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	<title>LISA Brownbag - GW Notes &#187; astro-ph.IM</title>
	<atom:link href="http://brownbag.lisascience.org/category/astro-phim/feed/" rel="self" type="application/rss+xml" />
	<link>http://brownbag.lisascience.org</link>
	<description></description>
	<lastBuildDate>Thu, 29 Jul 2010 09:19:13 +0000</lastBuildDate>
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		<title>MYRIAD: A new N-body code for simulations of Star Clusters</title>
		<link>http://brownbag.lisascience.org/arxiv1006-3326/</link>
		<comments>http://brownbag.lisascience.org/arxiv1006-3326/#comments</comments>
		<pubDate>Fri, 18 Jun 2010 08:34:42 +0000</pubDate>
		<dc:creator>lbb_robot</dc:creator>
				<category><![CDATA[GPU]]></category>
		<category><![CDATA[GRAPE hw]]></category>
		<category><![CDATA[astro-ph.GA]]></category>
		<category><![CDATA[astro-ph.IM]]></category>
		<category><![CDATA[astrophysics]]></category>
		<category><![CDATA[globular clusters]]></category>
		<category><![CDATA[intermediate-mass black holes]]></category>
		<category><![CDATA[numerical methods]]></category>
		<category><![CDATA[stellar dynamics]]></category>
		<category><![CDATA[supermassive black holes]]></category>

		<guid isPermaLink="false">http://brownbag.lisascience.org/arxiv1006-3326/</guid>
		<description><![CDATA[arXiv:1006.3326
by Konstantinidis, Simos and Kokkotas, Kostas D.
24 pages, 28 figures

  We present a new C++ code for collisional N-body simulations of star clusters. The code uses the Hermite fourth-order scheme with block time steps, for advancing the particles in time, while the forces and neighboring particles are computed using the GRAPE-6 board. Special treatment [...]]]></description>
			<content:encoded><![CDATA[<p><b><a href="http://arxiv.org/abs/1006.3326">arXiv:1006.3326</a></b></p>
<p>by <b>Konstantinidis, Simos</b> and <b>Kokkotas, Kostas D.</b><br />
24 pages, 28 figures</p>
<p><span id="more-866"></span></p>
<p>  We present a new C++ code for collisional N-body simulations of star clusters. The code uses the Hermite fourth-order scheme with block time steps, for advancing the particles in time, while the forces and neighboring particles are computed using the GRAPE-6 board. Special treatment is used for close encounters, binary and multiple sub-systems that either form dynamically or exist in the initial configuration. The structure of the code is modular and allows the appropriate treatment of more physical phenomena, such as stellar and binary evolution, stellar collisions and evolution of close black-hole binaries. Moreover, it can be easily modified so that the part of the code that uses GRAPE-6, could be replaced by another module that uses other accelerating-hardware like the Graphics Processing Units (GPUs). Appropriate choice of the free parameters give a good accuracy and speed for simulations of star clusters up to and beyond core collapse. Simulations of Plummer models consisting of equal-mass stars reached core collapse at t~17 half-mass relaxation times, which compares very well with existing results, while the cumulative relative error in the energy remained below 0.001. Also, comparisons with published results of other codes for the time of core collapse for different initial conditions, show excellent agreement. Simulations of King models with an initial mass-function, similar to those found in the literature, reached core collapse at t~0.17, which is slightly smaller than the expected result from previous works. Finally, the code accuracy becomes comparable and even better than the accuracy of existing codes, when a number of close binary systems is dynamically created in a simulation. This is due to the high accuracy of the method that is used for close binary and multiple sub-systems. </p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Experimental Demonstration of Time-Delay Interferometry for the Laser  Interferometer Space Antenna</title>
		<link>http://brownbag.lisascience.org/arxiv1005-2176/</link>
		<comments>http://brownbag.lisascience.org/arxiv1005-2176/#comments</comments>
		<pubDate>Mon, 17 May 2010 14:39:55 +0000</pubDate>
		<dc:creator>lbb_robot</dc:creator>
				<category><![CDATA[astro-ph.IM]]></category>
		<category><![CDATA[detectors]]></category>
		<category><![CDATA[gr-qc]]></category>
		<category><![CDATA[instruments]]></category>
		<category><![CDATA[interferometers]]></category>
		<category><![CDATA[physics.ins-det]]></category>

		<guid isPermaLink="false">http://brownbag.lisascience.org/arxiv1005-2176/</guid>
		<description><![CDATA[arXiv:1005.2176
by de Vine, Glenn and Ware, Brent and McKenzie, Kirk and Spero, Robert E. and Klipstein, William M. and Shaddock, Daniel A.
4 pages, 4 figures, to appear in Physical Review Letters end of May  2010

