric two-peak profiles in both the X-ray and the TeV light curves. Recently, an unexpected GeV flare was detected by $Fermi$ gamma-ray observatory several weeks after the last periastron passage. In this paper, we show that this observed GeV flare could be produced by the Doppler-boosted synchrotron emission in the bow shock tail. An anisotropic pulsar wind model, which mainly affects the energy flux injection to the termination shock in different orbital phase, is also used in this paper, and we find that the anisotropy in the pulsar wind can play a significant role in producing the asymmetric two-peak profiles in both X-ray and TeV light curves. The X-ray and TeV photons before periastron are mainly produced by the shocked electrons around the shock apex and the light curves after periastron are contributed by the emission from the shock apex and the shock tail together, which result in the asymmetric two-peak light curves.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/modelling-the-light-curves-of-psr-b1259-63ls-2883-ii-the-effects-of-anisotropic-pulsar-wind-and-doppler-boosting-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>GRB 091208B: First Detection of the Optical Polarization in Early Forward Shock Emission of a Gamma-Ray Burst Afterglow [Replacement]</title>
		<link>http://voxcharta.org/2012/05/13/grb-091208b-first-detection-of-the-optical-polarization-in-early-forward-shock-emission-of-a-gamma-ray-burst-afterglow-replacement/</link>
		<comments>http://voxcharta.org/2012/05/13/grb-091208b-first-detection-of-the-optical-polarization-in-early-forward-shock-emission-of-a-gamma-ray-burst-afterglow-replacement/#comments</comments>
		<pubDate>Mon, 14 May 2012 00:31:47 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[angle]]></category>
		<category><![CDATA[decay]]></category>
		<category><![CDATA[emission region]]></category>
		<category><![CDATA[forward shock]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[optical light curve]]></category>
		<category><![CDATA[plasma]]></category>
		<category><![CDATA[polarization]]></category>
		<category><![CDATA[skin depth]]></category>
		<category><![CDATA[temporal change]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/13/grb-091208b-first-detection-of-the-optical-polarization-in-early-forward-shock-emission-of-a-gamma-ray-burst-afterglow-replacement/</guid>
		<description><![CDATA[We report that the optical polarization in the afterglow of GRB 091208B is measured at t = 149 &#8211; 706 s after the burst trigger, and the polarization degree is P = 10.4% +/- 2.5%. The optical light curve at this time shows a power-law decay with index -0.75 +/- 0.02, which is interpreted as [...]]]></description>
			<content:encoded><![CDATA[<p>We report that the optical polarization in the afterglow of GRB 091208B is measured at t = 149 &#8211; 706 s after the burst trigger, and the polarization degree is P = 10.4% +/- 2.5%. The optical light curve at this time shows a power-law decay with index -0.75 +/- 0.02, which is interpreted as the forward shock synchrotron emission, and thus this is the first detection of the early-time optical polarization in the forward shock (rather than that in the reverse shock reported by Steele et al. (2009). This detection disfavors the afterglow model in which the magnetic fields in the emission region are random on the plasma skin depth scales, such as amplified by the plasma instabilities, e.g., Weibel instability. We suggest that the fields are amplified by the magnetohydrodynamic instabilities, which would be tested by future observations of the temporal changes of the polarization degrees and angles for other bursts.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/13/grb-091208b-first-detection-of-the-optical-polarization-in-early-forward-shock-emission-of-a-gamma-ray-burst-afterglow-replacement/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>Revised production cross-section of gamma-rays in p-p collisions with LHC data for the study of TeV gamma-ray astronomy</title>
		<link>http://voxcharta.org/2012/05/10/revised-production-cross-section-of-gamma-rays-in-p-p-collisions-with-lhc-data-for-the-study-of-tev-gamma-ray-astronomy/</link>
		<comments>http://voxcharta.org/2012/05/10/revised-production-cross-section-of-gamma-rays-in-p-p-collisions-with-lhc-data-for-the-study-of-tev-gamma-ray-astronomy/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:44:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accelerator]]></category>
		<category><![CDATA[center of mass]]></category>
		<category><![CDATA[cms]]></category>
		<category><![CDATA[collisions]]></category>
		<category><![CDATA[cross section]]></category>
		<category><![CDATA[empirical formula]]></category>
		<category><![CDATA[energy range]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[gamma ray astronomy]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[hadron]]></category>
		<category><![CDATA[mass system]]></category>
		<category><![CDATA[mev]]></category>
		<category><![CDATA[pev]]></category>
		<category><![CDATA[projectile]]></category>
		<category><![CDATA[proton]]></category>
		<category><![CDATA[rapidity]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[totem]]></category>
		<category><![CDATA[transverse momentum]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/revised-production-cross-section-of-gamma-rays-in-p-p-collisions-with-lhc-data-for-the-study-of-tev-gamma-ray-astronomy/</guid>
		<description><![CDATA[We present the production cross-section of gamma-rays based on data of p-p collisions at LHC, revising the previous semi-empirical formula mainly for 1) the inelastic cross-section in p-p collisions, $\sigma_{\scriptsize {pp}}(E_0)$, and 2) the inclusive $\gamma$-ray spectrum in the forward region, $\sigma_{pp \rightarrow \gamma}(E_0, E_\gamma)$. We find that the previous cross-section gives a significantly softer [...]]]></description>
			<content:encoded><![CDATA[<p>We present the production cross-section of gamma-rays based on data of p-p collisions at LHC, revising the previous semi-empirical formula mainly for 1) the inelastic cross-section in p-p collisions, $\sigma_{\scriptsize {pp}}(E_0)$, and 2) the inclusive $\gamma$-ray spectrum in the forward region, $\sigma_{pp \rightarrow \gamma}(E_0, E_\gamma)$. We find that the previous cross-section gives a significantly softer spectrum than found in the data of LHC. In this paper, we focus our interest mainly upon the LHC forward (LHCf) experiment, giving gamma-ray spectra in the very forward region with the pseudo-rapidity $\eta^*$\,$\gsim$\,8.8 in the center of mass system (CMS), which have not been reported so far. We also give the pseudo-rapidity distribution of charged hadrons with $-3 \le \eta^* \le 3$ obtained by ALICE and TOTEM experiments, both with LHC. We find that the revised cross-section reproduces quite well the accelerator data over the wide energy range from GeV to 30 PeV for projectile protons, corresponding approximately to 100 MeV to 3 PeV for secondary gamma-rays. The production cross-section of gamma-rays produced in the forward region is essential for the study of gamma-ray astronomy, while not important are those produced in the central region in CMS, and of much less importance in the backward. We discuss also the average transverse momentum of gamma-rays, $\bar{p}_{t}$, and the average inelasticity transferred to gamma-rays, $\bar{k}_\gamma^*$, obtaining that the former increases very slowly with $\bar{p}_{t} = 100 \sim 220$\,MeV/c for $E_0 = 1\,{GeV} \sim 26\,{PeV}$, and the latter is almost independent of $E_0$, with $\bar{k}_\gamma^* \approx 1/6,$ while we can not exclude the possibility of a small increase of $\bar{k}_\gamma^*$.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/revised-production-cross-section-of-gamma-rays-in-p-p-collisions-with-lhc-data-for-the-study-of-tev-gamma-ray-astronomy/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Modelling the light curves of PSR B1259-63/LS 2883</title>
		<link>http://voxcharta.org/2012/05/10/modelling-the-light-curves-of-psr-b1259-63ls-2883/</link>
		<comments>http://voxcharta.org/2012/05/10/modelling-the-light-curves-of-psr-b1259-63ls-2883/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:43:44 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[anisotropic]]></category>
		<category><![CDATA[anisotropy]]></category>
		<category><![CDATA[binary system]]></category>
		<category><![CDATA[bow shock]]></category>
		<category><![CDATA[eccentric orbit]]></category>
		<category><![CDATA[energy flux]]></category>
		<category><![CDATA[flare]]></category>
		<category><![CDATA[gamma ray observatory]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[orbital period]]></category>
		<category><![CDATA[orbital phase]]></category>
		<category><![CDATA[peak light]]></category>
		<category><![CDATA[photon]]></category>
		<category><![CDATA[psr b1259]]></category>
		<category><![CDATA[termination shock]]></category>
		<category><![CDATA[two peak]]></category>
		<category><![CDATA[wind model]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/modelling-the-light-curves-of-psr-b1259-63ls-2883/</guid>
		<description><![CDATA[PSR B1259-63/LS 2883 is a binary system in which a 48-ms pulsar orbits around a Be star in a high eccentric orbit with a long orbital period of about 3.4 yr. It is special for having asymmetric two-peak profiles in both the X-ray and the TeV light curves. Recently, an unexpected GeV flare was detected [...]]]></description>
			<content:encoded><![CDATA[<p>PSR B1259-63/LS 2883 is a binary system in which a 48-ms pulsar orbits around a Be star in a high eccentric orbit with a long orbital period of about 3.4 yr. It is special for having asymmetric two-peak profiles in both the X-ray and the TeV light curves. Recently, an unexpected GeV flare was detected by $Fermi$ gamma-ray observatory several weeks after the last periastron passage. In this paper, we show that this observed GeV flare could be produced by the Doppler-boosted synchrotron emission in the bow shock tail. An anisotropic pulsar wind model, which mainly affects the energy flux injection to the termination shock in different orbital phase, is also used in this paper, and we find that the anisotropy in the pulsar wind can play a significant role in producing the asymmetric two-peak profiles in both X-ray and TeV light curves. The X-ray and TeV photons before periastron are mainly produced by the shocked electrons around the shock apex and the light curves after periastron are contributed by the emission from the shock apex and the shock tail together, which result in the asymmetric two-peak light curves.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/modelling-the-light-curves-of-psr-b1259-63ls-2883/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Early Optical Polarization of Forward Shock Afterglow of GRB 091208B</title>
		<link>http://voxcharta.org/2012/05/10/early-optical-polarization-of-forward-shock-afterglow-of-grb-091208b/</link>
		<comments>http://voxcharta.org/2012/05/10/early-optical-polarization-of-forward-shock-afterglow-of-grb-091208b/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:43:24 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[afterglow]]></category>
		<category><![CDATA[angle]]></category>
		<category><![CDATA[burst]]></category>
		<category><![CDATA[decay]]></category>
		<category><![CDATA[emission region]]></category>
		<category><![CDATA[forward shock]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[optical light curve]]></category>
		<category><![CDATA[plasma]]></category>
		<category><![CDATA[polarization]]></category>
		<category><![CDATA[skin depth]]></category>
		<category><![CDATA[temporal change]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/early-optical-polarization-of-forward-shock-afterglow-of-grb-091208b/</guid>
		<description><![CDATA[We report that the optical polarization in the afterglow of GRB 091208B is measured at t = 149 &#8211; 706 s after the burst trigger, and the polarization degree is P = 10.4% +/- 2.5%. The optical light curve at this time shows a power-law decay with index -0.75 +/- 0.02, which is interpreted as [...]]]></description>
			<content:encoded><![CDATA[<p>We report that the optical polarization in the afterglow of GRB 091208B is measured at t = 149 &#8211; 706 s after the burst trigger, and the polarization degree is P = 10.4% +/- 2.5%. The optical light curve at this time shows a power-law decay with index -0.75 +/- 0.02, which is interpreted as the forward shock synchrotron emission, and thus this is the first detection of the early-time optical polarization in the forward shock (rather than that in the reverse shock reported by Steele et al. (2009). This detection disfavors the afterglow model in which the magnetic fields in the emission region are random on the plasma skin depth scales, such as amplified by the plasma instabilities, e.g., Weibel instability. We suggest that the fields are amplified by the magnetohydrodynamic instabilities, which would be tested by future observations of the temporal changes of the polarization degrees and angles for other bursts.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/early-optical-polarization-of-forward-shock-afterglow-of-grb-091208b/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Short-Term Variability of PKS1510-089</title>
		<link>http://voxcharta.org/2012/05/10/short-term-variability-of-pks1510-089/</link>
		<comments>http://voxcharta.org/2012/05/10/short-term-variability-of-pks1510-089/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:43:14 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[agns]]></category>
		<category><![CDATA[doppler]]></category>
		<category><![CDATA[galactic nucleus]]></category>
		<category><![CDATA[intrinsic variability]]></category>
		<category><![CDATA[term radio]]></category>
		<category><![CDATA[term variability]]></category>
		<category><![CDATA[time scale]]></category>
		<category><![CDATA[variation]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/short-term-variability-of-pks1510-089/</guid>
		<description><![CDATA[We searched a short-term radio variability in an active galactic nucleus PKS 1510-089. A daily flux monitoring for 143 days at 8.4 GHz was performed, and VLBI observations at 8.4, 22, and 43 GHz were carried out 4 times during the flux monitoring period. As a result, variability with time scale of 20 to 30 [...]]]></description>
			<content:encoded><![CDATA[<p>We searched a short-term radio variability in an active galactic nucleus PKS 1510-089. A daily flux monitoring for 143 days at 8.4 GHz was performed, and VLBI observations at 8.4, 22, and 43 GHz were carried out 4 times during the flux monitoring period. As a result, variability with time scale of 20 to 30 days was detected. The variation patterns were well alike on three frequencies, moreover those at 22 and 43 GHz were synchronized. These properties support that this short-term variability is an intrinsic one. The Doppler factor estimated from the variability time scale is 47. Since the Doppler factor is not extraordinary large for AGN, such intrinsic variability with time scale less than 30 days would exist in other AGNs.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/short-term-variability-of-pks1510-089/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>First results from the ANTARES neutrino telescope</title>
		<link>http://voxcharta.org/2012/05/10/first-results-from-the-antares-neutrino-telescope/</link>
		<comments>http://voxcharta.org/2012/05/10/first-results-from-the-antares-neutrino-telescope/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:42:15 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[4 months]]></category>
		<category><![CDATA[antares]]></category>
		<category><![CDATA[atmospheric neutrino flux]]></category>
		<category><![CDATA[blazar]]></category>
		<category><![CDATA[construction phase]]></category>
		<category><![CDATA[deep sea]]></category>
		<category><![CDATA[energy events]]></category>
		<category><![CDATA[energy range]]></category>
		<category><![CDATA[excesses]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[mediterranean sea]]></category>
		<category><![CDATA[muon flux]]></category>
		<category><![CDATA[neutrino]]></category>
		<category><![CDATA[neutrino signal]]></category>
		<category><![CDATA[neutrino telescope]]></category>
		<category><![CDATA[particle detector]]></category>
		<category><![CDATA[sky distribution]]></category>
		<category><![CDATA[southern sky]]></category>
		<category><![CDATA[TeV]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/first-results-from-the-antares-neutrino-telescope/</guid>
		<description><![CDATA[The ANTARES detector is the most sensitive neutrino telescope observing the southern sky and the world&#8217;s first particle detector operating in the deep sea. It is installed in the Mediterranean Sea at a depth of 2475 m. As an example of early results, the determination of the atmospheric muon flux is discussed and a good [...]]]></description>
			<content:encoded><![CDATA[<p>The ANTARES detector is the most sensitive neutrino telescope observing the southern sky and the world&#8217;s first particle detector operating in the deep sea. It is installed in the Mediterranean Sea at a depth of 2475 m. As an example of early results, the determination of the atmospheric muon flux is discussed and a good agreement with previous measurements is found. Furthermore, the results of a search for high-energy events in excess of the atmospheric neutrino flux are reported and significant limits are set on the diffuse cosmic neutrino flux in the multi-TeV to PeV energy range. Using data from more than 800 days of effective data taking, partly during the construction phase, a first analysis searching for point-like excesses in the neutrino sky distribution has been performed. The resulting sensitivity of ANTARES is reported and compared to measurements of other detectors. A method employed for a first search for neutrinos from Fermi-detected gamma-ray flaring blazars in the last 4 months of 2008 is described and the results are reported. No significant neutrino signal in excess of that expected from atmospheric background has been found.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/first-results-from-the-antares-neutrino-telescope/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Particle acceleration in relativistic outflows</title>
		<link>http://voxcharta.org/2012/05/10/particle-acceleration-in-relativistic-outflows/</link>
		<comments>http://voxcharta.org/2012/05/10/particle-acceleration-in-relativistic-outflows/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:41:14 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[observational result]]></category>
		<category><![CDATA[particle acceleration]]></category>
		<category><![CDATA[relativistic outflows]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/particle-acceleration-in-relativistic-outflows/</guid>
		<description><![CDATA[In this review we confront the current theoretical understanding of particle acceleration at relativistic outflows with recent observational results on various source classes thought to involve such outflows, e.g. gamma-ray bursts, active galactic nuclei, and pulsar wind nebulae. We highlight the possible contributions of these sources to ultra-high-energy cosmic rays.
]]></description>
			<content:encoded><![CDATA[<p>In this review we confront the current theoretical understanding of particle acceleration at relativistic outflows with recent observational results on various source classes thought to involve such outflows, e.g. gamma-ray bursts, active galactic nuclei, and pulsar wind nebulae. We highlight the possible contributions of these sources to ultra-high-energy cosmic rays.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/particle-acceleration-in-relativistic-outflows/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Search for gravitational waves associated with gamma-ray bursts during LIGO science run 6 and Virgo science runs 2 and 3</title>
		<link>http://voxcharta.org/2012/05/10/search-for-gravitational-waves-associated-with-gamma-ray-bursts-during-ligo-science-run-6-and-virgo-science-runs-2-and-3/</link>
		<comments>http://voxcharta.org/2012/05/10/search-for-gravitational-waves-associated-with-gamma-ray-bursts-during-ligo-science-run-6-and-virgo-science-runs-2-and-3/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:40:33 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[coincidence]]></category>
		<category><![CDATA[counterpart]]></category>
		<category><![CDATA[distance]]></category>
		<category><![CDATA[exclusions]]></category>
		<category><![CDATA[gamma ray burst]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[GRB]]></category>
		<category><![CDATA[grbs]]></category>
		<category><![CDATA[median value]]></category>
		<category><![CDATA[mpc]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[priors]]></category>
		<category><![CDATA[progenitor]]></category>
		<category><![CDATA[satellite observations]]></category>
		<category><![CDATA[source parameters]]></category>
		<category><![CDATA[virgo]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/search-for-gravitational-waves-associated-with-gamma-ray-bursts-during-ligo-science-run-6-and-virgo-science-runs-2-and-3/</guid>
		<description><![CDATA[We present the results of a search for gravitational waves associated with 154 gamma-ray bursts (GRBs) that were detected by satellite-based gamma-ray experiments in 2009-2010, during the sixth LIGO science run and the second and third Virgo science runs. We perform two distinct searches: a modeled search for coalescences of either two neutron stars or [...]]]></description>
			<content:encoded><![CDATA[<p>We present the results of a search for gravitational waves associated with 154 gamma-ray bursts (GRBs) that were detected by satellite-based gamma-ray experiments in 2009-2010, during the sixth LIGO science run and the second and third Virgo science runs. We perform two distinct searches: a modeled search for coalescences of either two neutron stars or a neutron star and black hole; and a search for generic, unmodeled gravitational-wave bursts. We find no evidence for gravitational-wave counterparts, either with any individual GRB in this sample or with the population as a whole. For all GRBs we place lower bounds on the distance to the progenitor, under the optimistic assumption of a gravitational-wave emission energy of 10^-2 M c^2 at 150 Hz, with a median limit of 17 Mpc. For short hard GRBs we place exclusion distances on binary neutron star and neutron star-black hole progenitors, using astrophysically motivated priors on the source parameters, with median values of 16 Mpc and 28 Mpc respectively. These distance limits, while significantly larger than for a search that is not aided by GRB satellite observations, are not large enough to expect a coincidence with a GRB. However, projecting these exclusions to the sensitivities of Advanced LIGO and Virgo, which should begin operation in 2015, we find that the detection of gravitational waves associated with GRBs will become quite possible.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/search-for-gravitational-waves-associated-with-gamma-ray-bursts-during-ligo-science-run-6-and-virgo-science-runs-2-and-3/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<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>Flaring Activity from 0836+710 (4C +71.07): What Can We Learn With Limited Multiwavelength Coverage?</title>
		<link>http://voxcharta.org/2012/05/10/flaring-activity-from-0836710-4c-71-07-what-can-we-learn-with-limited-multiwavelength-coverage/</link>
		<comments>http://voxcharta.org/2012/05/10/flaring-activity-from-0836710-4c-71-07-what-can-we-learn-with-limited-multiwavelength-coverage/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:39:34 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[egret]]></category>
		<category><![CDATA[flare]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[high frequency]]></category>
		<category><![CDATA[quiescence]]></category>
		<category><![CDATA[radio emission]]></category>
		<category><![CDATA[radio observation]]></category>
		<category><![CDATA[spectrum radio]]></category>
		<category><![CDATA[variability]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/flaring-activity-from-0836710-4c-71-07-what-can-we-learn-with-limited-multiwavelength-coverage/</guid>
		<description><![CDATA[After a long period of quiescence in \gamma-rays, blazar 0836+710 (4C +71.07) flared in the Spring of 2011. We found only limited multiwavelength coverage of the source. An indication of correlated optical / \gamma-ray variability is not surprising for a Flat Spectrum Radio Quasar (FSRQ) like this one. Radio observations at high frequencies, however, had [...]]]></description>
			<content:encoded><![CDATA[<p>After a long period of quiescence in \gamma-rays, blazar 0836+710 (4C +71.07) flared in the Spring of 2011. We found only limited multiwavelength coverage of the source. An indication of correlated optical / \gamma-ray variability is not surprising for a Flat Spectrum Radio Quasar (FSRQ) like this one. Radio observations at high frequencies, however, had seen a flare in 2010, well offset from possible \gamma-ray activity. The 2011 \gamma-ray activity comes during a period of rising radio emission, a pattern that has been seen since the EGRET era.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/flaring-activity-from-0836710-4c-71-07-what-can-we-learn-with-limited-multiwavelength-coverage/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Kinetic formation of DC magnetic field in unmagnetized Kelvin-Helmholtz instability [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/10/kinetic-formation-of-dc-magnetic-field-in-unmagnetized-kelvin-helmholtz-instability-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/10/kinetic-formation-of-dc-magnetic-field-in-unmagnetized-kelvin-helmholtz-instability-cross-listing/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:37:50 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[average temperature]]></category>
		<category><![CDATA[cell pic]]></category>
		<category><![CDATA[electron]]></category>
		<category><![CDATA[emergence]]></category>
		<category><![CDATA[field component]]></category>
		<category><![CDATA[fluid theory]]></category>
		<category><![CDATA[interface]]></category>
		<category><![CDATA[kelvin]]></category>
		<category><![CDATA[khi]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[pic simulations]]></category>
		<category><![CDATA[saturation level]]></category>
		<category><![CDATA[thermal expansion]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/kinetic-formation-of-dc-magnetic-field-in-unmagnetized-kelvin-helmholtz-instability-cross-listing/</guid>
		<description><![CDATA[Recent particle-in-cell (PIC) simulations of the Kelvin-Helmholtz instability have revealed the emergence of a strong and large-scale DC magnetic field component at the shear interface, which is not captured by the standard linear two-fluid theory. We show that the DC magnetic field results from electron mixing across the shear interface. The mixing mechanism can be [...]]]></description>
			<content:encoded><![CDATA[<p>Recent particle-in-cell (PIC) simulations of the Kelvin-Helmholtz instability have revealed the emergence of a strong and large-scale DC magnetic field component at the shear interface, which is not captured by the standard linear two-fluid theory. We show that the DC magnetic field results from electron mixing across the shear interface. The mixing mechanism can be modeled by a an electron thermal expansion across the shear, in a warm shear scenario, and we connect this picture to the cold shear scenario where the development of the standard cold fluid KHI produces an effective average temperature that drives the expansion. We outline a simple analytical model that describes the growth and saturation level of the DC magnetic field.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/kinetic-formation-of-dc-magnetic-field-in-unmagnetized-kelvin-helmholtz-instability-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Intra-night optical variability of core dominated radio quasars: the role of optical polarization</title>
		<link>http://voxcharta.org/2012/05/10/intra-night-optical-variability-of-core-dominated-radio-quasars-the-role-of-optical-polarization/</link>
		<comments>http://voxcharta.org/2012/05/10/intra-night-optical-variability-of-core-dominated-radio-quasars-the-role-of-optical-polarization/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:36:14 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[amplitude]]></category>
		<category><![CDATA[blazar]]></category>
		<category><![CDATA[dcs]]></category>
		<category><![CDATA[definitions]]></category>
		<category><![CDATA[duty cycle]]></category>
		<category><![CDATA[existence]]></category>
		<category><![CDATA[inov]]></category>
		<category><![CDATA[literature]]></category>
		<category><![CDATA[necessary condition]]></category>
		<category><![CDATA[optical emission lines]]></category>
		<category><![CDATA[optical flux]]></category>
		<category><![CDATA[optical variability]]></category>
		<category><![CDATA[polarization]]></category>
		<category><![CDATA[quasar]]></category>
		<category><![CDATA[radio core]]></category>
		<category><![CDATA[rapid variations]]></category>
		<category><![CDATA[spectrum radio]]></category>
		<category><![CDATA[sufficient condition]]></category>
		<category><![CDATA[telescopes]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/intra-night-optical-variability-of-core-dominated-radio-quasars-the-role-of-optical-polarization/</guid>
		<description><![CDATA[{Abridged} Rapid variations in optical flux are seen in many quasars and all blazars. The amount of variability in different classes of Active Galactic Nuclei has been studied extensively but many questions remain unanswered. We present the results of a long-term programme to investigate the intra-night optical variability (INOV) of powerful flat spectrum radio core-dominated [...]]]></description>
			<content:encoded><![CDATA[<p>{Abridged} Rapid variations in optical flux are seen in many quasars and all blazars. The amount of variability in different classes of Active Galactic Nuclei has been studied extensively but many questions remain unanswered. We present the results of a long-term programme to investigate the intra-night optical variability (INOV) of powerful flat spectrum radio core-dominated quasars (CDQs), with a focus on probing the relationship of INOV to the degree of optical polarization. We observed a sample of 16 bright CDQs showing strong broad optical emission lines and consisting of both high and low optical polarization quasars (HPCDQs and LPCDQs). We employed ARIES, IIA, IGO telescopes, to carry out {\it R}-band monitoring on a total of 47 nights. Combining these INOV data with those taken from the literature, we were able to increase the sample size to 21 CDQs(12 LPCDQs and 9 HPCDQs) monitored on a total of 73 nights. As the existence of a prominent flat-spectrum radio core signifies that strong relativistic beaming is present in all these CDQs, the definitions of the two sets differ primarily in fractional optical polarization, the LPCDQs showing a very low median$ P_{op} \simeq$ 0.4 per cent.   Our study yields an INOV duty cycle (DC) of $\sim$28 per cent for the LPCDQs and $\sim 68$ percent for HPCDQs.   If only strong INOV with fractional amplitude above 3 per cent is considered, the corresponding DCs are $\sim$ 7 per cent and $\sim$ 40 per cent, respectively.From this strong contrast between the two classes of luminous, relativistically beamed quasars, it is apparent that relativistic beaming is normally not a sufficient condition for strong INOV and a high optical polarization is the other necessary condition.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/intra-night-optical-variability-of-core-dominated-radio-quasars-the-role-of-optical-polarization/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Time-dependent simulations of emission from FSRQ PKS1510-089: multiwavelength variability of external Compton and SSC models</title>
		<link>http://voxcharta.org/2012/05/10/time-dependent-simulations-of-emission-from-fsrq-pks1510-089-multiwavelength-variability-of-external-compton-and-ssc-models/</link>
		<comments>http://voxcharta.org/2012/05/10/time-dependent-simulations-of-emission-from-fsrq-pks1510-089-multiwavelength-variability-of-external-compton-and-ssc-models/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:35:43 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[blr]]></category>
		<category><![CDATA[critical bands]]></category>
		<category><![CDATA[external radiation]]></category>
		<category><![CDATA[finite size]]></category>
		<category><![CDATA[gamma ray emission]]></category>
		<category><![CDATA[inverse compton]]></category>
		<category><![CDATA[light curves]]></category>
		<category><![CDATA[light travel time]]></category>
		<category><![CDATA[multi zone]]></category>
		<category><![CDATA[quality data]]></category>
		<category><![CDATA[realistic treatment]]></category>
		<category><![CDATA[relativistic electron]]></category>
		<category><![CDATA[seds]]></category>
		<category><![CDATA[synchrotron radiation]]></category>
		<category><![CDATA[time dependence]]></category>
		<category><![CDATA[time effect]]></category>
		<category><![CDATA[time scale]]></category>
		<category><![CDATA[time variability]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[zone models]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/time-dependent-simulations-of-emission-from-fsrq-pks1510-089-multiwavelength-variability-of-external-compton-and-ssc-models/</guid>
		<description><![CDATA[[abridged] We present results of modeling the SED and multiwavelength variability of the bright FSRQ PKS1510-089 with our time-dependent multizone Monte Carlo/Fokker-Planck code (Chen et al. 2001). As primary source of seed photons for inverse Compton scattering, we consider radiation from the broad line region (BLR), from the molecular torus, and the local synchrotron radiation [...]]]></description>
			<content:encoded><![CDATA[<p>[abridged] We present results of modeling the SED and multiwavelength variability of the bright FSRQ PKS1510-089 with our time-dependent multizone Monte Carlo/Fokker-Planck code (Chen et al. 2001). As primary source of seed photons for inverse Compton scattering, we consider radiation from the broad line region (BLR), from the molecular torus, and the local synchrotron radiation (SSC). Different scenarios are assessed by comparing simulated light curves and SEDs with one of the best flares by PKS1510-089, in March 2009. The time-dependence of our code and its correct handling of light travel time effects allow us to fully take into account the effect of the finite size of the active region, and in turn to fully exploit the information carried by time resolved observed SEDs, increasingly available since the launch of Fermi. We confirm that the spectrum adopted for the external radiation has an important impact on the modeling of the SED, in particular for the lower energy end of the Compton component, observed in the X-ray band, which in turn is one of the most critical bands to assess the differences between EC and SSC emission. In the context of the scenario presented here, where the flaring is caused by the increase of the number of relativistic electrons ascribed to the effect of the interaction of a portion of the jet (blob) with a shock, we can not firmly discriminate the three main scenarios for gamma-ray emission. However, results show clearly the differences produced by a more realistic treatment of the emitting source in the shape of SEDs and their time variability over relevant, observable time-scales, and demonstrate the crucial importance of time-dependent multi-zone models to advance our understanding of the physics of these sources, by taking full advantage of the wealth of information offered by the high quality data of current multiwavelength campaigns.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/time-dependent-simulations-of-emission-from-fsrq-pks1510-089-multiwavelength-variability-of-external-compton-and-ssc-models/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>No Correlation Between Disc Scale-Height and Jet Power in GRMHD Simulations [Replacement]</title>
		<link>http://voxcharta.org/2012/05/10/no-correlation-between-disc-scale-height-and-jet-power-in-grmhd-simulations-replacement/</link>
		<comments>http://voxcharta.org/2012/05/10/no-correlation-between-disc-scale-height-and-jet-power-in-grmhd-simulations-replacement/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:31:58 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion disc]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[corona]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[disc geometry]]></category>
		<category><![CDATA[jet power]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[mass x]]></category>
		<category><![CDATA[numerical simulation]]></category>
		<category><![CDATA[phenomena]]></category>
		<category><![CDATA[proxy]]></category>
		<category><![CDATA[radii]]></category>
		<category><![CDATA[radio power]]></category>
		<category><![CDATA[radio properties]]></category>
		<category><![CDATA[ray binaries]]></category>
		<category><![CDATA[thicknesses]]></category>
		<category><![CDATA[thin disc]]></category>
		<category><![CDATA[topology]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/no-correlation-between-disc-scale-height-and-jet-power-in-grmhd-simulations-replacement/</guid>
		<description><![CDATA[It is now well established that changes in the X-ray spectral state of black hole low-mass X-ray binaries are correlated with changes in the radio properties of those systems. Assuming radio power is a proxy for jet power, we can say that the jet is continuously present in the hard state and undetectable (and therefore [...]]]></description>
			<content:encoded><![CDATA[<p>It is now well established that changes in the X-ray spectral state of black hole low-mass X-ray binaries are correlated with changes in the radio properties of those systems. Assuming radio power is a proxy for jet power, we can say that the jet is continuously present in the hard state and undetectable (and therefore weaker) in the soft state. Since the different accretion states are also generally assumed to be associated with different disc geometries &#8212; the hard state with a hot, thick flow, and the soft state with a cold, thin disc &#8212; we investigate the possibility that these two phenomena are linked; i.e., that the difference in disc geometry is the cause of the difference in observed jet power. We do this by comparing various measures of jet power in numerical simulations of accretion discs of differing temperatures and thicknesses. We perform these simulations using the general relativistic magnetohydrodynamic code Cosmos++ and a newly added cooling function, which allows us to regulate the disc scale height H/r at different radii. We find no apparent correlation between the disc scale height and jet power whenever we normalize the latter by the mass accretion history of each simulation. We attribute this result to the role that the &#8220;corona&#8221; plays in confining and accelerating the jet (our corona may also be considered a failed MHD &#8220;wind&#8221;). The properties of the corona do not vary significantly from one simulation to another, even though the scale heights of the discs vary by up to a factor of four. If this holds true in nature, then it suggests that the correlation between spectral state and jet power must be attributable to some other property, possibly the topology of the magnetic field. Alternatively, it could be that the corona disappears altogether in the soft state, which would be consistent with observations, but has so far not been seen in simulations.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/no-correlation-between-disc-scale-height-and-jet-power-in-grmhd-simulations-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Fermi 130 GeV gamma-ray excess and dark matter annihilation in sub-haloes and in the Galactic centre [Replacement]</title>
		<link>http://voxcharta.org/2012/05/10/fermi-130-gev-gamma-ray-excess-and-dark-matter-annihilation-in-sub-haloes-and-in-the-galactic-centre-replacement-2/</link>
		<comments>http://voxcharta.org/2012/05/10/fermi-130-gev-gamma-ray-excess-and-dark-matter-annihilation-in-sub-haloes-and-in-the-galactic-centre-replacement-2/#comments</comments>
		<pubDate>Fri, 11 May 2012 00:31:50 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[annihilation]]></category>
		<category><![CDATA[cern]]></category>
		<category><![CDATA[clear peak]]></category>
		<category><![CDATA[cross section]]></category>
		<category><![CDATA[cusp]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[galactic centre]]></category>
		<category><![CDATA[gamma ray data]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[halo]]></category>
		<category><![CDATA[intermediate state]]></category>
		<category><![CDATA[lhc experiment]]></category>
		<category><![CDATA[model particles]]></category>
		<category><![CDATA[photon]]></category>
		<category><![CDATA[previous works]]></category>
		<category><![CDATA[signal peak]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectral feature]]></category>
		<category><![CDATA[standard model]]></category>
		<category><![CDATA[statistical significance]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/10/fermi-130-gev-gamma-ray-excess-and-dark-matter-annihilation-in-sub-haloes-and-in-the-galactic-centre-replacement-2/</guid>
		<description><![CDATA[We analyze publicly available Fermi-LAT high-energy gamma-ray data and confirm the existence of clear spectral feature peaked at $E_\gamma= 130$ GeV. Scanning over the Galaxy we identify several disconnected regions where the observed excess originates from. Our best optimized fit is obtained for the central region of Galaxy with a clear peak at 130 GeV [...]]]></description>
			<content:encoded><![CDATA[<p>We analyze publicly available Fermi-LAT high-energy gamma-ray data and confirm the existence of clear spectral feature peaked at $E_\gamma= 130$ GeV. Scanning over the Galaxy we identify several disconnected regions where the observed excess originates from. Our best optimized fit is obtained for the central region of Galaxy with a clear peak at 130 GeV with statistical significance $4.5\sigma.$ The observed excess is not correlated with Fermi bubbles. We compute the photon spectra induced by dark matter annihilations into two and four standard model particles, the latter via two light intermediate states, and fit the spectra with data. Since our fits indicate sharper and higher signal peak than in the previous works, data disfavors all but the dark matter direct two-body annihilation channels into photons. If Einasto halo profile correctly predicts the central cusp of Galaxy, dark matter annihilation cross-section to two photons is of order ten percent of the standard thermal freeze-out cross-section. If the observed gamma-ray excess comes from dark matter annihilations, we have identified the most dense dark matter sub-structures of our Galaxy. The large dark matter two-body annihilation cross-section to photons may signal a new resonance that should be searched for at the CERN LHC experiments.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/10/fermi-130-gev-gamma-ray-excess-and-dark-matter-annihilation-in-sub-haloes-and-in-the-galactic-centre-replacement-2/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Deep Silicate absorption features in Compton-thick AGN predominantly arise due to dust in the host galaxy</title>
		<link>http://voxcharta.org/2012/05/09/deep-silicate-absorption-features-in-compton-thick-agn-predominantly-arise-due-to-dust-in-the-host-galaxy/</link>