  We report on the first demonstration of time-delay interferometry (TDI) for LISA, the Laser Interferometer Space Antenna. TDI [...]]]></description>
			<content:encoded><![CDATA[<p><b><a href="http://arxiv.org/abs/1005.2176">arXiv:1005.2176</a></b></p>
<p>by <b>de Vine, Glenn</b> and <b>Ware, Brent</b> and <b>McKenzie, Kirk</b> and <b>Spero, Robert E.</b> and <b>Klipstein, William M.</b> and <b>Shaddock, Daniel A.</b><br />
4 pages, 4 figures, to appear in Physical Review Letters end of May  2010</p>
<p><span id="more-837"></span></p>
<p>  We report on the first demonstration of time-delay interferometry (TDI) for LISA, the Laser Interferometer Space Antenna. TDI was implemented in a laboratory experiment designed to mimic the noise couplings that will occur in LISA. TDI suppressed laser frequency noise by approximately 10^9 and clock phase noise by 6&#215;10^4, recovering the intrinsic displacement noise floor of our laboratory test bed. This removal of laser frequency noise and clock phase noise in post-processing marks the first experimental validation of the LISA measurement scheme. </p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Detection, Localization and Characterization of Gravitational Wave  Bursts in a Pulsar Timing Array</title>
		<link>http://brownbag.lisascience.org/arxiv1004-3499-2/</link>
		<comments>http://brownbag.lisascience.org/arxiv1004-3499-2/#comments</comments>
		<pubDate>Sun, 09 May 2010 20:04:41 +0000</pubDate>
		<dc:creator>lbb_robot</dc:creator>
				<category><![CDATA[astro-ph.IM]]></category>
		<category><![CDATA[bursts]]></category>
		<category><![CDATA[data analysis]]></category>
		<category><![CDATA[gr-qc]]></category>
		<category><![CDATA[parameter estimation]]></category>
		<category><![CDATA[physics.data-an]]></category>
		<category><![CDATA[search algorithms]]></category>
		<category><![CDATA[sky resolution]]></category>
		<category><![CDATA[supermassive black holes]]></category>
		<category><![CDATA[waveforms]]></category>

		<guid isPermaLink="false">http://brownbag.lisascience.org/?p=833</guid>
		<description><![CDATA[arXiv:1004.3499
by Finn, Lee Samuel and Lommen, Andrea N.
43 pages, 13 figures, submitted to ApJ.

Efforts to detect gravitational waves by timing an array of pulsars have focused traditionally on stationary gravitational waves: e.g., stochastic or periodic signals. Gravitational wave bursts &#8212; signals whose duration is much shorter than the observation period &#8212; will also arise in [...]]]></description>
			<content:encoded><![CDATA[<p><strong><a href="http://arxiv.org/abs/1004.3499">arXiv:1004.3499</a></strong></p>
<p>by <strong>Finn, Lee Samuel</strong> and <strong>Lommen, Andrea N.</strong><br />
43 pages, 13 figures, submitted to ApJ.</p>
<p><span id="more-833"></span></p>
<p>Efforts to detect gravitational waves by timing an array of pulsars have focused traditionally on stationary gravitational waves: e.g., stochastic or periodic signals. Gravitational wave bursts &#8212; signals whose duration is much shorter than the observation period &#8212; will also arise in the pulsar timing array waveband. Sources that give rise to detectable bursts include the formation or coalescence of supermassive black holes (SMBHs), the periapsis passage of compact objects in highly elliptic or unbound orbits about a SMBH, or cusps on cosmic strings. Here we describe how pulsar timing array data may be analyzed to detect and characterize these bursts. Our analysis addresses, in a mutually consistent manner, a hierarchy of three questions: \emph{i}) What are the odds that a dataset includes the signal from a gravitational wave burst? \emph{ii}) Assuming the presence of a burst, what is the direction to its source? and \emph{iii}) Assuming the burst propagation direction, what is the burst waveform&#8217;s time dependence in each of its polarization states? Applying our analysis to synthetic data sets we find that we can \emph{detect} gravitational waves even when the radiation is too weak to either localize the source of infer the waveform, and \emph{detect} and \emph{localize} sources even when the radiation amplitude is too weak to permit the waveform to be determined. While the context of our discussion is gravitational wave detection via pulsar timing arrays, the analysis itself is directly applicable to gravitational wave detection using either ground or space-based detector data.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>The Supermassive Black Hole at the Heart of Centaurus A: Revealed by  Gas- and Stellar Kinematics</title>
		<link>http://brownbag.lisascience.org/arxiv1002-0965/</link>
		<comments>http://brownbag.lisascience.org/arxiv1002-0965/#comments</comments>
		<pubDate>Fri, 05 Feb 2010 10:17:51 +0000</pubDate>
		<dc:creator>lbb_robot</dc:creator>
				<category><![CDATA[astro-ph.CO]]></category>
		<category><![CDATA[astro-ph.IM]]></category>
		<category><![CDATA[astrophysics]]></category>
		<category><![CDATA[observations]]></category>
		<category><![CDATA[supermassive black holes]]></category>