		<comments>http://voxcharta.org/2012/05/09/deep-silicate-absorption-features-in-compton-thick-agn-predominantly-arise-due-to-dust-in-the-host-galaxy/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:48:12 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorption feature]]></category>
		<category><![CDATA[AGN]]></category>
		<category><![CDATA[cm 2]]></category>
		<category><![CDATA[compton]]></category>
		<category><![CDATA[dust extinction]]></category>
		<category><![CDATA[hard energy]]></category>
		<category><![CDATA[host galaxy]]></category>
		<category><![CDATA[infrared spectrograph]]></category>
		<category><![CDATA[irs]]></category>
		<category><![CDATA[keV]]></category>
		<category><![CDATA[Lambda]]></category>
		<category><![CDATA[obs]]></category>
		<category><![CDATA[silicate]]></category>
		<category><![CDATA[spectral measurement]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[star formation]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/deep-silicate-absorption-features-in-compton-thick-agn-predominantly-arise-due-to-dust-in-the-host-galaxy/</guid>
		<description><![CDATA[We explore the origin of mid-infrared (mid-IR) dust extinction in all 20 nearby (z  1.5 x 10^24 cm^-2) AGN with hard energy (E &#62; 10 keV) X-ray spectral measurements. We accurately measure the silicate absorption features at lambda~9.7um in archival low-resolution (R~57-127) Spitzer Infrared Spectrograph (IRS) spectroscopy, and show that only a minority (~45%) [...]]]></description>
			<content:encoded><![CDATA[<p>We explore the origin of mid-infrared (mid-IR) dust extinction in all 20 nearby (z  1.5 x 10^24 cm^-2) AGN with hard energy (E &gt; 10 keV) X-ray spectral measurements. We accurately measure the silicate absorption features at lambda~9.7um in archival low-resolution (R~57-127) Spitzer Infrared Spectrograph (IRS) spectroscopy, and show that only a minority (~45%) of nearby Compton-thick AGN have strong Si-absorption features (S_9.7 = ln(f_{int}/f_{obs}) &gt; 0.5) which would indicate significant dust attenuation. The majority (~60%) are star-formation dominated (AGN:SB&lt;0.5) at mid-IR wavelengths and lack the spectral signatures of AGN activity at optical wavelengths, most likely because the AGN emission-lines are optically-extinguished. Those Compton-thick AGN hosted in low-inclination angle galaxies exhibit a narrow-range in Si-absorption (S_9.7 ~ 0-0.3), which is consistent with that predicted by clumpy-torus models. However, on the basis of the IR spectra and additional lines of evidence, we conclude that the dominant contribution to the observed mid-IR dust extinction is dust located in the host galaxy (i.e., due to disturbed morphologies; dust-lanes; galaxy inclination angles) and not necessarily a compact obscuring torus surrounding the central engine.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/deep-silicate-absorption-features-in-compton-thick-agn-predominantly-arise-due-to-dust-in-the-host-galaxy/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Energetic galaxy-wide outflows in high-redshift ultra-luminous infrared galaxies hosting AGN activity</title>
		<link>http://voxcharta.org/2012/05/09/energetic-galaxy-wide-outflows-in-high-redshift-ultra-luminous-infrared-galaxies-hosting-agn-activity/</link>
		<comments>http://voxcharta.org/2012/05/09/energetic-galaxy-wide-outflows-in-high-redshift-ultra-luminous-infrared-galaxies-hosting-agn-activity/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:47:57 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[AGN]]></category>
		<category><![CDATA[doublet]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[field spectroscopy]]></category>
		<category><![CDATA[galaxy dynamics]]></category>
		<category><![CDATA[high velocity]]></category>
		<category><![CDATA[host galaxy]]></category>
		<category><![CDATA[integral field]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[luminous galaxies]]></category>
		<category><![CDATA[luminous infrared galaxies]]></category>
		<category><![CDATA[massive galaxy]]></category>
		<category><![CDATA[merger]]></category>
		<category><![CDATA[offsets]]></category>
		<category><![CDATA[radio jet]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[signature]]></category>
		<category><![CDATA[sim4]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/energetic-galaxy-wide-outflows-in-high-redshift-ultra-luminous-infrared-galaxies-hosting-agn-activity/</guid>
		<description><![CDATA[We present integral field spectroscopy observations, covering the [O III]4959,5007 emission-line doublet of eight high-redshift (z=1.4-3.4) ultra-luminous infrared galaxies (ULIRGs) that host active galactic nuclei (AGN) activity, including known sub-millimetre luminous galaxies (SMGs). The targets have moderate radio luminosities that are typical of high-redshift ULIRGs (L[1.4GHz]=10^24-10^25 W/Hz) and therefore are not radio-loud AGN. We de-couple [...]]]></description>
			<content:encoded><![CDATA[<p>We present integral field spectroscopy observations, covering the [O III]4959,5007 emission-line doublet of eight high-redshift (z=1.4-3.4) ultra-luminous infrared galaxies (ULIRGs) that host active galactic nuclei (AGN) activity, including known sub-millimetre luminous galaxies (SMGs). The targets have moderate radio luminosities that are typical of high-redshift ULIRGs (L[1.4GHz]=10^24-10^25 W/Hz) and therefore are not radio-loud AGN. We de-couple kinematic components due to the galaxy dynamics and mergers from those due to outflows. We find evidence in the most luminous systems, L([O III])\gtrsim10^43 erg/s, for the signatures of large-scale energetic outflows: extremely broad [O III] emission (FWHM \sim 700-1400 km/s) across \sim4-15 kpc, with high velocity offsets from the systemic redshifts (up to \sim850 km/s). These outflows are potentially depositing energy into their host galaxies at considerable rates (\sim10^43-10^45 erg/s) and are likely to unbind some of the gas from the host galaxies. Based on energetic arguments we find that the radiative power of the AGN, as opposed to star formation or radio jets, is likely to dominate in driving these outflows. We suggest that the galaxies observed may represent a key stage in the evolution of massive galaxies.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/energetic-galaxy-wide-outflows-in-high-redshift-ultra-luminous-infrared-galaxies-hosting-agn-activity/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Possible Detection of an Emission Cyclotron Resonance Scattering Feature from the Accretion-powered Pulsar 4U 1626-67</title>
		<link>http://voxcharta.org/2012/05/09/possible-detection-of-an-emission-cyclotron-resonance-scattering-feature-from-the-accretion-powered-pulsar-4u-1626-67/</link>
		<comments>http://voxcharta.org/2012/05/09/possible-detection-of-an-emission-cyclotron-resonance-scattering-feature-from-the-accretion-powered-pulsar-4u-1626-67/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:47:26 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorption]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[binary system]]></category>
		<category><![CDATA[cm 2]]></category>
		<category><![CDATA[cyclotron resonance]]></category>
		<category><![CDATA[emission line]]></category>
		<category><![CDATA[gaussian model]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[mass x]]></category>
		<category><![CDATA[phase spectrum]]></category>
		<category><![CDATA[physical parameter]]></category>
		<category><![CDATA[ray detector]]></category>
		<category><![CDATA[resonance energy]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[statistical significance]]></category>
		<category><![CDATA[suzaku]]></category>
		<category><![CDATA[systematic error]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[x10]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/possible-detection-of-an-emission-cyclotron-resonance-scattering-feature-from-the-accretion-powered-pulsar-4u-1626-67/</guid>
		<description><![CDATA[We present analysis of 4U 1626-67, a 7.7 s pulsar in a low-mass X-ray binary system, observed with the hard X-ray detector of the Japanese X-ray satellite Suzaku in March 2006 for a net exposure of \sim88 ks. The source was detected at an average 10-60 keV flux of \sim4 x10^-10 erg cm^-2 s^-1. The [...]]]></description>
			<content:encoded><![CDATA[<p>We present analysis of 4U 1626-67, a 7.7 s pulsar in a low-mass X-ray binary system, observed with the hard X-ray detector of the Japanese X-ray satellite Suzaku in March 2006 for a net exposure of \sim88 ks. The source was detected at an average 10-60 keV flux of \sim4 x10^-10 erg cm^-2 s^-1. The phase-averaged spectrum is reproduced well by combining a negative and positive power-law times exponential cutoff (NPEX) model modified at \sim 37 keV by a cyclotron resonance scattering feature (CRSF). The phase-resolved analysis shows that the spectra at the bright phases are well fit by the NPEX with CRSF model. On the other hand, the spectrum in the dim phase lacks the NPEX high-energy cutoff component, and the CRSF can be reproduced by either an emission or an absorption profile. When fitting the dim phase spectrum with the NPEX plus Gaussian model, we find that the feature is better described in terms of an emission rather than an absorption profile. The statistical significance of this result, evaluated by means of an F-test, is between 2.91 x 10^-3 and 1.53 x 10^-5, taking into account the systematic errors in the background evaluation of HXD-PIN. We find that, the emission profile is more feasible than the absorption one for comparing the physical parameters in other phases. Therefore, we have possibly detected an emission line at the cyclotron resonance energy in the dim phase.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/possible-detection-of-an-emission-cyclotron-resonance-scattering-feature-from-the-accretion-powered-pulsar-4u-1626-67/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Mass Measurements of Black Holes in X-Ray Transients: Is There a Mass Gap?</title>
		<link>http://voxcharta.org/2012/05/09/mass-measurements-of-black-holes-in-x-ray-transients-is-there-a-mass-gap/</link>
		<comments>http://voxcharta.org/2012/05/09/mass-measurements-of-black-holes-in-x-ray-transients-is-there-a-mass-gap/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:47:13 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[careful examination]]></category>
		<category><![CDATA[donor]]></category>
		<category><![CDATA[gap]]></category>
		<category><![CDATA[hole mass]]></category>
		<category><![CDATA[low mass]]></category>
		<category><![CDATA[mass distribution]]></category>
		<category><![CDATA[mass gap]]></category>
		<category><![CDATA[mass measurement]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[odot]]></category>
		<category><![CDATA[orbital inclination]]></category>
		<category><![CDATA[paucity]]></category>
		<category><![CDATA[soft x]]></category>
		<category><![CDATA[systematic error]]></category>
		<category><![CDATA[transients]]></category>
		<category><![CDATA[typical data]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/mass-measurements-of-black-holes-in-x-ray-transients-is-there-a-mass-gap/</guid>
		<description><![CDATA[We explore possible systematic errors in the mass measurements of stellar mass black holes. We find that significant errors can arise from the assumption of zero or constant emission from the accretion flow, which is commonly used when determining orbital inclination by modelling ellipsoidal variations. For A0620-00, the system with the best available data, we [...]]]></description>
			<content:encoded><![CDATA[<p>We explore possible systematic errors in the mass measurements of stellar mass black holes. We find that significant errors can arise from the assumption of zero or constant emission from the accretion flow, which is commonly used when determining orbital inclination by modelling ellipsoidal variations. For A0620-00, the system with the best available data, we show that typical data sets and analysis procedures can lead to systematic underestimates of the inclination by ten degrees or more. A careful examination of the available data for the 15 other X-ray transients with low-mass donors suggests that this effect may significantly reduce the black hole mass estimates in several other cases, most notably that of GRO J0422+32. With these revisions, our analysis of the black hole mass distribution in soft X-ray transients does not suggest any &#8220;mass gap&#8221; between the low end of the distribution and the maximum theoretical neutron star mass, as has been identified in previous studies. Nevertheless, we find that the mass distribution retains other previously identified characteristics, namely a peak around 8M\odot, a paucity of sources with masses below 5M\odot, and a sharp drop-off above 10M\odot.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/mass-measurements-of-black-holes-in-x-ray-transients-is-there-a-mass-gap/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A combined Optical and X-ray Spectra Study for Type 1 AGN. III. Broadband SED Properties</title>
		<link>http://voxcharta.org/2012/05/09/a-combined-optical-and-x-ray-spectra-study-for-type-1-agn-iii-broadband-sed-properties/</link>
		<comments>http://voxcharta.org/2012/05/09/a-combined-optical-and-x-ray-spectra-study-for-type-1-agn-iii-broadband-sed-properties/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:46:08 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion rates]]></category>
		<category><![CDATA[bhb]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[correlation matrix]]></category>
		<category><![CDATA[cross correlation]]></category>
		<category><![CDATA[eddington]]></category>
		<category><![CDATA[hole mass]]></category>
		<category><![CDATA[pca results]]></category>
		<category><![CDATA[physical parameter]]></category>
		<category><![CDATA[principal component analysis]]></category>
		<category><![CDATA[principal component analysis pca]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[spectral index]]></category>
		<category><![CDATA[spectral states]]></category>
		<category><![CDATA[spectral studies]]></category>
		<category><![CDATA[supermassive black hole]]></category>
		<category><![CDATA[systematic change]]></category>
		<category><![CDATA[uv line]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/a-combined-optical-and-x-ray-spectra-study-for-type-1-agn-iii-broadband-sed-properties/</guid>
		<description><![CDATA[In this third paper in a series of three, we present a detailed study of the AGN broadband SED based on a nearby unobscured Type 1 AGN sample. We perform a systematic cross-correlation study of the following key parameters: $\Gamma_{2-10keV}$, $L_{2-10keV}$, $L_{bol}$, $L_{bol}/L_{Edd}$, $\kappa_{2-10keV}$, $\kappa_{5100A}$, FWHM$_{H\beta}$, M$_{BH}$, $\alpha_{ox}$, $\alpha_{X}$ and $\alpha_{UV}$, and identify various strong [...]]]></description>
			<content:encoded><![CDATA[<p>In this third paper in a series of three, we present a detailed study of the AGN broadband SED based on a nearby unobscured Type 1 AGN sample. We perform a systematic cross-correlation study of the following key parameters: $\Gamma_{2-10keV}$, $L_{2-10keV}$, $L_{bol}$, $L_{bol}/L_{Edd}$, $\kappa_{2-10keV}$, $\kappa_{5100A}$, FWHM$_{H\beta}$, M$_{BH}$, $\alpha_{ox}$, $\alpha_{X}$ and $\alpha_{UV}$, and identify various strong correlations among these parameters. The principal component analysis (PCA) is performed on the correlation matrix of the above parameters, which shows that the three physical parameters, i.e. black hole mass, mass accretion rate and Eddington ratio, drive the majority of the correlations. This is consistent with PCA results found from previous optical spectral studies.   We produce various mean SEDs classified by each of the key parameters. Most parameters, except L$_{bol}$, show similar systematic changes in the mean SEDs such that the temperature at which the disc peaks is correlated with the ratio of power in the disc versus the Comptonised components and the hard X-ray spectral index. This underlying change in SED shape shows that AGN do exhibit intrinsically different spectral states. This is superficially similar to the SED differences in BHB seen as $\lambda_{Edd}$ increases, but the analogy does not hold in detail. Only objects with the highest $\lambda_{Edd}$ appear to correspond to a BHB spectral state (the disc dominated high/soft state). The AGN with typical mass accretion rates have spectra which do not match well with any state observed in BHB. We speculate that this could be due to the presence of a powerful UV line driven disc wind, which complicates simple mass scaling between stellar and supermassive black holes.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/a-combined-optical-and-x-ray-spectra-study-for-type-1-agn-iii-broadband-sed-properties/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>On the instability regime of the rotating Kerr spacetime to massive scalar perturbations [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/09/on-the-instability-regime-of-the-rotating-kerr-spacetime-to-massive-scalar-perturbations-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/09/on-the-instability-regime-of-the-rotating-kerr-spacetime-to-massive-scalar-perturbations-cross-listing/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:45:43 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[angular frequency]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[bomb]]></category>
		<category><![CDATA[dynamical instability]]></category>
		<category><![CDATA[kerr]]></category>
		<category><![CDATA[mirror]]></category>
		<category><![CDATA[perturbation]]></category>
		<category><![CDATA[phenomena]]></category>
		<category><![CDATA[regime]]></category>
		<category><![CDATA[rest mass]]></category>
		<category><![CDATA[spacetime]]></category>
		<category><![CDATA[turning point]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/on-the-instability-regime-of-the-rotating-kerr-spacetime-to-massive-scalar-perturbations-cross-listing/</guid>
		<description><![CDATA[The instability of rotating Kerr black holes due to massive scalar perturbations is investigated. It is well known that a bosonic field impinging on a Kerr black hole can be amplified as it scatters off the hole. This superradiant scattering occurs for frequencies in the range $\omega&#60;m\Omega$, where $\Omega$ is the angular frequency of the [...]]]></description>
			<content:encoded><![CDATA[<p>The instability of rotating Kerr black holes due to massive scalar perturbations is investigated. It is well known that a bosonic field impinging on a Kerr black hole can be amplified as it scatters off the hole. This superradiant scattering occurs for frequencies in the range $\omega&lt;m\Omega$, where $\Omega$ is the angular frequency of the black hole and $m$ is the azimuthal harmonic index of the mode. If the incident field has a non-zero rest mass, $\mu$, then the mass term effectively works as a mirror, reflecting the scattered wave back towards the black hole. The wave may bounce back and forth between the black hole and some turning point amplifying itself each time. This may lead to a dynamical instability of the system, a phenomena known as a &quot;black-hole bomb&quot;. In this work we provide a bound on the instability regime of rotating Kerr spacetimes. In particular, we show that Kerr black holes are stable to massive perturbations in the regime $\mu\geq\sqrt{2}m\Omega$.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/on-the-instability-regime-of-the-rotating-kerr-spacetime-to-massive-scalar-perturbations-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Hot Electron and Pair Production from the Texas Petawatt Laser Irradiating Thick Gold Targets [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/09/hot-electron-and-pair-production-from-the-texas-petawatt-laser-irradiating-thick-gold-targets-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/09/hot-electron-and-pair-production-from-the-texas-petawatt-laser-irradiating-thick-gold-targets-cross-listing/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:45:33 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[cm 2]]></category>
		<category><![CDATA[deconvolution algorithm]]></category>
		<category><![CDATA[direct evidence]]></category>
		<category><![CDATA[electron]]></category>
		<category><![CDATA[energy spectra]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[intensity]]></category>
		<category><![CDATA[magnetic spectrometer]]></category>
		<category><![CDATA[Measurement]]></category>
		<category><![CDATA[mev]]></category>
		<category><![CDATA[pair production]]></category>
		<category><![CDATA[petawatt laser]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[target]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/hot-electron-and-pair-production-from-the-texas-petawatt-laser-irradiating-thick-gold-targets-cross-listing/</guid>
		<description><![CDATA[We present data from electron-positron pair production by an ultra-intense laser incident on solid Au targets with thickness between 1 and 4 mm. The experiment was performed at the Texas Petawatt Laser in July 2011, with intensities on the order of several x1019W.cm-2 and laser energies around 50 J. We discuss the design of an [...]]]></description>
			<content:encoded><![CDATA[<p>We present data from electron-positron pair production by an ultra-intense laser incident on solid Au targets with thickness between 1 and 4 mm. The experiment was performed at the Texas Petawatt Laser in July 2011, with intensities on the order of several x1019W.cm-2 and laser energies around 50 J. We discuss the design of an electron-positron magnetic spectrometer to record the lepton energy spectra ejected from the Au targets. We then present a deconvolution algorithm to extract the lepton energy spectra. We measured hot electron spectra out to &gt; 50MeV, which show a narrow peak around 10 &#8211; 15 MeV, plus exponential tail consistent with ponderomotive temperature scaling. We did not observe direct evidence of positron production above the background, even though separate gamma-ray measurement hints at the presence of positrons.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/hot-electron-and-pair-production-from-the-texas-petawatt-laser-irradiating-thick-gold-targets-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Diffusive Shock Acceleration Simulations of Radio Relics</title>
		<link>http://voxcharta.org/2012/05/09/diffusive-shock-acceleration-simulations-of-radio-relics/</link>
		<comments>http://voxcharta.org/2012/05/09/diffusive-shock-acceleration-simulations-of-radio-relics/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:44:45 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[clusters of galaxies]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[electron acceleration]]></category>
		<category><![CDATA[electron injection]]></category>
		<category><![CDATA[energy loss]]></category>
		<category><![CDATA[gev electron]]></category>
		<category><![CDATA[inverse compton]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[merger]]></category>
		<category><![CDATA[outskirt]]></category>
		<category><![CDATA[radiation]]></category>
		<category><![CDATA[radio emission]]></category>
		<category><![CDATA[radio observation]]></category>
		<category><![CDATA[radio relics]]></category>
		<category><![CDATA[shock]]></category>
		<category><![CDATA[shock acceleration]]></category>
		<category><![CDATA[shock wave]]></category>
		<category><![CDATA[simulation]]></category>
		<category><![CDATA[spectral distribution]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/diffusive-shock-acceleration-simulations-of-radio-relics/</guid>
		<description><![CDATA[Recent radio observations have identified a class of structures, so-called radio relics, in clusters of galaxies. The radio emission from these sources is interpreted as synchrotron radiation from GeV electrons gyrating in microG-level magnetic fields. Radio relics, located mostly in the outskirts of clusters, seem to associate with shock waves, especially those developed during mergers. [...]]]></description>
			<content:encoded><![CDATA[<p>Recent radio observations have identified a class of structures, so-called radio relics, in clusters of galaxies. The radio emission from these sources is interpreted as synchrotron radiation from GeV electrons gyrating in microG-level magnetic fields. Radio relics, located mostly in the outskirts of clusters, seem to associate with shock waves, especially those developed during mergers. In fact, they seem to be good structures to identify and probe such shocks in intracluster media (ICMs), provided we understand the electron acceleration and re-acceleration at those shocks. In this paper, we describe time-dependent simulations for diffusive shock acceleration at weak shocks that are expected to be found in ICMs. Freshly injected as well as pre-existing populations of cosmic-ray (CR) electrons are considered, and energy losses via synchrotron and inverse Compton are included. We then compare the synchrotron flux and spectral distributions estimated from the simulations with those in two well-observed radio relics in CIZA J2242.8+5301 and ZwCl0008.8+5215. Considering that the CR electron injection is rather inefficient at weak shocks with Mach number M &lt;~ a few, the existence of radio relics could indicate the pre-existing population of low-energy CR electrons in ICMs. The implication of our results on the merger shock scenario of radio relics is discussed.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/diffusive-shock-acceleration-simulations-of-radio-relics/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>VLT Suzaku observations of the Fermi pulsar PSR J1028-5819</title>
		<link>http://voxcharta.org/2012/05/09/vlt-suzaku-observations-of-the-fermi-pulsar-psr-j1028-5819/</link>
		<comments>http://voxcharta.org/2012/05/09/vlt-suzaku-observations-of-the-fermi-pulsar-psr-j1028-5819/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:44:12 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absorption]]></category>
		<category><![CDATA[angular extent]]></category>
		<category><![CDATA[cm 2]]></category>
		<category><![CDATA[column density]]></category>
		<category><![CDATA[diffuse emission]]></category>
		<category><![CDATA[Fermi]]></category>
		<category><![CDATA[nebula]]></category>
		<category><![CDATA[observation]]></category>
		<category><![CDATA[optical counterpart]]></category>
		<category><![CDATA[optical image]]></category>
		<category><![CDATA[presence]]></category>
		<category><![CDATA[radio]]></category>
		<category><![CDATA[spectral index]]></category>
		<category><![CDATA[spectrum]]></category>
		<category><![CDATA[surface brightness]]></category>
		<category><![CDATA[Telescope]]></category>
		<category><![CDATA[type star]]></category>
		<category><![CDATA[uncertainty]]></category>
		<category><![CDATA[vlt]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/vlt-suzaku-observations-of-the-fermi-pulsar-psr-j1028-5819/</guid>
		<description><![CDATA[We used optical images taken with the Very Large Telescope (VLT) in the B and V bands to search for the optical counterpart of PSR J1028-5819 or constrain its optical brightness. At the same time, we used an archival Suzaku observation to confirm the preliminary identification of the pulsar&#8217;s X-ray counterpart obtained by Swift. Due [...]]]></description>
			<content:encoded><![CDATA[<p>We used optical images taken with the Very Large Telescope (VLT) in the B and V bands to search for the optical counterpart of PSR J1028-5819 or constrain its optical brightness. At the same time, we used an archival Suzaku observation to confirm the preliminary identification of the pulsar&#8217;s X-ray counterpart obtained by Swift. Due to the large uncertainty on the pulsar&#8217;s radio position and the presence of a bright (V = 13.2) early F-type star at &lt; 4&quot;, we could not detect its counterpart down to flux limits of B~25.4 and V ~25.3, the deepest obtained so far for PSR J1028-5819. From the Suzaku observations, we found that the X-ray spectrum of the pulsar&#039;s candidate counterpart is best-fit by a power-law with spectral index 1.7 +/- 0.2 and an absorption column density NH &lt; 10^21 cm-2, which would support the proposed X-ray identification. Moreover, we found possible evidence for the presence of diffuse emission around the pulsar. If real, and associated with a pulsar wind nebula (PWN), its surface brightness and angular extent would be compatible with the expectations for a ~100 kyr old pulsar at the PSR J1028-5819 distance.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/vlt-suzaku-observations-of-the-fermi-pulsar-psr-j1028-5819/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Unification and physical interpretation of the radio spectra variability patterns in Fermi blazars and jet emission from NLSy1s</title>
		<link>http://voxcharta.org/2012/05/09/unification-and-physical-interpretation-of-the-radio-spectra-variability-patterns-in-fermi-blazars-and-jet-emission-from-nlsy1s/</link>
		<comments>http://voxcharta.org/2012/05/09/unification-and-physical-interpretation-of-the-radio-spectra-variability-patterns-in-fermi-blazars-and-jet-emission-from-nlsy1s/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:41:38 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[3 years]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[band radio]]></category>
		<category><![CDATA[blazar]]></category>
		<category><![CDATA[broad band]]></category>
		<category><![CDATA[cm to mm]]></category>
		<category><![CDATA[component model]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[physical interpretation]]></category>
		<category><![CDATA[physics]]></category>
		<category><![CDATA[radio spectra]]></category>
		<category><![CDATA[spectral evolution]]></category>
		<category><![CDATA[time span]]></category>
		<category><![CDATA[unification]]></category>
		<category><![CDATA[variability]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/unification-and-physical-interpretation-of-the-radio-spectra-variability-patterns-in-fermi-blazars-and-jet-emission-from-nlsy1s/</guid>
		<description><![CDATA[The F-GAMMA program is among the most comprehensive programs that aim at understanding the physics in active galactic nuclei through the multi-frequency monitoring of Fermi blazars. Here we discuss monthly sampled broad-band radio spectra (2.6 &#8211; 142 GHz). Two different studies are presented. (a) We discuss that the variability patterns traced can be classified into [...]]]></description>
			<content:encoded><![CDATA[<p>The F-GAMMA program is among the most comprehensive programs that aim at understanding the physics in active galactic nuclei through the multi-frequency monitoring of Fermi blazars. Here we discuss monthly sampled broad-band radio spectra (2.6 &#8211; 142 GHz). Two different studies are presented. (a) We discuss that the variability patterns traced can be classified into two classes: (1) to those showing intense spectral-evolution and (2) those showing a self-similar quasi-achromatic behaviour. We show that a simple two-component model can very well reproduce the observed phenomenologies. (b) We present the cm-to-mm behaviour of three gamma-ray bright Narrow Line Seyfert 1 galaxies over time spans varying between ~1.5 and 3 years and compare their variability characteristics with typical blazars.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/unification-and-physical-interpretation-of-the-radio-spectra-variability-patterns-in-fermi-blazars-and-jet-emission-from-nlsy1s/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>Properties and Spatial Distribution of Dust Emission in the Crab Nebula</title>
		<link>http://voxcharta.org/2012/05/09/properties-and-spatial-distribution-of-dust-emission-in-the-crab-nebula/</link>
		<comments>http://voxcharta.org/2012/05/09/properties-and-spatial-distribution-of-dust-emission-in-the-crab-nebula/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:38:51 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[amorphous carbon]]></category>
		<category><![CDATA[carbon grains]]></category>
		<category><![CDATA[continuum emission]]></category>
		<category><![CDATA[core collapse supernova]]></category>
		<category><![CDATA[crab nebula]]></category>
		<category><![CDATA[dust emission]]></category>
		<category><![CDATA[dust grains]]></category>
		<category><![CDATA[emission spectra]]></category>
		<category><![CDATA[filament]]></category>
		<category><![CDATA[infrared spectrograph]]></category>
		<category><![CDATA[ir spectra]]></category>
		<category><![CDATA[line emission]]></category>
		<category><![CDATA[silicate]]></category>
		<category><![CDATA[solar mass]]></category>
		<category><![CDATA[spatial distribution]]></category>
		<category><![CDATA[spitzer space telescope]]></category>
		<category><![CDATA[supernova remnant]]></category>
		<category><![CDATA[synchrotron nebula]]></category>
		<category><![CDATA[theoretical model]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/properties-and-spatial-distribution-of-dust-emission-in-the-crab-nebula/</guid>
		<description><![CDATA[Recent infrared (IR) observations of freshly-formed dust in supernova remnants (SNRs) have yielded significantly lower dust masses than predicted by theoretical models and measured from high redshift observations. The Crab Nebula&#8217;s pulsar wind is thought to be sweeping up freshly-formed supernova (SN) dust along with the ejected gas. The evidence for this dust was found [...]]]></description>
			<content:encoded><![CDATA[<p>Recent infrared (IR) observations of freshly-formed dust in supernova remnants (SNRs) have yielded significantly lower dust masses than predicted by theoretical models and measured from high redshift observations. The Crab Nebula&#8217;s pulsar wind is thought to be sweeping up freshly-formed supernova (SN) dust along with the ejected gas. The evidence for this dust was found in the form of an IR excess in the integrated spectrum of the Crab and in extinction against the synchrotron nebula that revealed the presence of dust in the filament cores. We present the first spatially resolved emission spectra of dust in the Crab Nebula acquired with the Infrared Spectrograph aboard the Spitzer Space Telescope. The IR spectra are dominated by synchrotron emission and show forbidden line emission from from S, Si, Ne, Ar, O, Fe, and Ni. We derived a synchrotron spectral map from the 3.6 and 4.5 microns images, and subtracted this contribution from our data to produce a map of the residual continuum emission from dust. The dust emission appears to be concentrated along the ejecta filaments and is well described by an amorphous carbon or silicate grain compositions. We find a dust temperature of 55+/- 4 K for silicates and 60 +/- 7 K for carbon grains. The total estimated dust mass is 0.0012-0.012 solar masses, well below the theoretical dust yield predicted for a core-collapse supernova. Our grain heating model implies that the dust grain radii are relatively small, unlike what is expected for dust grains formed in a Type IIP SN.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/properties-and-spatial-distribution-of-dust-emission-in-the-crab-nebula/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>
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		<title>On the origin of LS 5039 and PSR J1825-1446</title>
		<link>http://voxcharta.org/2012/05/09/on-the-origin-of-ls-5039-and-psr-j1825-1446/</link>
		<comments>http://voxcharta.org/2012/05/09/on-the-origin-of-ls-5039-and-psr-j1825-1446/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:38:21 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[ascension and declination]]></category>
		<category><![CDATA[characteristic age]]></category>
		<category><![CDATA[conclusion]]></category>
		<category><![CDATA[distance]]></category>
		<category><![CDATA[galactic rotation]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[high velocity]]></category>
		<category><![CDATA[kyr]]></category>
		<category><![CDATA[myr]]></category>
		<category><![CDATA[ob2]]></category>
		<category><![CDATA[optical observation]]></category>
		<category><![CDATA[orbit]]></category>
		<category><![CDATA[proper motion]]></category>
		<category><![CDATA[pulsar psr]]></category>
		<category><![CDATA[right ascension and declination]]></category>
		<category><![CDATA[snr]]></category>
		<category><![CDATA[supernova remnant]]></category>
		<category><![CDATA[synchronization]]></category>
		<category><![CDATA[trajectory]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/on-the-origin-of-ls-5039-and-psr-j1825-1446/</guid>
		<description><![CDATA[Context. The gamma-ray binary LS 5039 and the isolated pulsar PSR J1825-1446 were proposed to have been formed in the supernova remnant (SNR) G016.8-01.1. Aims. We aim to obtain the Galactic trajectory of LS 5039 and PSR J1825-1446 to find their origin in the Galaxy, and in particular to check their association with SNR G016.8-01.1 [...]]]></description>
			<content:encoded><![CDATA[<p>Context. The gamma-ray binary LS 5039 and the isolated pulsar PSR J1825-1446 were proposed to have been formed in the supernova remnant (SNR) G016.8-01.1. Aims. We aim to obtain the Galactic trajectory of LS 5039 and PSR J1825-1446 to find their origin in the Galaxy, and in particular to check their association with SNR G016.8-01.1 to restrict their age. Methods. By means of radio and optical observations we obtained the proper motion and the space velocity of the sources. Results. The proper motion of PSR J1825-1446 corresponds to a transverse space velocity of 690 km/s at a distance of 5 kpc. Its Galactic velocity at different distances is not compatible with the expected Galactic rotation. The velocity and characteristic age of PSR J1825-1446 make it incompatible with SNR G016.8-01.1. There are no clear OB associations or SNRs crossing the past trajectory of PSR J1825-1446. We estimate the age of the pulsar to be 80-245 kyr, which is compatible with its characteristic age. The proper motion of LS 5039 is 7.09 and -8.82 mas/yr in right ascension and declination, respectively. The association of LS 5039 with SNR G016.8-01.1 is unlikely, although we cannot to discard it. The system would have had to be formed in the association Ser OB2 (at 2.0 kpc) if the age of the system is 1.0-1.2 Myr, or in the association Sct OB3 (distance 1.5-2 kpc) for an age of 0.1-0.2 Myr. If the system were not formed close to Ser OB2, the pseudo-synchronization of the orbit would be unlikely. Conclusions. PSR J1825-1446 is a high-velocity isolated pulsar ejected from the Galaxy. The distance to LS 5039, which needs to be constrained by future astrometric missions such as Gaia, is a key parameter for restricting its origin and age.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/on-the-origin-of-ls-5039-and-psr-j1825-1446/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Cosmological Impact of Luminous TeV Blazars I: Implications of Plasma Instabilities for the Intergalactic Magnetic Field and Extragalactic Gamma-Ray Background [Replacement]</title>
		<link>http://voxcharta.org/2012/05/09/the-cosmological-impact-of-luminous-tev-blazars-i-implications-of-plasma-instabilities-for-the-intergalactic-magnetic-field-and-extragalactic-gamma-ray-background-replacement/</link>
		<comments>http://voxcharta.org/2012/05/09/the-cosmological-impact-of-luminous-tev-blazars-i-implications-of-plasma-instabilities-for-the-intergalactic-magnetic-field-and-extragalactic-gamma-ray-background-replacement/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:37:53 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[annihilation]]></category>
		<category><![CDATA[background light]]></category>
		<category><![CDATA[blazar]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[energy loss]]></category>
		<category><![CDATA[Fermi]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[intergalactic medium]]></category>
		<category><![CDATA[inverse compton]]></category>
		<category><![CDATA[loss mechanism]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[plasma beam]]></category>
		<category><![CDATA[plasma instability]]></category>
		<category><![CDATA[plausible mechanism]]></category>
		<category><![CDATA[primary energy]]></category>
		<category><![CDATA[quasar luminosity function]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[stringent limits]]></category>
		<category><![CDATA[tev sources]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/the-cosmological-impact-of-luminous-tev-blazars-i-implications-of-plasma-instabilities-for-the-intergalactic-magnetic-field-and-extragalactic-gamma-ray-background-replacement/</guid>
		<description><![CDATA[Inverse-Compton cascades initiated by energetic gamma rays (E&#62;100 GeV) enhance the GeV emission from bright, extragalactic TeV sources. The absence of this emission from bright TeV blazars has been used to constrain the intergalactic magnetic field (IGMF), and the stringent limits placed upon the unresolved extragalactic gamma-ray background (EGRB) by Fermi has been used to [...]]]></description>
			<content:encoded><![CDATA[<p>Inverse-Compton cascades initiated by energetic gamma rays (E&gt;100 GeV) enhance the GeV emission from bright, extragalactic TeV sources. The absence of this emission from bright TeV blazars has been used to constrain the intergalactic magnetic field (IGMF), and the stringent limits placed upon the unresolved extragalactic gamma-ray background (EGRB) by Fermi has been used to argue against a large number of such objects at high redshifts. However, these are predicated upon the assumption that inverse-Compton scattering is the primary energy-loss mechanism for the ultra-relativistic pairs produced by the annihilation of the energetic gamma rays on extragalactic background light photons. Here we show that for sufficiently bright TeV sources (isotropic-equivalent luminosities &gt;10^{42} erg/s) plasma beam instabilities, specifically the &#8220;oblique&#8221; instability, present a plausible mechanism by which the energy of these pairs can be dissipated locally, heating the intergalactic medium. Since these instabilities typically grow on timescales short in comparison to the inverse-Compton cooling rate, they necessarily suppress the inverse-Compton cascades. As a consequence, this places a severe constraint upon efforts to limit the IGMF from the lack of a discernible GeV bump in TeV sources. Similarly, it considerably weakens the Fermi limits upon the evolution of blazar populations. Specifically, we construct a TeV-blazar luminosity function from those objects presently observed and find that it is very well described by the quasar luminosity function at z~0.1, shifted to lower luminosities and number densities, suggesting that both classes of sources are regulated by similar processes. Extending this relationship to higher redshifts, we show that the magnitude and shape of the EGRB above ~10 GeV is naturally reproduced with this particular example of a rapidly evolving TeV-blazar luminosity function.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/the-cosmological-impact-of-luminous-tev-blazars-i-implications-of-plasma-instabilities-for-the-intergalactic-magnetic-field-and-extragalactic-gamma-ray-background-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Cosmological Impact of Luminous TeV Blazars II: Rewriting the Thermal History of the Intergalactic Medium [Replacement]</title>
		<link>http://voxcharta.org/2012/05/09/the-cosmological-impact-of-luminous-tev-blazars-ii-rewriting-the-thermal-history-of-the-intergalactic-medium-replacement/</link>
		<comments>http://voxcharta.org/2012/05/09/the-cosmological-impact-of-luminous-tev-blazars-ii-rewriting-the-thermal-history-of-the-intergalactic-medium-replacement/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:37:44 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[bl lac]]></category>
		<category><![CDATA[blazar]]></category>
		<category><![CDATA[broderick]]></category>
		<category><![CDATA[energy gamma rays]]></category>
		<category><![CDATA[extragalactic background light]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[intergalactic medium]]></category>
		<category><![CDATA[inverse compton]]></category>
		<category><![CDATA[kinetic energy]]></category>
		<category><![CDATA[luminosity density]]></category>
		<category><![CDATA[pair]]></category>
		<category><![CDATA[photon]]></category>
		<category><![CDATA[plasma instability]]></category>
		<category><![CDATA[TeV]]></category>
		<category><![CDATA[thermal history]]></category>
		<category><![CDATA[universe]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/the-cosmological-impact-of-luminous-tev-blazars-ii-rewriting-the-thermal-history-of-the-intergalactic-medium-replacement/</guid>
		<description><![CDATA[The Universe is opaque to extragalactic very high-energy gamma rays (VHEGRs, E&#62;100 GeV) because they annihilate and pair produce on the extragalactic background light. The resulting ultra-relativistic pairs are assumed to lose energy through inverse Compton scattering of CMB photons. In Broderick et al. (2011, Paper I of this three paper series), we argued that [...]]]></description>
			<content:encoded><![CDATA[<p>The Universe is opaque to extragalactic very high-energy gamma rays (VHEGRs, E&gt;100 GeV) because they annihilate and pair produce on the extragalactic background light. The resulting ultra-relativistic pairs are assumed to lose energy through inverse Compton scattering of CMB photons. In Broderick et al. (2011, Paper I of this three paper series), we argued that instead powerful plasma instabilities in the ultra-relativistic pair beam dissipate the kinetic energy of the TeV-generated pairs locally, heating the intergalactic medium (IGM). Here, we explore the effect of this heating upon the thermal history of the IGM. We collate the observed extragalactic VHEGR sources to determine a local VHEGR heating rate and correct for the pointed nature of VHEGR observations using Fermi observations of high and intermediate peaked BL Lacs. Because the local extragalactic VHEGR flux is dominated by TeV blazars, we tie the TeV blazar luminosity density to the quasar luminosity density, and produce a VHEGR heating rate as a function of redshift. This heating is relatively homogeneous for z&lt;~4 with increasing spatial variation at higher redshift (order unity at z~6). This new heating process dominates photoheating at low redshift and the inclusion of TeV blazar heating qualitatively and quantitatively changes the structure and history of the IGM. TeV blazars produce a uniform volumetric heating rate that is sufficient to increase the temperature of the mean density IGM by nearly an order of magnitude, and at low densities by substantially more, naturally producing an inverted equation of state inferred by observations of the Ly-alpha forest, a feature that is difficult to reconcile with standard reionization models. Finally, we close with a discussion on the possibility of detecting this hot low-density IGM, but find that such measurements are currently not feasible. (abridged)</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/the-cosmological-impact-of-luminous-tev-blazars-ii-rewriting-the-thermal-history-of-the-intergalactic-medium-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Cosmological Impact of Luminous TeV Blazars III: Implications for Galaxy Clusters and the Formation of Dwarf Galaxies [Replacement]</title>
		<link>http://voxcharta.org/2012/05/09/the-cosmological-impact-of-luminous-tev-blazars-iii-implications-for-galaxy-clusters-and-the-formation-of-dwarf-galaxies-replacement/</link>
		<comments>http://voxcharta.org/2012/05/09/the-cosmological-impact-of-luminous-tev-blazars-iii-implications-for-galaxy-clusters-and-the-formation-of-dwarf-galaxies-replacement/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:37:17 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[angular scale]]></category>
		<category><![CDATA[broderick]]></category>
		<category><![CDATA[cluster gas]]></category>
		<category><![CDATA[coupling]]></category>
		<category><![CDATA[dwarf galaxy]]></category>
		<category><![CDATA[entropy]]></category>
		<category><![CDATA[extragalactic background light]]></category>
		<category><![CDATA[galaxy cluster]]></category>
		<category><![CDATA[galaxy group]]></category>
		<category><![CDATA[instabilities]]></category>
		<category><![CDATA[intergalactic medium]]></category>
		<category><![CDATA[merger]]></category>
		<category><![CDATA[plasma beam]]></category>
		<category><![CDATA[power spectrum]]></category>
		<category><![CDATA[redshift]]></category>
		<category><![CDATA[structure formation]]></category>
		<category><![CDATA[subset]]></category>
		<category><![CDATA[tev gamma rays]]></category>
		<category><![CDATA[Zel]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/the-cosmological-impact-of-luminous-tev-blazars-iii-implications-for-galaxy-clusters-and-the-formation-of-dwarf-galaxies-replacement/</guid>
		<description><![CDATA[A subset of blazars emit TeV gamma rays which annihilate and pair produce on the extragalactic background light. We have argued in Broderick et al. (2011, Paper I) that plasma beam instabilities can dissipate the pairs&#8217; energy locally. This heats the intergalactic medium and dramatically increases its entropy after redshift z~2, with important implications for [...]]]></description>