		<guid isPermaLink="false">http://brownbag.lisascience.org/arxiv1002-0965/</guid>
		<description><![CDATA[arXiv:1002.0965
by Neumayer, Nadine
8 pages, accepted for publication in PASA, contribution for &#8220;The Many  Faces of Centaurus A&#8221; conference in Sydney, 2009

  At less than 4 Mpc distance the radio galaxy NGC 5128 (Centaurus A) is the prime example to study the supermassive black hole and its influence on the environment in great detail. [...]]]></description>
			<content:encoded><![CDATA[<p><b><a href="http://arxiv.org/abs/1002.0965">arXiv:1002.0965</a></b></p>
<p>by <b>Neumayer, Nadine</b><br />
8 pages, accepted for publication in PASA, contribution for &#8220;The Many  Faces of Centaurus A&#8221; conference in Sydney, 2009</p>
<p><span id="more-772"></span></p>
<p>  At less than 4 Mpc distance the radio galaxy NGC 5128 (Centaurus A) is the prime example to study the supermassive black hole and its influence on the environment in great detail. To model and understand the feeding and feedback mechanisms one needs an accurate determination of the mass of the supermassive black hole. The aim of this review is to give an overview of the recent studies that have been dedicated to measure the black hole mass in Centaurus A from both gas and stellar kinematics. It shows how the advancement in observing techniques and instrumentation drive the field of black hole mass measurements and concludes that adaptive optics assisted integral field spectroscopy is the key to identify the effects of the AGN on the surrounding ionised gas. Using data from SINFONI at the ESO Very Large Telescope, the best-fit black hole mass is M_BH=4.5 +1.7/-1.0 x 10^7 Msolar (from H_2 kinematics) and M_BH= (5.5 +/- 3.0) x 10^7 Msolar (from stellar kinematics; both with 3 sigma errors). This is one of the cleanest gas vs star comparison of a M_BH determination, and brings Centaurus A into agreement with the M_BH-sigma relation. </p>
]]></content:encoded>
			<wfw:commentRss>http://brownbag.lisascience.org/arxiv1002-0965/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Supercomputing and stellar dynamics</title>
		<link>http://brownbag.lisascience.org/arxiv09090879/</link>
		<comments>http://brownbag.lisascience.org/arxiv09090879/#comments</comments>
		<pubDate>Wed, 09 Sep 2009 10:25:33 +0000</pubDate>
		<dc:creator>lbb_robot</dc:creator>
				<category><![CDATA[GPU]]></category>
		<category><![CDATA[astro-ph.GA]]></category>
		<category><![CDATA[astro-ph.IM]]></category>
		<category><![CDATA[astrophysics]]></category>
		<category><![CDATA[stellar dynamics]]></category>

		<guid isPermaLink="false">http://brownbag.lisascience.org/arxiv09090879/</guid>
		<description><![CDATA[arXiv:0909.0879
by Capuzzo-Dolcetta, R.
Invited talk to the 2009 general Conference of the Societa&#8217;  Astronomica Italiana. 6 pages including 1 figure

  In this paper I will outline some of the aspects and problems of modern celestial mechanics and stellar dynamics, in the context of the quickly growing computing facilities. I will point the attention on [...]]]></description>
			<content:encoded><![CDATA[<p><b><a href="http://arxiv.org/abs/0909.0879">arXiv:0909.0879</a></b></p>
<p>by <b>Capuzzo-Dolcetta, R.</b><br />
Invited talk to the 2009 general Conference of the Societa&#8217;  Astronomica Italiana. 6 pages including 1 figure</p>
<p><span id="more-628"></span></p>
<p>  In this paper I will outline some of the aspects and problems of modern celestial mechanics and stellar dynamics, in the context of the quickly growing computing facilities. I will point the attention on the great advantages in using, for astrophysical simulations, the modern, fast and cheap Graphic Processing Units (GPUs) acting as true supercomputers. Finally, I present and discuss some characteristics and performances of a new double-parallel code exploiting the joint power of multicore CPUs and GPUs. </p>
]]></content:encoded>
			<wfw:commentRss>http://brownbag.lisascience.org/arxiv09090879/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>Oct-tree Method on GPU</title>
		<link>http://brownbag.lisascience.org/arxiv09090541/</link>
		<comments>http://brownbag.lisascience.org/arxiv09090541/#comments</comments>
		<pubDate>Fri, 04 Sep 2009 09:25:29 +0000</pubDate>
		<dc:creator>lbb_robot</dc:creator>
				<category><![CDATA[GPU]]></category>
		<category><![CDATA[astro-ph.GA]]></category>
		<category><![CDATA[astro-ph.IM]]></category>
		<category><![CDATA[astrophysics]]></category>
		<category><![CDATA[stellar dynamics]]></category>