			<content:encoded><![CDATA[<p>A subset of blazars emit TeV gamma rays which annihilate and pair produce on the extragalactic background light. We have argued in Broderick et al. (2011, Paper I) that plasma beam instabilities can dissipate the pairs&#8217; energy locally. This heats the intergalactic medium and dramatically increases its entropy after redshift z~2, with important implications for structure formation: (1) This suggests a scenario for the origin of the cool core (CC)/non-cool core (NCC) bimodality in galaxy clusters and groups. Early forming galaxy groups are unaffected because they can efficiently radiate the additional entropy, developing a CC. However, late forming groups do not have sufficient time to cool before the entropy is gravitationally reprocessed through successive mergers &#8211; counteracting cooling and raising the core entropy further. Hence blazar heating works different than feedback by active galactic nuclei, which balances radiative cooling but is unable to transform CC into NCC clusters due to the weak coupling to the cluster gas. (2) We predict a suppression of the Sunyaev-Zel&#8217;dovich power spectrum on angular scales smaller than 5&#8242; due to the globally reduced central pressure of groups and clusters forming after z~1. (3) Our redshift dependent entropy floor increases the characteristic halo mass below which dwarf galaxies cannot form by a factor of ~10 (50) at mean density (in voids) over that found in models that include photoionization alone. This prevents the formation of late forming dwarf galaxies (z&lt;2) with masses ranging from 10^{10} to 10^{11} M_sun for redshifts z~2 to 0, respectively. This may help resolve the &quot;missing satellite problem&quot; in the Milky Way and the &quot;void phenomenon&quot; of the low observed abundances of dwarf satellites compared to cold dark matter simulations and may bring the observed early star formation histories into agreement with galaxy formation models. (abridged)</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/the-cosmological-impact-of-luminous-tev-blazars-iii-implications-for-galaxy-clusters-and-the-formation-of-dwarf-galaxies-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Post-Periastron Gamma Ray Flare from PSR B1259-63/LS 2883 as a Result of Comptonization of the Cold Pulsar Wind [Replacement]</title>
		<link>http://voxcharta.org/2012/05/09/post-periastron-gamma-ray-flare-from-psr-b1259-63ls-2883-as-a-result-of-comptonization-of-the-cold-pulsar-wind-replacement/</link>
		<comments>http://voxcharta.org/2012/05/09/post-periastron-gamma-ray-flare-from-psr-b1259-63ls-2883-as-a-result-of-comptonization-of-the-cold-pulsar-wind-replacement/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:36:52 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[collaboration]]></category>
		<category><![CDATA[density]]></category>
		<category><![CDATA[dramatic increase]]></category>
		<category><![CDATA[electron positron]]></category>
		<category><![CDATA[element]]></category>
		<category><![CDATA[flare]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[infrared photons]]></category>
		<category><![CDATA[inverse compton]]></category>
		<category><![CDATA[kinetic energy]]></category>
		<category><![CDATA[lorentz factor]]></category>
		<category><![CDATA[proportional increase]]></category>
		<category><![CDATA[psr]]></category>
		<category><![CDATA[radiation]]></category>
		<category><![CDATA[suppression]]></category>
		<category><![CDATA[Telescope]]></category>
		<category><![CDATA[wind zone]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/post-periastron-gamma-ray-flare-from-psr-b1259-63ls-2883-as-a-result-of-comptonization-of-the-cold-pulsar-wind-replacement/</guid>
		<description><![CDATA[We argue that the bright flare of the binary pulsar \object{PSR B1259$-$63/LS2883} detected by the {\it Fermi} Large Area Telescope (LAT), is due to the inverse Compton (IC) scattering of the unshocked electron-positron pulsar wind with a Lorentz factor $\Gamma_0 \approx 10^4$. The combination of two effects both linked to the circumstellar disk (CD), is [...]]]></description>
			<content:encoded><![CDATA[<p>We argue that the bright flare of the binary pulsar \object{PSR B1259$-$63/LS2883} detected by the {\it Fermi} Large Area Telescope (LAT), is due to the inverse Compton (IC) scattering of the unshocked electron-positron pulsar wind with a Lorentz factor $\Gamma_0 \approx 10^4$. The combination of two effects both linked to the circumstellar disk (CD), is a key element in the proposed model. The first effect is related to the impact of the surrounding medium on the termination of the pulsar wind. Inside the disk, the &#8220;early&#8221; termination of the wind results in suppression of its gamma-ray luminosity. When the pulsar escapes the disk, the conditions for termination of the wind undergo significant changes. This would lead to a dramatic increase of the pulsar wind zone, and thus to the proportional increase of the gamma-ray flux. On the other hand, if the parts of the CD disturbed by the pulsar can supply infrared photons of density high enough for efficient Comptonization of the wind, almost the entire kinetic energy of the pulsar wind would be converted to radiation, thus the gamma-ray luminosity of the wind could approach to the level of the pulsar&#8217;s spin-down luminosity as reported by the {\it Fermi} collaboration.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/post-periastron-gamma-ray-flare-from-psr-b1259-63ls-2883-as-a-result-of-comptonization-of-the-cold-pulsar-wind-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Reconstruction efficiency and discovery potential of a Mediterranean neutrino telescope: A simulation study using the Hellenic Open University Reconstruction &amp; Simulation (HOURS) package [Replacement]</title>
		<link>http://voxcharta.org/2012/05/09/reconstruction-efficiency-and-discovery-potential-of-a-mediterranean-neutrino-telescope-a-simulation-study-using-the-hellenic-open-university-reconstruction-simulation-hours-package-replacem/</link>
		<comments>http://voxcharta.org/2012/05/09/reconstruction-efficiency-and-discovery-potential-of-a-mediterranean-neutrino-telescope-a-simulation-study-using-the-hellenic-open-university-reconstruction-simulation-hours-package-replacem/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:34:56 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[angular resolution]]></category>
		<category><![CDATA[atmospheric neutrino]]></category>
		<category><![CDATA[capability]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[energy neutrino]]></category>
		<category><![CDATA[experimental time]]></category>
		<category><![CDATA[gamma ray emission]]></category>
		<category><![CDATA[hadronic interactions]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[muon]]></category>
		<category><![CDATA[neutrino flux]]></category>
		<category><![CDATA[neutrino telescope]]></category>
		<category><![CDATA[open university]]></category>
		<category><![CDATA[point source]]></category>
		<category><![CDATA[reconstruction efficiency]]></category>
		<category><![CDATA[simulation study]]></category>
		<category><![CDATA[software package]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/reconstruction-efficiency-and-discovery-potential-of-a-mediterranean-neutrino-telescope-a-simulation-study-using-the-hellenic-open-university-reconstruction-simulation-hours-package-replacem/</guid>
		<description><![CDATA[We report on the evaluation of the performance of a Mediterranean very large volume neutrino telescope. We present results of our studies concerning the capability of the telescope in detecting/discovering galactic (steady point sources) and extragalactic, transient (Gamma Ray Bursts) high energy neutrino sources as well as measuring ultra high energy diffuse neutrino fluxes. The [...]]]></description>
			<content:encoded><![CDATA[<p>We report on the evaluation of the performance of a Mediterranean very large volume neutrino telescope. We present results of our studies concerning the capability of the telescope in detecting/discovering galactic (steady point sources) and extragalactic, transient (Gamma Ray Bursts) high energy neutrino sources as well as measuring ultra high energy diffuse neutrino fluxes. The neutrino effective area and angular resolution are presented as a function of the neutrino energy, and the background event rate (atmospheric neutrinos and muons) is estimated. The discovery potential of the neutrino telescope is evaluated and the experimental time required for a significant discovery of potential neutrino emitters (known from their gamma ray emission, assumedly produced by hadronic interactions) is estimated. For the simulation we use the HOU Reconstruction &amp; Simulation (HOURS) software package.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/reconstruction-efficiency-and-discovery-potential-of-a-mediterranean-neutrino-telescope-a-simulation-study-using-the-hellenic-open-university-reconstruction-simulation-hours-package-replacem/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A Feasibility Study for the Detection of Supernova Explosions with an Undersea Neutrino Telescope [Replacement]</title>
		<link>http://voxcharta.org/2012/05/09/a-feasibility-study-for-the-detection-of-supernova-explosions-with-an-undersea-neutrino-telescope-replacement/</link>
		<comments>http://voxcharta.org/2012/05/09/a-feasibility-study-for-the-detection-of-supernova-explosions-with-an-undersea-neutrino-telescope-replacement/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:34:47 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[coincidence]]></category>
		<category><![CDATA[electron antineutrino]]></category>
		<category><![CDATA[explosion results]]></category>
		<category><![CDATA[feasibility study]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[neutrino]]></category>
		<category><![CDATA[neutrino telescope]]></category>
		<category><![CDATA[optical module]]></category>
		<category><![CDATA[photomultiplier tube]]></category>
		<category><![CDATA[signature]]></category>
		<category><![CDATA[sn explosion]]></category>
		<category><![CDATA[supernova explosion]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/a-feasibility-study-for-the-detection-of-supernova-explosions-with-an-undersea-neutrino-telescope-replacement/</guid>
		<description><![CDATA[We study the potential of a very large volume underwater Mediterranean neutrino telescope to observe neutrinos from supernova (SN) explosions within our galaxy. The intense neutrino burst emitted in a SN explosion results in a large number of MeV neutrinos inside the instrumented volume of the neutrino telescope that can be detected (mainly) via the [...]]]></description>
			<content:encoded><![CDATA[<p>We study the potential of a very large volume underwater Mediterranean neutrino telescope to observe neutrinos from supernova (SN) explosions within our galaxy. The intense neutrino burst emitted in a SN explosion results in a large number of MeV neutrinos inside the instrumented volume of the neutrino telescope that can be detected (mainly) via the reaction \nu_e-bar + p -&gt; e^+ + n . In this study we simulated the response of the underwater neutrino telescope to the electron antineutrino flux predicted by the Garching model for SN explosions. We assumed that the neutrino telescope comprises 6160 direction sensitive optical modules, each containing 31 small photomultiplier tubes. Multiple coincidences between the photomultiplier tubes of the same optical module are utilized to suppress the noise produced by $^{40}K$ radioactive decays and to establish a statistical significant signature of the SN explosion.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/a-feasibility-study-for-the-detection-of-supernova-explosions-with-an-undersea-neutrino-telescope-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Can A Higgs Portal Dark Matter be Compatible with the Anti-proton Cosmic-ray? [Replacement]</title>
		<link>http://voxcharta.org/2012/05/09/can-a-higgs-portal-dark-matter-be-compatible-with-the-anti-proton-cosmic-ray-replacement/</link>
		<comments>http://voxcharta.org/2012/05/09/can-a-higgs-portal-dark-matter-be-compatible-with-the-anti-proton-cosmic-ray-replacement/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:33:06 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[annihilation]]></category>
		<category><![CDATA[boson]]></category>
		<category><![CDATA[cogent]]></category>
		<category><![CDATA[constraint]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[cross section]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[lep]]></category>
		<category><![CDATA[light higgs]]></category>
		<category><![CDATA[proton flux]]></category>
		<category><![CDATA[relic density]]></category>
		<category><![CDATA[s wave]]></category>
		<category><![CDATA[suppression]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/can-a-higgs-portal-dark-matter-be-compatible-with-the-anti-proton-cosmic-ray-replacement/</guid>
		<description><![CDATA[Recent direct detection experiments of Dark Matter (DM), CoGeNT and DAMA implicate a light DM of a few GeV. Such a light DM would generate a large amount of anti-proton since suppression for anti-proton flux from DM annihilation is ineffective. We discuss whether a light dark matter with mass of 5-15 GeV, which is especially [...]]]></description>
			<content:encoded><![CDATA[<p>Recent direct detection experiments of Dark Matter (DM), CoGeNT and DAMA implicate a light DM of a few GeV. Such a light DM would generate a large amount of anti-proton since suppression for anti-proton flux from DM annihilation is ineffective. We discuss whether a light dark matter with mass of 5-15 GeV, which is especially in favor of the recent experiments reported by CoGeNT, is compatible with the anti-proton no excess in the cosmic-ray. In view of the direct detection of DM and no anti-proton excess in the cosmic-ray both, we show that a Dirac DM is favored than a scalar one since there is no s-wave of the annihilation cross section for the Dirac DM. A large elastic cross section for direct detection can be obtained through the additional light Higgs exchange. We show an allowed region that simultaneously satisfies the DM relic density, the elastic cross section favored by CoGeNT and also the constraint of H_L Z Z coupling of the light Higgs boson by LEP.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/can-a-higgs-portal-dark-matter-be-compatible-with-the-anti-proton-cosmic-ray-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>WISeREP &#8211; An Interactive Supernova Data Repository [Replacement]</title>
		<link>http://voxcharta.org/2012/05/09/wiserep-an-interactive-supernova-data-repository-replacement/</link>
		<comments>http://voxcharta.org/2012/05/09/wiserep-an-interactive-supernova-data-repository-replacement/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:32:51 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[archive data]]></category>
		<category><![CDATA[Caltech]]></category>
		<category><![CDATA[cfa]]></category>
		<category><![CDATA[core collapse]]></category>
		<category><![CDATA[data repository]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[graphical interface]]></category>
		<category><![CDATA[guest users]]></category>
		<category><![CDATA[interactive plots]]></category>
		<category><![CDATA[interactive web]]></category>
		<category><![CDATA[legacy data]]></category>
		<category><![CDATA[massive data sets]]></category>
		<category><![CDATA[meta data]]></category>
		<category><![CDATA[modern tools]]></category>
		<category><![CDATA[palomar]]></category>
		<category><![CDATA[SNe]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[Supernova]]></category>
		<category><![CDATA[UC Berkeley]]></category>
		<category><![CDATA[velocities]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/wiserep-an-interactive-supernova-data-repository-replacement/</guid>
		<description><![CDATA[We have entered an era of massive data sets in astronomy. In particular, the number of supernova (SN) discoveries and classifications has substantially increased over the years from few tens to thousands per year. It is no longer the case that observations of a few prototypical events encapsulate most spectroscopic information about SNe, motivating the [...]]]></description>
			<content:encoded><![CDATA[<p>We have entered an era of massive data sets in astronomy. In particular, the number of supernova (SN) discoveries and classifications has substantially increased over the years from few tens to thousands per year. It is no longer the case that observations of a few prototypical events encapsulate most spectroscopic information about SNe, motivating the development of modern tools to collect, archive, organize and distribute spectra in general, and SN spectra in particular. For this reason we have developed the Weizmann Interactive Supernova data REPository &#8211; WISeREP &#8211; an SQL-based database (DB) with an interactive web-based graphical interface. The system serves as an archive of high quality SN spectra, including both historical (legacy) data as well as data that is accumulated by ongoing modern programs. The archive provides information about objects, their spectra, and related meta-data. Utilizing interactive plots, we provide a graphical interface to visualize data, perform line identification of the major relevant species, determine object redshifts, classify SNe and measure expansion velocities. Guest users may view and download spectra or other data that have been placed in the public domain. Registered users may also view and download data that are proprietary to specific programs with which they are associated. The DB currently holds &gt;8000 spectra, of which &gt;5000 are public; the latter include published spectra from the Palomar Transient Factory, all of the SUSPECT archive, the Caltech-Core-Collapse Program, the CfA SN spectra archive and published spectra from the UC Berkeley SNDB repository. It offers an efficient and convenient way to archive data and share it with colleagues, and we expect that data stored in this way will be easy to access, increasing its visibility, usefulness and scientific impact.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/wiserep-an-interactive-supernova-data-repository-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>VLBA and Chandra Observations of Jets in FRI radio galaxies: Constraints on Jet Evolution [Replacement]</title>
		<link>http://voxcharta.org/2012/05/09/vlba-and-chandra-observations-of-jets-in-fri-radio-galaxies-constraints-on-jet-evolution-replacement/</link>
		<comments>http://voxcharta.org/2012/05/09/vlba-and-chandra-observations-of-jets-in-fri-radio-galaxies-constraints-on-jet-evolution-replacement/#comments</comments>
		<pubDate>Thu, 10 May 2012 00:31:21 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[archival data]]></category>
		<category><![CDATA[chandra data]]></category>
		<category><![CDATA[chandra observation]]></category>
		<category><![CDATA[core]]></category>
		<category><![CDATA[fri]]></category>
		<category><![CDATA[high frequency]]></category>
		<category><![CDATA[jet evolution]]></category>
		<category><![CDATA[jet radius]]></category>
		<category><![CDATA[jet sources]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[peak intensity]]></category>
		<category><![CDATA[polarization]]></category>
		<category><![CDATA[poynting]]></category>
		<category><![CDATA[radio galaxy]]></category>
		<category><![CDATA[ray jets]]></category>
		<category><![CDATA[ugc]]></category>
		<category><![CDATA[very long baseline array]]></category>
		<category><![CDATA[vlba]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/09/vlba-and-chandra-observations-of-jets-in-fri-radio-galaxies-constraints-on-jet-evolution-replacement/</guid>
		<description><![CDATA[(ABRIDGED) We present here the results from new Very Long Baseline Array observations at 1.6 and 5 GHz of 19 galaxies of a complete sample of 21 UGC FRI radio galaxies. New Chandra data of two sources, viz., UGC00408 and UGC08433, are combined with the Chandra archival data of 13 sources. The 5 GHz observations [...]]]></description>
			<content:encoded><![CDATA[<p>(ABRIDGED) We present here the results from new Very Long Baseline Array observations at 1.6 and 5 GHz of 19 galaxies of a complete sample of 21 UGC FRI radio galaxies. New Chandra data of two sources, viz., UGC00408 and UGC08433, are combined with the Chandra archival data of 13 sources. The 5 GHz observations of ten &#8220;core-jet&#8221; sources are polarization-sensitive, while the 1.6 GHz observations constitute second epoch total intensity observations of nine &#8220;core-only&#8221; sources. Polarized emission is detected in the jets of seven sources at 5 GHz, but the cores are essentially unpolarized, except in M87. Polarization is detected at the jet edges in several sources, and the inferred magnetic field is primarily aligned with the jet direction. This could be indicative of magnetic field &#8220;shearing&#8221; due to jet-medium interaction, or the presence of helical magnetic fields. The jet peak intensity $I_\nu$ falls with distance $d$ from the core, following the relation, $I_\nu\propto d^a$, where $a$ is typically -1.5. Assuming that adiabatic expansion losses are primarily responsible for the jet intensity &#8220;dimming&#8221;, two limiting cases are considered: [1] the jet has a constant speed on parsec-scales and is expanding gradually such that the jet radius $r\propto d^0.4$; this expansion is however unobservable in the laterally unresolved jets at 5 GHz, and [2] the jet is cylindrical and is accelerating on parsec-scales. Accelerating parsec-scale jets are consistent with the phenomenon of &#8220;magnetic driving&#8221; in Poynting flux dominated jets. Chandra observations of 15 UGC FRIs detect X-ray jets in nine of them. The high frequency of occurrence of X-ray jets in this complete sample suggests that they are a signature of a ubiquitous process in FRI jets.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/09/vlba-and-chandra-observations-of-jets-in-fri-radio-galaxies-constraints-on-jet-evolution-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>The dynamics, appearance and demographics of relativistic jets triggered by tidal disruption of stars in quiescent supermassive black holes</title>
		<link>http://voxcharta.org/2012/05/08/the-dynamics-appearance-and-demographics-of-relativistic-jets-triggered-by-tidal-disruption-of-stars-in-quiescent-supermassive-black-holes/</link>
		<comments>http://voxcharta.org/2012/05/08/the-dynamics-appearance-and-demographics-of-relativistic-jets-triggered-by-tidal-disruption-of-stars-in-quiescent-supermassive-black-holes/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:47:31 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion disk]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[density stratification]]></category>
		<category><![CDATA[disruption]]></category>
		<category><![CDATA[flare]]></category>
		<category><![CDATA[galactic nuclei]]></category>
		<category><![CDATA[hydrodynamic model]]></category>
		<category><![CDATA[hydrodynamic simulation]]></category>
		<category><![CDATA[instabilities]]></category>
		<category><![CDATA[interstellar medium]]></category>
		<category><![CDATA[light curve]]></category>
		<category><![CDATA[number density]]></category>
		<category><![CDATA[propagation]]></category>
		<category><![CDATA[relativistic jet]]></category>
		<category><![CDATA[supermassive black hole]]></category>
		<category><![CDATA[symmetry]]></category>
		<category><![CDATA[tidal disruption]]></category>
		<category><![CDATA[transitioning]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/the-dynamics-appearance-and-demographics-of-relativistic-jets-triggered-by-tidal-disruption-of-stars-in-quiescent-supermassive-black-holes/</guid>
		<description><![CDATA[We examine the consequences of a model in which relativistic jets can be triggered in quiescent massive black holes when a geometrically thick and hot accretion disk forms as a result of the tidal disruption of a star. To estimate the power, thrust and lifetime of the jet, we use the mass accretion history onto [...]]]></description>
			<content:encoded><![CDATA[<p>We examine the consequences of a model in which relativistic jets can be triggered in quiescent massive black holes when a geometrically thick and hot accretion disk forms as a result of the tidal disruption of a star. To estimate the power, thrust and lifetime of the jet, we use the mass accretion history onto the black hole as calculated by detailed hydrodynamic simulations of the tidal disruption of stars. We go on to determine the states of the interstellar medium in various types of quiescent galactic nuclei, and describe how this external matter can affect jets propagating through it. We use this information, together with a two-dimensional hydrodynamic model of the structure of the relativistic flow, to study the dynamics of the jet, the propagation of which is regulated by the density stratification of the environment and by its injection history. The breaking of symmetry involved in transitioning from one to two dimensions is crucial and leads to qualitatively new phenomena. Many of the observed properties of the Swift 1644+57/GRB 110328A event can be understood as resulting from accretion onto and jets driven by a $10^6 M_\odot$ central mass black hole following the disruption of sun-like star. With the inclusion of a stochastic contribution to the luminosity due to variations in the feeding rate driven by instabilities near the tidal radius, we find that our model can explain the X-ray light curve without invoking a rarely-occurring deep encounter. In conjunction with the number density of black holes in the local universe, we hypothesize that the conditions required to produce the Swift event are not anomalous, but are in fact representative of the jet-driven flare population arising from tidal disruptions.   [abridged]</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/the-dynamics-appearance-and-demographics-of-relativistic-jets-triggered-by-tidal-disruption-of-stars-in-quiescent-supermassive-black-holes/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Extra U(1) as natural source of a monochromatic gamma ray line [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/08/extra-u1-as-natural-source-of-a-monochromatic-gamma-ray-line-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/08/extra-u1-as-natural-source-of-a-monochromatic-gamma-ray-line-cross-listing/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:45:34 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[chern]]></category>
		<category><![CDATA[coupling]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[gauge]]></category>
		<category><![CDATA[gev]]></category>
		<category><![CDATA[heavy fermions]]></category>
		<category><![CDATA[line extensions]]></category>
		<category><![CDATA[natural source]]></category>
		<category><![CDATA[natural values]]></category>
		<category><![CDATA[standard model]]></category>
		<category><![CDATA[Telescope]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/extra-u1-as-natural-source-of-a-monochromatic-gamma-ray-line-cross-listing/</guid>
		<description><![CDATA[Extensions of the Standard Model with an extra U&#8217;(1) abelian group generically generate terms coming from loops of heavy fermions, leading to three gauge boson couplings, in particular Z&#8217;Z gamma. We show that WMAP data constrains the gauge coupling of the group g_D to values comparable with the electro-weak ones, rather independently of the mass [...]]]></description>
			<content:encoded><![CDATA[<p>Extensions of the Standard Model with an extra U&#8217;(1) abelian group generically generate terms coming from loops of heavy fermions, leading to three gauge boson couplings, in particular Z&#8217;Z gamma. We show that WMAP data constrains the gauge coupling of the group g_D to values comparable with the electro-weak ones, rather independently of the mass of Z&#8217;. Moreover, the model predicts a monochromatic gamma-ray line which can fit a 130 GeV signal at the FERMI telescope for natural values of the Chern-Simons terms and a dark matter mass around 144.5 GeV.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/extra-u1-as-natural-source-of-a-monochromatic-gamma-ray-line-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>On the thermodynamic self-similarity of the nearest, most relaxed, giant ellipticals</title>
		<link>http://voxcharta.org/2012/05/08/on-the-thermodynamic-self-similarity-of-the-nearest-most-relaxed-giant-ellipticals/</link>
		<comments>http://voxcharta.org/2012/05/08/on-the-thermodynamic-self-similarity-of-the-nearest-most-relaxed-giant-ellipticals/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:43:25 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[agn activity]]></category>
		<category><![CDATA[energy balance]]></category>
		<category><![CDATA[entropy]]></category>
		<category><![CDATA[giant elliptical galaxy]]></category>
		<category><![CDATA[giant ellipticals]]></category>
		<category><![CDATA[hot x]]></category>
		<category><![CDATA[inner regions]]></category>
		<category><![CDATA[innermost region]]></category>
		<category><![CDATA[interstellar medium]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[mass profiles]]></category>
		<category><![CDATA[massive black hole]]></category>
		<category><![CDATA[relativistic jet]]></category>
		<category><![CDATA[self similarity]]></category>
		<category><![CDATA[thermodynamic profiles]]></category>
		<category><![CDATA[thermodynamic properties]]></category>
		<category><![CDATA[time distribution]]></category>
		<category><![CDATA[time scale]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/on-the-thermodynamic-self-similarity-of-the-nearest-most-relaxed-giant-ellipticals/</guid>
		<description><![CDATA[We present detailed spatially resolved measurements of the thermodynamic properties of the X-ray emitting gas in the inner regions of the five nearest, X-ray and optically brightest, and most X-ray morphologically relaxed giant elliptical galaxies known. Beyond the innermost region at r &#62; 1 kpc, and out to r ~ 6 kpc, the density, pressure, [...]]]></description>
			<content:encoded><![CDATA[<p>We present detailed spatially resolved measurements of the thermodynamic properties of the X-ray emitting gas in the inner regions of the five nearest, X-ray and optically brightest, and most X-ray morphologically relaxed giant elliptical galaxies known. Beyond the innermost region at r &gt; 1 kpc, and out to r ~ 6 kpc, the density, pressure, entropy, and cooling time distributions for the X-ray emitting gas follow remarkably similar, simple, power-law like distributions. Notably, the entropy profiles follow a power-law form, with an index 0.92-1.07. The cumulative hot X-ray emitting gas mass profiles and the gas-mass to stellar-light ratios of all five galaxies are also similar. Overall the observed similarity of the thermodynamic profiles in this radial range argues that, in these systems, relativistic jets heat the gas at a similar rate averaged over time scales longer than the cooling time of 10^8 yr. These jets are powered by accretion from the hot gas, or material entrained within it, onto the central super-massive black hole. This jet heating creates an energy balance where heating and cooling are in equilibrium, keeping the hot galactic atmospheres in a `steady-state&#8217;. Within r &lt; 1 kpc, this similarity breaks down: the observed entropy profiles show well resolved flattening and the values differ from system to system substantially. The accretion rate onto the black hole and the AGN activity, heating the interstellar medium, must therefore vary significantly on time scales shorter than the cooling time of 10^7 &#8211; 10^8 yr.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/on-the-thermodynamic-self-similarity-of-the-nearest-most-relaxed-giant-ellipticals/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Broad-band spectral analysis of the Galactic Ridge X-ray Emission</title>
		<link>http://voxcharta.org/2012/05/08/broad-band-spectral-analysis-of-the-galactic-ridge-x-ray-emission/</link>
		<comments>http://voxcharta.org/2012/05/08/broad-band-spectral-analysis-of-the-galactic-ridge-x-ray-emission/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:43:16 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[broad band]]></category>
		<category><![CDATA[chandra satellite]]></category>
		<category><![CDATA[faint point]]></category>
		<category><![CDATA[galactic bulge]]></category>
		<category><![CDATA[high spatial resolution]]></category>
		<category><![CDATA[keV]]></category>
		<category><![CDATA[number density]]></category>
		<category><![CDATA[plasma temperature]]></category>
		<category><![CDATA[point source]]></category>
		<category><![CDATA[ray emission]]></category>
		<category><![CDATA[ray sources]]></category>
		<category><![CDATA[spectral analysis]]></category>
		<category><![CDATA[spectral components]]></category>
		<category><![CDATA[spectral model]]></category>
		<category><![CDATA[spectroscopic]]></category>
		<category><![CDATA[suzaku]]></category>
		<category><![CDATA[thermal emission]]></category>
		<category><![CDATA[white dwarf]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/broad-band-spectral-analysis-of-the-galactic-ridge-x-ray-emission/</guid>
		<description><![CDATA[Detailed spectral analysis of the Galactic X-ray background emission, or the Galactic Ridge X-ray Emission (GRXE), is presented. To study the origin of the emission, broad-band and high-quality GRXE spectra were produced from 18 pointing observations with Suzaku in the Galactic bulge region, with the total exposure of 1 Ms. The spectra were successfully fitted [...]]]></description>
			<content:encoded><![CDATA[<p>Detailed spectral analysis of the Galactic X-ray background emission, or the Galactic Ridge X-ray Emission (GRXE), is presented. To study the origin of the emission, broad-band and high-quality GRXE spectra were produced from 18 pointing observations with Suzaku in the Galactic bulge region, with the total exposure of 1 Ms. The spectra were successfully fitted by a sum of two major spectral components; a spectral model of magnetic accreting white dwarfs with a mass of 0.66 (0.59-0.75) solar, and a softer optically-thin thermal emission with a plasma temperature of 1.2-1.5 keV which is attributable to coronal X-ray sources.   When combined with previous studies which employed high spatial resolution of the Chandra satellite (e.g. Revnivtsev et al. 2009, Nature), the present spectroscopic result gives another strong support to a scenario that the GRXE is essentially an assembly of numerous discrete faint X-ray stars.   The detected GRXE flux in the hard X-ray band was used to estimate the number density of the unresolved hard X-ray sources. When integrated over a luminosity range of ~10^30-10^34 erg/s, the result is consistent with a value which was reported previously by directly resolving faint point sources.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/broad-band-spectral-analysis-of-the-galactic-ridge-x-ray-emission/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A cosmic ray cocoon along the X-ray jet of M87?</title>
		<link>http://voxcharta.org/2012/05/08/a-cosmic-ray-cocoon-along-the-x-ray-jet-of-m87/</link>
		<comments>http://voxcharta.org/2012/05/08/a-cosmic-ray-cocoon-along-the-x-ray-jet-of-m87/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:40:00 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[ambient medium]]></category>
		<category><![CDATA[chandra x ray]]></category>
		<category><![CDATA[cocoon]]></category>
		<category><![CDATA[cosmic ray]]></category>
		<category><![CDATA[dynamic effect]]></category>
		<category><![CDATA[galaxy m87]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[intensity]]></category>
		<category><![CDATA[interaction]]></category>
		<category><![CDATA[kpc]]></category>
		<category><![CDATA[m87 jet]]></category>
		<category><![CDATA[magnetic field structure]]></category>
		<category><![CDATA[morphological structure]]></category>
		<category><![CDATA[polarization]]></category>
		<category><![CDATA[radio galaxy]]></category>
		<category><![CDATA[relativistic jet]]></category>
		<category><![CDATA[side boundaries]]></category>
		<category><![CDATA[signature]]></category>
		<category><![CDATA[velocity gradient]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/a-cosmic-ray-cocoon-along-the-x-ray-jet-of-m87/</guid>
		<description><![CDATA[Relativistic jets propagating through an ambient medium must produce some observational effects along their side boundaries because of interactions across the large velocity gradient. One possible effect of such an interaction would be a sheared magnetic field structure at the jet boundaries, leading to a characteristic radio polarization pattern. As proposed by Ostrowski, another effect [...]]]></description>
			<content:encoded><![CDATA[<p>Relativistic jets propagating through an ambient medium must produce some observational effects along their side boundaries because of interactions across the large velocity gradient. One possible effect of such an interaction would be a sheared magnetic field structure at the jet boundaries, leading to a characteristic radio polarization pattern. As proposed by Ostrowski, another effect can come from the generation of a high energy cosmic ray component at the boundary, producing dynamic effects on the medium surrounding the jet and forming a cocoon dominated by cosmic rays with a decreased thermal gas emissivity. We selected this process for our first attempt to look for the effects of this type of interaction. We analyzed the Chandra X-ray data for the radio galaxy M87 in order to verify if the expected regions of diminished emissivity may be present near the spectacular X-ray jet in this source. The detailed analysis of the data, merged from 42 separate observations, shows signatures of lower emissivity surrounding the jet. In particular we detect an intensity dip along the part of the jet, which would be approximately 150 pc x 2 kpc in size, if situated along the jet which is inclined toward us. Due to a highly non-uniform X-ray background in the central region we are not able to claim the discovery of a cosmic ray cocoon around the M87 jet: we only have demonstrated that the data show morphological structures which could be accounted for if a cosmic ray cocoon exists.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/a-cosmic-ray-cocoon-along-the-x-ray-jet-of-m87/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Wind braking of magnetars</title>
		<link>http://voxcharta.org/2012/05/08/wind-braking-of-magnetars/</link>
		<comments>http://voxcharta.org/2012/05/08/wind-braking-of-magnetars/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:39:16 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[correlation]]></category>
		<category><![CDATA[decay]]></category>
		<category><![CDATA[dipole field]]></category>
		<category><![CDATA[energetics]]></category>
		<category><![CDATA[fundamental plane]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[magnetar]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetism]]></category>
		<category><![CDATA[Measurement]]></category>
		<category><![CDATA[nebula]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[radio emission]]></category>
		<category><![CDATA[repeater]]></category>
		<category><![CDATA[sgrs]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/wind-braking-of-magnetars/</guid>
		<description><![CDATA[Anomalous X-ray pulsars (AXPs) and soft gamma-ray repeaters (SGRs) are magnetar candidates. During their studies, the magnetic dipole braking mechanism is often assumed. This will result in a high surface dipole field for most AXPs and SGRs. It will also bring several problems challenging the magnetar interpretation. Alternatively, it is possible that AXPs and SGRs [...]]]></description>
			<content:encoded><![CDATA[<p>Anomalous X-ray pulsars (AXPs) and soft gamma-ray repeaters (SGRs) are magnetar candidates. During their studies, the magnetic dipole braking mechanism is often assumed. This will result in a high surface dipole field for most AXPs and SGRs. It will also bring several problems challenging the magnetar interpretation. Alternatively, it is possible that AXPs and SGRs are braked down by a particle wind which also originates from magnetic field decay. In the wind braking scenario, magnetars are neutron stars with strong multipole field. A strong dipole field is no longer required. Recent challenging observations of magnetars may be explained naturally in the wind braking scenario: (1) The supernova energetics of those associated with magnetars are of normal value; (2) The non-detection in Fermi observations of magnetars; (3) The problem posed by the low-magnetic field soft gamma-ray repeater; (4) The relation between magnetars and high magnetic field pulsars ; (5) A decreasing period derivative during magnetar outbursts etc. For magnetars with $L_{\rm x}&lt;-\dot{E}_{\rm rot}$, they may still be magnetic dipole braking. This may explain the &quot;fundamental plane&quot; of magnetar radio emissions. A magnetism-powered (instead of rotation-powered) pulsar wind nebula will be one of the consequences of wind braking. For a magnetism-powered pulsar wind nebula, we should see a correlation between the nebula luminosity and the magnetar luminosity. This may be the case of the extended emission around AXP 1E 1547.0-5408. A braking index different from three is also calculated. Future braking index measurement of a magnetar may tell us whether magnetars are wind braking or magnetic dipole braking.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/wind-braking-of-magnetars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Exploring the FRI/FRII radio dichotomy with the Fermi satellite</title>
		<link>http://voxcharta.org/2012/05/08/exploring-the-frifrii-radio-dichotomy-with-the-fermi-satellite/</link>
		<comments>http://voxcharta.org/2012/05/08/exploring-the-frifrii-radio-dichotomy-with-the-fermi-satellite/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:36:41 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[dichotomy]]></category>
		<category><![CDATA[emitters]]></category>
		<category><![CDATA[energy photons]]></category>
		<category><![CDATA[fri]]></category>
		<category><![CDATA[frii]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[gamma ray photons]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[localization]]></category>
		<category><![CDATA[power radio]]></category>
		<category><![CDATA[quasar]]></category>
		<category><![CDATA[radio core]]></category>
		<category><![CDATA[radio galaxy]]></category>
		<category><![CDATA[radio lobes]]></category>
		<category><![CDATA[satellite]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/exploring-the-frifrii-radio-dichotomy-with-the-fermi-satellite/</guid>
		<description><![CDATA[Misaligned Active Galactic Nuclei (MAGNs), i.e., radio galaxies and quasars with the jet not directly pointing at the observer, are a new class of GeV emitters. In low power radio galaxies (i.e., FRIs), gamma-rays are mainly produced in compact jet regions, although in at least one case, Centaurus A, high energy photons from the radio [...]]]></description>
			<content:encoded><![CDATA[<p>Misaligned Active Galactic Nuclei (MAGNs), i.e., radio galaxies and quasars with the jet not directly pointing at the observer, are a new class of GeV emitters. In low power radio galaxies (i.e., FRIs), gamma-rays are mainly produced in compact jet regions, although in at least one case, Centaurus A, high energy photons from the radio lobes have been also observed. The first localization of the gamma-ray dissipation zone in a high power radio galaxy (i.e., FRII) excludes major contributions from extended regions. The study of the FRII source 3C111 indicates that gamma-ray photons are produced in the jet. The site, coincident with the radio core, is estimated to be at a distance &lt;~0.3 pc from the black hole. Although the place where high energy photons are produced is probably similar in FRIs and FRIIs, high power radio galaxies are rarer in the GeV sky. Our study of all the radio sources belonging to four complete radio catalogs (3CR, 3CRR, MS4, 2Jy) disfavors the idea that the paucity of FRIIs is due to their larger distance (and therefore to their faintness) and supports other possibilities, pointing to beaming/jet structural differences between FRIs and FRIIs.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/exploring-the-frifrii-radio-dichotomy-with-the-fermi-satellite/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<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>X-Ray view of Misaligned AGNs</title>
		<link>http://voxcharta.org/2012/05/08/x-ray-view-of-misaligned-agns/</link>
		<comments>http://voxcharta.org/2012/05/08/x-ray-view-of-misaligned-agns/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:36:21 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[fri]]></category>
		<category><![CDATA[frii]]></category>
		<category><![CDATA[mechanisms]]></category>
		<category><![CDATA[misaligned]]></category>
		<category><![CDATA[radio galaxy]]></category>
		<category><![CDATA[radio source]]></category>
		<category><![CDATA[ray analysis]]></category>
		<category><![CDATA[ray view]]></category>
		<category><![CDATA[satellite]]></category>
		<category><![CDATA[small group]]></category>
		<category><![CDATA[spectrum radio]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/x-ray-view-of-misaligned-agns/</guid>
		<description><![CDATA[The Fermi-LAT satellite has recently discovered a small group of radio galaxies and steep spectrum radio sources: the misaligned AGNs (MAGNs) sample. We present the X-ray analysis of all the sources of this sample (7 FRIs and 3 FRIIs) with a firm GeV association. This study supports the idea that FRIIs host more efficient accretion [...]]]></description>
			<content:encoded><![CDATA[<p>The Fermi-LAT satellite has recently discovered a small group of radio galaxies and steep spectrum radio sources: the misaligned AGNs (MAGNs) sample. We present the X-ray analysis of all the sources of this sample (7 FRIs and 3 FRIIs) with a firm GeV association. This study supports the idea that FRIIs host more efficient accretion mechanisms (m_dot &gt;0.1) than FRIs (m_dot &lt;0.003). Furthermore, in objects with high accretion rates the Broad Line Regions appear to be very active zones where, in addition to optical lines, the fluorescence iron Kalpha feature at 6.4 keV is also produced. It seems that the FRII jets propagate in an environment very rich in photons, explaining, at least at zeroth order, why the External Compton is the preferred mechanism to produce gamma-rays. In FRIs, where also the iron line is difficult to be detected, the paucity of photons in the circumnuclear ambient seems to favor the Synchrotron Self Compton process.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/x-ray-view-of-misaligned-agns/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Comparison of ejection events in the jet and accretion disc outflows in 3C 111</title>
		<link>http://voxcharta.org/2012/05/08/comparison-of-ejection-events-in-the-jet-and-accretion-disc-outflows-in-3c-111/</link>
		<comments>http://voxcharta.org/2012/05/08/comparison-of-ejection-events-in-the-jet-and-accretion-disc-outflows-in-3c-111/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:35:01 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion disc]]></category>
		<category><![CDATA[analogue]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[dips]]></category>
		<category><![CDATA[equilibrium]]></category>
		<category><![CDATA[galaxy 3c]]></category>
		<category><![CDATA[global flow]]></category>
		<category><![CDATA[knot]]></category>
		<category><![CDATA[light curve]]></category>
		<category><![CDATA[line radio]]></category>
		<category><![CDATA[momentum flux]]></category>
		<category><![CDATA[order of magnitude]]></category>
		<category><![CDATA[outflow]]></category>
		<category><![CDATA[radiation pressure]]></category>
		<category><![CDATA[radio galaxy]]></category>
		<category><![CDATA[ray observations]]></category>
		<category><![CDATA[relativistic outflows]]></category>
		<category><![CDATA[stratification]]></category>
		<category><![CDATA[ufos]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/comparison-of-ejection-events-in-the-jet-and-accretion-disc-outflows-in-3c-111/</guid>
		<description><![CDATA[We present a comparison of the parameters of accretion disc outflows and the jet of the broad-line radio galaxy 3C 111 on sub-pc scales. We make use of published X-ray observations of ultra-fast outflows (UFOs) and new 43GHz VLBA images to track the jet knots ejection. We find that the superluminal jet coexists with the [...]]]></description>