		<guid isPermaLink="false">http://brownbag.lisascience.org/arxiv09090541/</guid>
		<description><![CDATA[arXiv:0909.0541
by Nakasato, N.
Poster paper to be appeared in SC09

  The kd-tree is a fundamental tool in computer science. Among others, an application of the kd-tree search (oct-tree method) to fast evaluation of particle interactions and neighbor search is highly important since computational complexity of these problems are reduced from O(N^2) with a brute force [...]]]></description>
			<content:encoded><![CDATA[<p><b><a href="http://arxiv.org/abs/0909.0541">arXiv:0909.0541</a></b></p>
<p>by <b>Nakasato, N.</b><br />
Poster paper to be appeared in SC09</p>
<p><span id="more-621"></span></p>
<p>  The kd-tree is a fundamental tool in computer science. Among others, an application of the kd-tree search (oct-tree method) to fast evaluation of particle interactions and neighbor search is highly important since computational complexity of these problems are reduced from O(N^2) with a brute force method to O(N log N) with the tree method where N is a number of particles. In this paper, we present a parallel implementation of the tree method running on a graphic processor unit (GPU). We successfully run a simulation of structure formation in the universe very efficiently. On our system, which costs roughly $900, the run with N ~ 2.87&#215;10^6 particles took 5.79 hours and executed 1.2&#215;10^13 force evaluations in total. We obtained the sustained computing speed of 21.8 Gflops and the cost per Gflops of 41.6/Gflops that is two and half times better than the previous record in 2006. </p>
]]></content:encoded>
			<wfw:commentRss>http://brownbag.lisascience.org/arxiv09090541/feed/</wfw:commentRss>
		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>A Bayesian approach to the study of white dwarf binaries in LISA data:  The application of a reversible jump Markov chain Monte Carlo method</title>
		<link>http://brownbag.lisascience.org/arxiv09072198/</link>
		<comments>http://brownbag.lisascience.org/arxiv09072198/#comments</comments>
		<pubDate>Sat, 18 Jul 2009 16:24:34 +0000</pubDate>
		<dc:creator>lbb_robot</dc:creator>
				<category><![CDATA[MLDC]]></category>
		<category><![CDATA[astro-ph.IM]]></category>
		<category><![CDATA[back/foreground]]></category>
		<category><![CDATA[data analysis]]></category>

		<guid isPermaLink="false">http://brownbag.lisascience.org/arxiv09072198/</guid>
		<description><![CDATA[arXiv:0907.2198
by Stroeer, Alexander and Veitch, John
18 pages, 8 figures, 3 tables, submitted to PRD

  The Laser Interferometer Space Antenna (LISA) defines new demands on data analysis efforts in its all-sky gravitational wave survey, recording simultaneously thousands of galactic compact object binary foreground sources and tens to hundreds of background sources like binary black hole [...]]]></description>
			<content:encoded><![CDATA[<p><b><a href="http://arxiv.org/abs/0907.2198">arXiv:0907.2198</a></b></p>
<p>by <b>Stroeer, Alexander</b> and <b>Veitch, John</b><br />
18 pages, 8 figures, 3 tables, submitted to PRD</p>
<p><span id="more-544"></span></p>
<p>  The Laser Interferometer Space Antenna (LISA) defines new demands on data analysis efforts in its all-sky gravitational wave survey, recording simultaneously thousands of galactic compact object binary foreground sources and tens to hundreds of background sources like binary black hole mergers and extreme mass ratio inspirals. We approach this problem with an adaptive and fully automatic Reversible Jump Markov Chain Monte Carlo sampler, able to sample from the joint posterior density function (as established by Bayes theorem) for a given mixture of signals &#8220;out of the box&#8221;, handling the total number of signals as an additional unknown parameter beside the unknown parameters of each individual source and the noise floor. We show in examples from the LISA Mock Data Challenge implementing the full response of LISA in its TDI description that this sampler is able to extract monochromatic Double White Dwarf signals out of colored instrumental noise and additional foreground and background noise successfully in a global fitting approach. We introduce 2 examples with fixed number of signals (MCMC sampling), and 1 example with unknown number of signals (RJ-MCMC), the latter further promoting the idea behind an experimental adaptation of the model indicator proposal densities in the main sampling stage. We note that the experienced runtimes and degeneracies in parameter extraction limit the shown examples to the extraction of a low but realistic number of signals. </p>
]]></content:encoded>
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