			<content:encoded><![CDATA[<p>We present a comparison of the parameters of accretion disc outflows and the jet of the broad-line radio galaxy 3C 111 on sub-pc scales. We make use of published X-ray observations of ultra-fast outflows (UFOs) and new 43GHz VLBA images to track the jet knots ejection. We find that the superluminal jet coexists with the mildly relativistic outflows on sub-pc scales, possibly indicating a transverse stratification of a global flow. The two are roughly in pressure equilibrium, with the UFOs potentially providing additional support for the initial jet collimation. The UFOs are much more massive than the jet, but their kinetic power is probably about an order of magnitude lower, at least for the observations considered here. However, their momentum flux is equivalent and both of them are powerful enough to exert a concurrent feedback impact on the surrounding environment. A link between these components is naturally predicted in the context of MHD models for jet/outflow formation. However, given the high radiation throughput of AGNs, radiation pressure should also be taken into account. From the comparison with the long-term 2-10keV RXTE light curve we find that the UFOs are preferentially detected during periods of increasing flux. We also find the possibility to place the UFOs within the known X-ray dips-jet ejection cycles, which has been shown to be a strong proof of the disc-jet connection, in analogue with stellar-mass black holes. However, given the limited number of observations presently available, these relations are only tentative and additional spectral monitoring is needed to test them conclusively.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/comparison-of-ejection-events-in-the-jet-and-accretion-disc-outflows-in-3c-111/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The X-ray behaviour of Fermi/LAT pulsars</title>
		<link>http://voxcharta.org/2012/05/08/the-x-ray-behaviour-of-fermilat-pulsars/</link>
		<comments>http://voxcharta.org/2012/05/08/the-x-ray-behaviour-of-fermilat-pulsars/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:34:37 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Galactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[appendix]]></category>
		<category><![CDATA[chapter 3]]></category>
		<category><![CDATA[comprehension]]></category>
		<category><![CDATA[current status]]></category>
		<category><![CDATA[detailed description]]></category>
		<category><![CDATA[energetics]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[multiwavelength observations]]></category>
		<category><![CDATA[nebula]]></category>
		<category><![CDATA[neutron star]]></category>
		<category><![CDATA[population]]></category>
		<category><![CDATA[proposal]]></category>
		<category><![CDATA[proprieties]]></category>
		<category><![CDATA[pulsars]]></category>
		<category><![CDATA[ray observations]]></category>
		<category><![CDATA[spectra]]></category>
		<category><![CDATA[synergy]]></category>
		<category><![CDATA[thesis]]></category>
		<category><![CDATA[x ray]]></category>
		<category><![CDATA[zoo]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/the-x-ray-behaviour-of-fermilat-pulsars/</guid>
		<description><![CDATA[More than 40 years after the discovery of Isolated Neutron Stars, the comprehension of their physics is still rather poor. This thesis is based on a program of multiwavelength observations of pulsars which yielded new and important pieces of information about the overall proprieties of this class of sources. The thesis is organized as follows: [...]]]></description>
			<content:encoded><![CDATA[<p>More than 40 years after the discovery of Isolated Neutron Stars, the comprehension of their physics is still rather poor. This thesis is based on a program of multiwavelength observations of pulsars which yielded new and important pieces of information about the overall proprieties of this class of sources. The thesis is organized as follows: &#8211; In chapter 1 we give a very brief overview of the current status of the understanding of Isolated Neutron Stars. We also talk about the Fermi revolution that occurred in the last three years, focusing on the Fermi contribution to the knowledge of neutron stars. Then, we describe the results led by the synergy between X-ray and gamma-ray bands. &#8211; In chapter 2 we report two of our published papers containing the surprising results we obtained for two different radio-quiet pulsars. Such neutron stars, J0007+7303 and J0357+3205, can be considered &#8220;extreme&#8221; in the Fermi pulsars&#8217; zoo due to their energetics and ages. Both the X-ray observations and analyses are very different so that they can be considered as the standing-up examples of all the following analyses. &#8211; In chapter 3 we describe the analysis we done in the X-ray band and briefly report the obtained spectra of each pulsar and its nebula, if present. Then, we study the X-ray and gamma-ray pulsars&#8217; luminosities as a function of their rotational energies and ages in order to find any relationship between these values and any difference between the two populations of radio-quiet and radio-loud pulsars. &#8211; In chapter 4 we report the &#8220;identity card&#8221; of all Fermi pulsars, the detailed description of the analyses done and results obtained for each pulsar. Finally, in appendix we report our accepted proposals of the most significative X-ray observations used in this thesis plus the article on the X-ray behaviour of Fermi/LAT pulsars we published on the Astrophyisical Journal.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/the-x-ray-behaviour-of-fermilat-pulsars/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Diskoseismology and QPOs Confront Black Hole Spin</title>
		<link>http://voxcharta.org/2012/05/08/diskoseismology-and-qpos-confront-black-hole-spin/</link>
		<comments>http://voxcharta.org/2012/05/08/diskoseismology-and-qpos-confront-black-hole-spin/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:34:06 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[absence]]></category>
		<category><![CDATA[accretion disk]]></category>
		<category><![CDATA[angular momentum]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[circular orbit]]></category>
		<category><![CDATA[continuum]]></category>
		<category><![CDATA[determinations]]></category>
		<category><![CDATA[models]]></category>
		<category><![CDATA[oscillation]]></category>
		<category><![CDATA[periodic oscillation]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/diskoseismology-and-qpos-confront-black-hole-spin/</guid>
		<description><![CDATA[We compare the determinations of the angular momentum of stellar mass black holes via the continuum and line methods with those from diskoseismology. The assumption that is being tested is that one of the QPOs (quasi-periodic oscillations) in each binary X-ray source is produced by the fundamental g-mode. This should be the most robust and [...]]]></description>
			<content:encoded><![CDATA[<p>We compare the determinations of the angular momentum of stellar mass black holes via the continuum and line methods with those from diskoseismology. The assumption that is being tested is that one of the QPOs (quasi-periodic oscillations) in each binary X-ray source is produced by the fundamental g-mode. This should be the most robust and visible normal mode of oscillation of the accretion disk, and therefore its absence should rule out diskoseismology as the origin of QPOs. The comparisons are consistent with the second highest frequency QPO being produced by this g-mode, but are not consistent with models in which the QPO frequency is that of the innermost stable circular orbit.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/diskoseismology-and-qpos-confront-black-hole-spin/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Clustering of X-Ray-Selected AGN [Replacement]</title>
		<link>http://voxcharta.org/2012/05/08/clustering-of-x-ray-selected-agn-replacement/</link>
		<comments>http://voxcharta.org/2012/05/08/clustering-of-x-ray-selected-agn-replacement/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:32:54 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[AGN]]></category>
		<category><![CDATA[cxb]]></category>
		<category><![CDATA[dark matter halo]]></category>
		<category><![CDATA[disk instability]]></category>
		<category><![CDATA[formalism]]></category>
		<category><![CDATA[galaxy evolution]]></category>
		<category><![CDATA[galaxy group]]></category>
		<category><![CDATA[galaxy merger]]></category>
		<category><![CDATA[key result]]></category>
		<category><![CDATA[model prediction]]></category>
		<category><![CDATA[observational data]]></category>
		<category><![CDATA[qso]]></category>
		<category><![CDATA[ray observatory]]></category>
		<category><![CDATA[ray sky]]></category>
		<category><![CDATA[ray sources]]></category>
		<category><![CDATA[spatial distribution]]></category>
		<category><![CDATA[spatial structure]]></category>
		<category><![CDATA[tidal disruption]]></category>
		<category><![CDATA[two generations]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/clustering-of-x-ray-selected-agn-replacement/</guid>
		<description><![CDATA[The study of the angular and spatial structure of the X-ray sky has been under investigation since the times of the Einstein X-ray Observatory. This topic has fascinated more than two generations of scientists and slowly unveiled an unexpected scenario regarding the consequences of the angular and spatial distribution of X-ray sources. It was first [...]]]></description>
			<content:encoded><![CDATA[<p>The study of the angular and spatial structure of the X-ray sky has been under investigation since the times of the Einstein X-ray Observatory. This topic has fascinated more than two generations of scientists and slowly unveiled an unexpected scenario regarding the consequences of the angular and spatial distribution of X-ray sources. It was first established from the clustering of sources making the CXB that the source spatial distribution resembles that of optical QSO. It then it became evident that the distribution of X-ray AGN in the Universe was strongly reflecting that of Dark Matter. In particular one of the key result is that X-ray AGN are hosted by Dark Matter Halos of mass similar to that of galaxy groups. This result, together with model predictions, has lead to the hypothesis that galaxy mergers may constitute the main AGN triggering mechanism. However detailed analysis of observational data, acquired with modern telescopes, and the use of the new Halo Occupation formalism has revealed that the triggering of an AGN could also be attributed to phenomena like tidal disruption or disk instability, and to galaxy evolution. This paper reviews results from 1988 to 2011 in the field of X-ray selected AGN clustering.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/clustering-of-x-ray-selected-agn-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Numerical Simulations of Optically Thick Accretion onto a Black Hole &#8211; I. Spherical Case [Replacement]</title>
		<link>http://voxcharta.org/2012/05/08/numerical-simulations-of-optically-thick-accretion-onto-a-black-hole-i-spherical-case-replacement/</link>
		<comments>http://voxcharta.org/2012/05/08/numerical-simulations-of-optically-thick-accretion-onto-a-black-hole-i-spherical-case-replacement/#comments</comments>
		<pubDate>Wed, 09 May 2012 00:32:14 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[Instrumentation and Methods]]></category>
		<category><![CDATA[Replacements]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion disk]]></category>
		<category><![CDATA[accretion rates]]></category>
		<category><![CDATA[analytic solution]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[bondi]]></category>
		<category><![CDATA[bremsstrahlung]]></category>
		<category><![CDATA[convergence rate]]></category>
		<category><![CDATA[eddington luminosity]]></category>
		<category><![CDATA[hole accretion]]></category>
		<category><![CDATA[inflow]]></category>
		<category><![CDATA[numerical simulation]]></category>
		<category><![CDATA[opacity]]></category>
		<category><![CDATA[orders of magnitude]]></category>
		<category><![CDATA[radiation transport]]></category>
		<category><![CDATA[radiative processes]]></category>
		<category><![CDATA[realistic simulation]]></category>
		<category><![CDATA[shock tube]]></category>
		<category><![CDATA[solid surface]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/08/numerical-simulations-of-optically-thick-accretion-onto-a-black-hole-i-spherical-case-replacement/</guid>
		<description><![CDATA[Modeling the radiation generated by accreting matter is an important step towards realistic simulations of black hole accretion disks, especially at high accretion rates. To this end, we have recently added radiation transport to the existing general relativistic magnetohydrodynamic code, Cosmos++. However, before attempting to model radiative accretion disks, we have tested the new code [...]]]></description>
			<content:encoded><![CDATA[<p>Modeling the radiation generated by accreting matter is an important step towards realistic simulations of black hole accretion disks, especially at high accretion rates. To this end, we have recently added radiation transport to the existing general relativistic magnetohydrodynamic code, Cosmos++. However, before attempting to model radiative accretion disks, we have tested the new code using a series of shock tube and Bondi (spherical inflow) problems. The four radiative shock tube tests, first presented by Farris et al. (2008), have known analytic solutions, allowing us to calculate errors and convergence rates for our code. The Bondi problem only has an analytic solution when radiative processes are ignored, but is pertinent because it is closer to the physics we ultimately want to study. In our simulations, we include Thomson scattering and thermal bremsstrahlung in the opacity, focusing exclusively on the super-Eddington regime. Unlike accretion onto bodies with solid surfaces, super-Eddington accretion onto black holes does not produce super-Eddington luminosity. In our examples, despite accreting at up to 300 times the Eddington rate, our measured luminosity is always several orders of magnitude below Eddington.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/08/numerical-simulations-of-optically-thick-accretion-onto-a-black-hole-i-spherical-case-replacement/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Detection of a radio bridge in Abell 3667</title>
		<link>http://voxcharta.org/2012/05/07/detection-of-a-radio-bridge-in-abell-3667/</link>
		<comments>http://voxcharta.org/2012/05/07/detection-of-a-radio-bridge-in-abell-3667/#comments</comments>
		<pubDate>Tue, 08 May 2012 01:04:24 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[acceleration]]></category>
		<category><![CDATA[central regions]]></category>
		<category><![CDATA[diffuse emission]]></category>
		<category><![CDATA[direct evidence]]></category>
		<category><![CDATA[galaxy cluster abell]]></category>
		<category><![CDATA[large scale]]></category>
		<category><![CDATA[magnetic field intensity]]></category>
		<category><![CDATA[natural explanation]]></category>
		<category><![CDATA[observation]]></category>
		<category><![CDATA[parkes radio telescope]]></category>
		<category><![CDATA[polarization]]></category>
		<category><![CDATA[ray bridge]]></category>
		<category><![CDATA[relativistic electron]]></category>
		<category><![CDATA[relic]]></category>
		<category><![CDATA[s pass]]></category>
		<category><![CDATA[shock front]]></category>
		<category><![CDATA[sky survey]]></category>
		<category><![CDATA[synchrotron emission]]></category>
		<category><![CDATA[Turbulence]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/detection-of-a-radio-bridge-in-abell-3667/</guid>
		<description><![CDATA[We have detected a radio bridge of unpolarized synchrotron emission connecting the NW relic of the galaxy cluster Abell 3667 to its central regions. We used data at 2.3 GHz from the S-band Polarization All Sky Survey (S-PASS) and at 3.3 GHz from a follow up observation, both conducted with the Parkes Radio Telescope. This [...]]]></description>
			<content:encoded><![CDATA[<p>We have detected a radio bridge of unpolarized synchrotron emission connecting the NW relic of the galaxy cluster Abell 3667 to its central regions. We used data at 2.3 GHz from the S-band Polarization All Sky Survey (S-PASS) and at 3.3 GHz from a follow up observation, both conducted with the Parkes Radio Telescope. This emission is further aligned with a diffuse X-ray bridge, and represents the most compelling direct evidence for an association between intracluster medium turbulence and diffuse synchrotron emission. This is the first clear detection of a bridge associated both with an outlying cluster relic and an X-ray bridge. We conclude that the synchrotron bridge is related to the post-shock turbulence wake trailing a shock front. Although the origin of the relativistic electrons is still unknown, the turbulent re-acceleration model provides a natural explanation for the large-scale emission. The bridge magnetic field intensity is 0.5-0.6 uG. We further detect diffuse emission coincident with the central regions of the cluster for the first time.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/detection-of-a-radio-bridge-in-abell-3667/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>High energy gamma-ray emission from compact Galactic sources in the context of observations with the next generation Cherenkov Telescope Arrays</title>
		<link>http://voxcharta.org/2012/05/07/high-energy-gamma-ray-emission-from-compact-galactic-sources-in-the-context-of-observations-with-the-next-generation-cherenkov-telescope-arrays/</link>
		<comments>http://voxcharta.org/2012/05/07/high-energy-gamma-ray-emission-from-compact-galactic-sources-in-the-context-of-observations-with-the-next-generation-cherenkov-telescope-arrays/#comments</comments>
		<pubDate>Tue, 08 May 2012 01:02:32 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[compact object]]></category>
		<category><![CDATA[cta]]></category>
		<category><![CDATA[energetic particle]]></category>
		<category><![CDATA[energy range]]></category>
		<category><![CDATA[galactic sources]]></category>
		<category><![CDATA[gamma ray emission]]></category>
		<category><![CDATA[gev energy]]></category>
		<category><![CDATA[high energy]]></category>
		<category><![CDATA[hypothesis]]></category>
		<category><![CDATA[observational result]]></category>
		<category><![CDATA[order of magnitude]]></category>
		<category><![CDATA[physical processes]]></category>
		<category><![CDATA[ray astronomy]]></category>
		<category><![CDATA[ray sources]]></category>
		<category><![CDATA[telescope array]]></category>
		<category><![CDATA[telescopes]]></category>
		<category><![CDATA[tev energies]]></category>
		<category><![CDATA[theoretical implications]]></category>
		<category><![CDATA[time resolution]]></category>
		<category><![CDATA[unexpected feature]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/high-energy-gamma-ray-emission-from-compact-galactic-sources-in-the-context-of-observations-with-the-next-generation-cherenkov-telescope-arrays/</guid>
		<description><![CDATA[The observational progress in the $\gamma$-ray astronomy in the last few years has led to the discovery of more than a thousand sources at GeV energies and more than a hundred sources at TeV energies. A few different classes of compact objects in the Galaxy have been established. They show many unexpected features at high [...]]]></description>
			<content:encoded><![CDATA[<p>The observational progress in the $\gamma$-ray astronomy in the last few years has led to the discovery of more than a thousand sources at GeV energies and more than a hundred sources at TeV energies. A few different classes of compact objects in the Galaxy have been established. They show many unexpected features at high energies the physics of which remains mainly unknown. At present it is clear that detailed investigation of these new phenomena can be performed only with the technical equipment which offer an order of magnitude better sensitivity, and a few times better energy, angular and time resolution in the broad energy range staring from a few tens of GeV up to a few hundreds TeV. Such facilities can be realized by the next generation of instruments such as the planned Cherenkov Telescope Array (CTA).   The aim of this report is to summarize up to date observational results on the compact galactic sources in the GeV-TeV $\gamma$-ray energy range, discuss their theoretical implications, and indicate which hypothesis considered at present might be verified with the next generation of telescopes. We point out which of the observational features of the $\gamma$-ray sources are important to investigate with special care with the planned CTA in order to put a new light on physical processes involved. Their knowledge should finally allow us to answer the question on the origin of energetic particles in our Galaxy.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/high-energy-gamma-ray-emission-from-compact-galactic-sources-in-the-context-of-observations-with-the-next-generation-cherenkov-telescope-arrays/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Swift follow-up observations of candidate gravitational-wave transient events</title>
		<link>http://voxcharta.org/2012/05/07/swift-follow-up-observations-of-candidate-gravitational-wave-transient-events/</link>
		<comments>http://voxcharta.org/2012/05/07/swift-follow-up-observations-of-candidate-gravitational-wave-transient-events/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:59:03 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[decade]]></category>
		<category><![CDATA[electromagnetic data]]></category>
		<category><![CDATA[feasibility]]></category>
		<category><![CDATA[follow ups]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[ligo]]></category>
		<category><![CDATA[low latency]]></category>
		<category><![CDATA[observatory image]]></category>
		<category><![CDATA[regime]]></category>
		<category><![CDATA[science]]></category>
		<category><![CDATA[sky location]]></category>
		<category><![CDATA[swift]]></category>
		<category><![CDATA[transient events]]></category>
		<category><![CDATA[transients]]></category>
		<category><![CDATA[ups]]></category>
		<category><![CDATA[virgo]]></category>
		<category><![CDATA[wavelength]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/swift-follow-up-observations-of-candidate-gravitational-wave-transient-events/</guid>
		<description><![CDATA[We present the first multi-wavelength follow-up observations of two candidate gravitational-wave (GW) transient events recorded by LIGO and Virgo in their 2009-2010 science run. The events were selected with low latency by the network of GW detectors and their candidate sky locations were observed by the Swift observatory. Image transient detection was used to analyze [...]]]></description>
			<content:encoded><![CDATA[<p>We present the first multi-wavelength follow-up observations of two candidate gravitational-wave (GW) transient events recorded by LIGO and Virgo in their 2009-2010 science run. The events were selected with low latency by the network of GW detectors and their candidate sky locations were observed by the Swift observatory. Image transient detection was used to analyze the collected electromagnetic data, which were found to be consistent with background. Off-line analysis of the GW data alone has also established that the selected GW events show no evidence of an astrophysical origin; one of them is consistent with background and the other one was a test, part of a &#8220;blind injection challenge&#8221;. With this work we demonstrate the feasibility of rapid follow-ups of GW transients and establish the sensitivity improvement joint electromagnetic and GW observations could bring. This is a first step toward an electromagnetic follow-up program in the regime of routine detections with the advanced GW instruments expected within this decade. In that regime multi-wavelength observations will play a significant role in completing the astrophysical identification of GW sources. We present the methods and results from this first combined analysis and discuss its implications in terms of sensitivity for the present and future instruments.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/swift-follow-up-observations-of-candidate-gravitational-wave-transient-events/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>GUT and Supersymmetry at the LHC and in dark matter [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/07/gut-and-supersymmetry-at-the-lhc-and-in-dark-matter-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/07/gut-and-supersymmetry-at-the-lhc-and-in-dark-matter-cross-listing/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:58:29 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[assumption]]></category>
		<category><![CDATA[boson mass]]></category>
		<category><![CDATA[dark matter]]></category>
		<category><![CDATA[discovery]]></category>
		<category><![CDATA[doublet]]></category>
		<category><![CDATA[electroweak symmetry]]></category>
		<category><![CDATA[energy physics]]></category>
		<category><![CDATA[focal surface]]></category>
		<category><![CDATA[grand unification]]></category>
		<category><![CDATA[hierarchy problem]]></category>
		<category><![CDATA[higgs field]]></category>
		<category><![CDATA[lhc]]></category>
		<category><![CDATA[low energy]]></category>
		<category><![CDATA[natural solution]]></category>
		<category><![CDATA[parameter space]]></category>
		<category><![CDATA[representations]]></category>
		<category><![CDATA[scale model]]></category>
		<category><![CDATA[supersymmetry]]></category>
		<category><![CDATA[triplet]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/gut-and-supersymmetry-at-the-lhc-and-in-dark-matter-cross-listing/</guid>
		<description><![CDATA[Conventional SO(10) models involve more than one scale for a complete breaking of the GUT symmetry requiring further assumptions on the VEVs of the Higgs fields that enter in the breaking to achieve viable models. Recent works where the breaking can be accomplished at one scale are discussed. There include models with just a pair [...]]]></description>
			<content:encoded><![CDATA[<p>Conventional SO(10) models involve more than one scale for a complete breaking of the GUT symmetry requiring further assumptions on the VEVs of the Higgs fields that enter in the breaking to achieve viable models. Recent works where the breaking can be accomplished at one scale are discussed. There include models with just a pair of $144+\bar{144}$ of Higgs fields. Further extensions of this idea utilizing $560+ \bar{560}$ of Higgs representations allow both the breaking at one scale, as well as accomplish a natural doublet-triplet splitting via the missing partner mechanism. More generally, we discuss the connection of high scale models to low energy physics in the context of supergravity grand unification. Here we discuss a natural solution to the little hierarchy problem and also discuss the implications of the LHC data for supersymmetry. It is shown that the LHC data implies that most of the parameter space of supergravity models consistent with the data lie on the Hyperbolic Branch of radiative breaking of the electroweak symmetry and more specifically on the Focal Surface of the Hyperbolic Branch. A discussion is also given of the implications of recent LHC data on the Higgs boson mass for the discovery of supersymmetry and for the search for dark matter.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/gut-and-supersymmetry-at-the-lhc-and-in-dark-matter-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Duration Distribution of Fermi/GBM Gamma-Ray Bursts: Instrumental Selection Effect of the Bimodal T90 Distribution</title>
		<link>http://voxcharta.org/2012/05/07/duration-distribution-of-fermigbm-gamma-ray-bursts-instrumental-selection-effect-of-the-bimodal-t90-distribution/</link>
		<comments>http://voxcharta.org/2012/05/07/duration-distribution-of-fermigbm-gamma-ray-bursts-instrumental-selection-effect-of-the-bimodal-t90-distribution/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:57:55 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[activity time]]></category>
		<category><![CDATA[bat 15]]></category>
		<category><![CDATA[bepposax]]></category>
		<category><![CDATA[bimodal]]></category>
		<category><![CDATA[cgro]]></category>
		<category><![CDATA[classification scheme]]></category>
		<category><![CDATA[distributions]]></category>
		<category><![CDATA[duration]]></category>
		<category><![CDATA[energy band]]></category>
		<category><![CDATA[energy dependence]]></category>
		<category><![CDATA[engine model]]></category>
		<category><![CDATA[flare]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[hete]]></category>
		<category><![CDATA[keV]]></category>
		<category><![CDATA[nai detectors]]></category>
		<category><![CDATA[selection effect]]></category>
		<category><![CDATA[statistical significance level]]></category>
		<category><![CDATA[time scale]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/duration-distribution-of-fermigbm-gamma-ray-bursts-instrumental-selection-effect-of-the-bimodal-t90-distribution/</guid>
		<description><![CDATA[The durations (T_{90}) of 315 Fermi GRBs detected with the GBM-NaI detectors (8-1000 KeV) by 2011 September are calculated using the Bayesian Block method. We compare the T_{90} distribution of the GBM-NaI sample to that observed with CGRO/BATSE (25-2000 keV), BeppoSAX/GRBM (40-700 KeV), HETE-2/FREGATE (6-80 keV), and Swift/BAT (15-150 keV). We show that the T_{90} [...]]]></description>
			<content:encoded><![CDATA[<p>The durations (T_{90}) of 315 Fermi GRBs detected with the GBM-NaI detectors (8-1000 KeV) by 2011 September are calculated using the Bayesian Block method. We compare the T_{90} distribution of the GBM-NaI sample to that observed with CGRO/BATSE (25-2000 keV), BeppoSAX/GRBM (40-700 KeV), HETE-2/FREGATE (6-80 keV), and Swift/BAT (15-150 keV). We show that the T_{90} distribution of the GBM-NaI GRB sample is bimodal, with a statistical significance level being comparable to that observed with BeppoSAX/GRBM and Swift/BAT but much lower than that observed with CGRO/BATSE. No bimodal T_{90} distribution is found in the HETE-2 GRB sample. Taking T_{90}=2 seconds as the division line between long and short GRBs, the ratio of short to long GRB numbers are 0:95, 51:557, 111:892, 39:253, and 500:1541 for the HETE-2/FREGATE, Swift/BAT, BeppoSAX/GRBM, GBM-NaI, and CGRO/BATSE GRB samples, respectively. These results suggest that the bimodal T_{90} distribution would be due to an instrumental selection effect. We investigate the energy dependence of T_{90} by measuring the T_{90} in the 8-15 KeV, 15-25 keV, 25-20 KeV, 50-100 keV, 100-350 keV, and 350-1000 keV energy bands with the GBM-NaI data. It is found that the T_{90} distributions in different energy bands are roughly consistent with the those derived from the instruments with similar corresponding energy bands. The value of T_{90} as a function of energy follows a relation T_{90}~ E^{-0.15}. Including X-ray flares, we found that the central engine activity time scale can be even much longer for some GRBs. Our results, together with the observed extended emission of Type I GRBs and significant flares in both the Type I and Type II GRBs, not only challenges the long-short GRB classification scheme, but also challenges the conventional GRB central engine models.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/duration-distribution-of-fermigbm-gamma-ray-bursts-instrumental-selection-effect-of-the-bimodal-t90-distribution/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Galactic annihilation emission from nucleosynthesis positrons</title>
		<link>http://voxcharta.org/2012/05/07/galactic-annihilation-emission-from-nucleosynthesis-positrons/</link>
		<comments>http://voxcharta.org/2012/05/07/galactic-annihilation-emission-from-nucleosynthesis-positrons/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:57:30 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[annihilation]]></category>
		<category><![CDATA[bulge]]></category>
		<category><![CDATA[central regions]]></category>
		<category><![CDATA[decay]]></category>
		<category><![CDATA[exact origin]]></category>
		<category><![CDATA[galaxy]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[intensity distribution]]></category>
		<category><![CDATA[interstellar medium]]></category>
		<category><![CDATA[large scale]]></category>
		<category><![CDATA[low energy]]></category>
		<category><![CDATA[nucleosynthesis]]></category>
		<category><![CDATA[particle]]></category>
		<category><![CDATA[positron]]></category>
		<category><![CDATA[prescriptions]]></category>
		<category><![CDATA[propagation]]></category>
		<category><![CDATA[radioactivity]]></category>
		<category><![CDATA[ratios]]></category>
		<category><![CDATA[spatial distribution]]></category>
		<category><![CDATA[telescopes]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/galactic-annihilation-emission-from-nucleosynthesis-positrons/</guid>
		<description><![CDATA[The Galaxy hosts a widespread population of low-energy positrons revealed by successive generations of gamma-ray telescopes through a bright annihilation emission from the bulge region, with a fainter contribution from the inner disk. The exact origin of these particles remains currently unknown. We estimate the contribution to the annihilation signal of positrons generated in the [...]]]></description>
			<content:encoded><![CDATA[<p>The Galaxy hosts a widespread population of low-energy positrons revealed by successive generations of gamma-ray telescopes through a bright annihilation emission from the bulge region, with a fainter contribution from the inner disk. The exact origin of these particles remains currently unknown. We estimate the contribution to the annihilation signal of positrons generated in the decay of radioactive 26Al, 56Ni and 44Ti. We adapted the GALPROP propagation code to simulate the transport and annihilation of radioactivity positrons in a model of our Galaxy. Using plausible source spatial distributions, we explored several possible propagation scenarios to account for the large uncertainties on the transport of ~1MeV positrons in the interstellar medium. We then compared the predicted intensity distributions to the INTEGRAL/SPI observations. We obtain similar intensity distributions with small bulge-to-disk ratios, even for extreme large-scale transport prescriptions. At least half of the positrons annihilate close to their sources, even when they are allowed to travel far away. In the high-diffusion, ballistic case, up to 40% of them escape the Galaxy. In proportion, this affects bulge positrons more than disk positrons because they are injected further off the plane in a tenuous medium, while disk positrons are mostly injected in the dense molecular ring. The predicted intensity distributions are fully consistent with the observed longitudinally-extended disk-like emission, but the transport scenario cannot be strongly constrained by the current data. Nucleosynthesis positrons alone cannot account for the observed annihilation emission in the frame of our model. An additional component is needed to explain the strong bulge contribution, and the latter is very likely concentrated in the central regions if positrons have initial energies in the 100keV-1MeV range.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/galactic-annihilation-emission-from-nucleosynthesis-positrons/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>A new look at spherical accretion in High Mass X-ray Binaries</title>
		<link>http://voxcharta.org/2012/05/07/a-new-look-at-spherical-accretion-in-high-mass-x-ray-binaries/</link>
		<comments>http://voxcharta.org/2012/05/07/a-new-look-at-spherical-accretion-in-high-mass-x-ray-binaries/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:55:22 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[accretion]]></category>
		<category><![CDATA[evolution]]></category>
		<category><![CDATA[high mass]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetosphere]]></category>
		<category><![CDATA[mass x]]></category>
		<category><![CDATA[parameter]]></category>
		<category><![CDATA[rotating neutron star]]></category>
		<category><![CDATA[stellar field]]></category>
		<category><![CDATA[torque]]></category>
		<category><![CDATA[turbulent diffusion]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/a-new-look-at-spherical-accretion-in-high-mass-x-ray-binaries/</guid>
		<description><![CDATA[Currently used model of spherical accretion onto a magnetized rotating neutron star encounters major difficulties in explaining the entry rate of accreting material into the stellar field and spin evolution of long-period X-ray pulsars. These difficulties can be, however, avoided if the magnetic field of the material captured by the neutron star is incorporated into [...]]]></description>
			<content:encoded><![CDATA[<p>Currently used model of spherical accretion onto a magnetized rotating neutron star encounters major difficulties in explaining the entry rate of accreting material into the stellar field and spin evolution of long-period X-ray pulsars. These difficulties can be, however, avoided if the magnetic field of the material captured by the neutron star is incorporated into the model. The magnetic field of the flow itself under certain conditions controls the accretion process and significantly affects the parameters of the accreting material. The mode by which the accretion flow enters the stellar magnetosphere in that case can be associated with Bohm (or turbulent) diffusion and the torque applied to the neutron star appears to be substantially higher than that evaluated in the non-magnetized accretion scenario.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/a-new-look-at-spherical-accretion-in-high-mass-x-ray-binaries/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<title>Testing Chern-Simons Modified Gravity with Gravitational-Wave Detections of Extreme-Mass-Ratio Binaries [Cross-Listing]</title>
		<link>http://voxcharta.org/2012/05/07/testing-chern-simons-modified-gravity-with-gravitational-wave-detections-of-extreme-mass-ratio-binaries-cross-listing/</link>
		<comments>http://voxcharta.org/2012/05/07/testing-chern-simons-modified-gravity-with-gravitational-wave-detections-of-extreme-mass-ratio-binaries-cross-listing/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:54:15 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[Cross-Listings]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[black hole]]></category>
		<category><![CDATA[compact object]]></category>
		<category><![CDATA[configuration space]]></category>
		<category><![CDATA[correct theory]]></category>
		<category><![CDATA[dimensional subspace]]></category>
		<category><![CDATA[emri]]></category>
		<category><![CDATA[extreme mass]]></category>
		<category><![CDATA[general relativity]]></category>
		<category><![CDATA[gravitational wave]]></category>
		<category><![CDATA[gravitational wave detector]]></category>
		<category><![CDATA[gravitational waveforms]]></category>
		<category><![CDATA[inspiral]]></category>
		<category><![CDATA[laser interferometer space antenna]]></category>
		<category><![CDATA[laser interferometer space antenna lisa]]></category>
		<category><![CDATA[mass ratio]]></category>
		<category><![CDATA[massive black hole]]></category>
		<category><![CDATA[orders of magnitude]]></category>
		<category><![CDATA[parameter estimation]]></category>
		<category><![CDATA[radiative]]></category>
		<category><![CDATA[true theory]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/testing-chern-simons-modified-gravity-with-gravitational-wave-detections-of-extreme-mass-ratio-binaries-cross-listing/</guid>
		<description><![CDATA[[abridged] The detection of gravitational waves from extreme-mass-ratio (EMRI) binaries, comprising a stellar-mass compact object orbiting around a massive black hole, is one of the main targets for low-frequency gravitational-wave detectors in space, like the Laser Interferometer Space Antenna (LISA or eLISA/NGO). The long-duration gravitational-waveforms emitted by such systems encode the structure of the strong [...]]]></description>
			<content:encoded><![CDATA[<p>[abridged] The detection of gravitational waves from extreme-mass-ratio (EMRI) binaries, comprising a stellar-mass compact object orbiting around a massive black hole, is one of the main targets for low-frequency gravitational-wave detectors in space, like the Laser Interferometer Space Antenna (LISA or eLISA/NGO). The long-duration gravitational-waveforms emitted by such systems encode the structure of the strong field region of the massive black hole, in which the inspiral occurs. The detection and analysis of EMRIs will therefore allow us to study the geometry of massive black holes and determine whether their nature is as predicted by General Relativity and even to test whether General Relativity is the correct theory to describe the dynamics of these systems. To achieve this, EMRI modeling in alternative theories of gravity is required to describe the generation of gravitational waves. In this paper, we explore to what extent EMRI observations with LISA or eLISA/NGO might be able to distinguish between General Relativity and a particular modification of it, known as Dynamical Chern-Simons Modified Gravity. Our analysis is based on a parameter estimation study that uses approximate gravitational waveforms obtained via a radiative-adiabatic method and is restricted to a five-dimensional subspace of the EMRI configuration space. This includes a Chern-Simons parameter that controls the strength of gravitational deviations from General Relativity. We find that, if Dynamical Chern-Simons Modified Gravity is the correct theory, an observatory like LISA or even eLISA/NGO should be able to measure the Chern-Simons parameter with fractional errors below 5%. If General Relativity is the true theory, these observatories should put bounds on this parameter at the level xi^(1/4) &lt; 10^4 km, which is four orders of magnitude better than current Solar System bounds.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/testing-chern-simons-modified-gravity-with-gravitational-wave-detections-of-extreme-mass-ratio-binaries-cross-listing/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Multifrequency radio observations of SNR J0536-6735 (N 59B) with associated pulsar</title>
		<link>http://voxcharta.org/2012/05/07/multifrequency-radio-observations-of-snr-j0536-6735-n-59b-with-associated-pulsar/</link>
		<comments>http://voxcharta.org/2012/05/07/multifrequency-radio-observations-of-snr-j0536-6735-n-59b-with-associated-pulsar/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:53:23 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[australian telescope]]></category>
		<category><![CDATA[continuum images]]></category>
		<category><![CDATA[density estimate]]></category>
		<category><![CDATA[diameter]]></category>
		<category><![CDATA[flux density]]></category>
		<category><![CDATA[hii region]]></category>
		<category><![CDATA[morphology]]></category>
		<category><![CDATA[nebulae]]></category>
		<category><![CDATA[northern limb]]></category>
		<category><![CDATA[optical emission]]></category>
		<category><![CDATA[point source]]></category>
		<category><![CDATA[radio continuum emission]]></category>
		<category><![CDATA[radio observation]]></category>
		<category><![CDATA[remnant]]></category>
		<category><![CDATA[spectral index]]></category>
		<category><![CDATA[sr 1]]></category>
		<category><![CDATA[surface brightness]]></category>
		<category><![CDATA[telescope compact array]]></category>
		<category><![CDATA[x ray]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/multifrequency-radio-observations-of-snr-j0536-6735-n-59b-with-associated-pulsar/</guid>
		<description><![CDATA[We present a study of new Australian Telescope Compact Array (ATCA) observations of supernova remnant, SNR J0536-6735. This remnant appears to follow a shell morphology with a diameter of D=36&#215;29 pc (with 1 pc uncertainty in each direction). There is an embedded Hii region on the northern limb of the remnant which made various analysis [...]]]></description>
			<content:encoded><![CDATA[<p>We present a study of new Australian Telescope Compact Array (ATCA) observations of supernova remnant, SNR J0536-6735. This remnant appears to follow a shell morphology with a diameter of D=36&#215;29 pc (with 1 pc uncertainty in each direction). There is an embedded Hii region on the northern limb of the remnant which made various analysis and measurements (such as flux density, spectral index and polarisation) difficult. The radio-continuum emission followed the same structure as the optical emission, allowing for extent and flux density estimates at 20 cm. We estimate a surface brightness for the SNR at 1 GHz of 2.55&#215;10^-21 W m^-2 Hz^-1 sr^-1. Also, we detect a distinctive radio-continuum point source which confirms the previous suggestion of this remnant being associated with a pulsar wind nebulae (PWN). The tail of this remnant isn&#8217;t seen in the radio-continuum images and is only seen in the optical and X-ray images.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/multifrequency-radio-observations-of-snr-j0536-6735-n-59b-with-associated-pulsar/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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		<item>
		<title>Southern-Hemisphere AGN Monitoring on (Sub-)Parsec Scales: The TANAMI Program</title>
		<link>http://voxcharta.org/2012/05/07/southern-hemisphere-agn-monitoring-on-sub-parsec-scales-the-tanami-program/</link>
		<comments>http://voxcharta.org/2012/05/07/southern-hemisphere-agn-monitoring-on-sub-parsec-scales-the-tanami-program/#comments</comments>
		<pubDate>Tue, 08 May 2012 00:46:36 +0000</pubDate>
		<dc:creator>astro-ph</dc:creator>
				<category><![CDATA[Cosmology and Extragalactic]]></category>
		<category><![CDATA[High Energy]]></category>
		<category><![CDATA[New]]></category>
		<category><![CDATA[astro-ph]]></category>
		<category><![CDATA[active galactic nuclei]]></category>
		<category><![CDATA[baseline array]]></category>
		<category><![CDATA[baseline interferometry]]></category>
		<category><![CDATA[deg declination]]></category>
		<category><![CDATA[emission models]]></category>
		<category><![CDATA[extragalactic jets]]></category>
		<category><![CDATA[follow ups]]></category>
		<category><![CDATA[gamma ray]]></category>
		<category><![CDATA[high angular resolution]]></category>
		<category><![CDATA[index map]]></category>
		<category><![CDATA[jet structure]]></category>
		<category><![CDATA[parsec]]></category>
		<category><![CDATA[radio galaxy]]></category>
		<category><![CDATA[radio gamma]]></category>
		<category><![CDATA[radio telescope]]></category>
		<category><![CDATA[southern hemisphere]]></category>
		<category><![CDATA[spectral energy distribution]]></category>
		<category><![CDATA[spectral index]]></category>
		<category><![CDATA[vlbi images]]></category>

		<guid isPermaLink="false">http://voxcharta.org/2012/05/07/southern-hemisphere-agn-monitoring-on-sub-parsec-scales-the-tanami-program/</guid>
		<description><![CDATA[The Very Long Baseline Interferometry (VLBI) monitoring program TANAMI provides bi-monthly, dualfrequency (8GHz and 22GHz) observations of extragalactic jets with milliarcsecond resolution south of -30 deg declination using the Australian Long Baseline Array (LBA) and additional radio telescopes in Antarctica, Chile, New Zealand and South Africa. Supporting programs provide multiwavelength coverage of the Fermi/LAT sources [...]]]></description>
			<content:encoded><![CDATA[<p>The Very Long Baseline Interferometry (VLBI) monitoring program TANAMI provides bi-monthly, dualfrequency (8GHz and 22GHz) observations of extragalactic jets with milliarcsecond resolution south of -30 deg declination using the Australian Long Baseline Array (LBA) and additional radio telescopes in Antarctica, Chile, New Zealand and South Africa. Supporting programs provide multiwavelength coverage of the Fermi/LAT sources of the TANAMI sample, in order to construct simultaneous broadband spectral energy distributions (SEDs), as well as rapid follow-ups of high energy flares. The main purpose of this project is to study the radio-gamma-ray connection seen in the jets of active galactic nuclei (AGN) via simultaneous monitoring of their VLBI structure and broadband emission in order to distinguish between different proposed emission models. Here we give a brief description of the TANAMI program and will then focus on its current status: (1) We present some results on the first simultaneous dual-frequency images of the whole sample resulting in spectral index maps of the parsec-scale core-jet structure. (2) The TANAMI array allows us to observe the closest radio galaxy Centaurus A with unprecedented high angular resolution resulting in the best-ever image of an AGN jet. We constructed the best resolved spectral index map of its jet-counterjet system revealing multiple possible production sites of gamma-rays recently detected by Fermi/LAT. With the first epochs of the TANAMI monitoring, we can study the proper jet motion of individual jet components of Cen A on sub-parsec scales. (3) Since the launch of Fermi/LAT we added newly detected gamma-ray bright AGN to the TANAMI observing list which is built as a combined radio and gamma-ray selected sample. For most of these sources the TANAMI observations obtain the first VLBI images ever made.</p>
]]></content:encoded>
			<wfw:commentRss>http://voxcharta.org/2012/05/07/southern-hemisphere-agn-monitoring-on-sub-parsec-scales-the-tanami-program/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
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	</channel>
</rss>

