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	<title>The PT Symmeter &#187; F. Schaefer</title>
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		<title>PT symmetry and spontaneous symmetry breaking in microwave billiards</title>
		<link>http://ptsymmetry.net/?p=509&#038;utm_source=rss&#038;utm_medium=rss&#038;utm_campaign=pt-symmetry-and-spontaneous-symmetry-breaking-in-microwave-billiards</link>
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		<pubDate>Fri, 22 Jul 2011 10:58:02 +0000</pubDate>
		<dc:creator>dwh</dc:creator>
				<category><![CDATA[ECT]]></category>
		<category><![CDATA[Helmholtz-Zentrum Dresden-Rossendorf]]></category>
		<category><![CDATA[Max-Planck-Institut fur Kernphysik]]></category>
		<category><![CDATA[Universitat Darmstadt]]></category>
		<category><![CDATA[University of Florence]]></category>
		<category><![CDATA[A. Richter]]></category>
		<category><![CDATA[B. Dietz]]></category>
		<category><![CDATA[F. Schaefer]]></category>
		<category><![CDATA[H. L. Harney]]></category>
		<category><![CDATA[M. Miski-Oglu]]></category>
		<category><![CDATA[S. Bittner]]></category>
		<category><![CDATA[U. Guenther]]></category>

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		<description><![CDATA[S. Bittner, B. Dietz, U. Guenther, H. L. Harney, M. Miski-Oglu, A. Richter, F. Schaefer We demonstrate the presence of parity-time (PT) symmetry for the non-Hermitian two-state Hamiltonian of a dissipative microwave billiard in the vicinity of an exceptional point (EP). The shape of the billiard depends on two parameters. The Hamiltonian is determined from&#8230;]]></description>
			<content:encoded><![CDATA[<p>S. Bittner, B. Dietz, U. Guenther, H. L. Harney, M. Miski-Oglu, A. Richter, F. Schaefer</p>
<p><a href="http://ptsymmetry.net/wp-content/uploads/2011/07/Fig2_kl.jpg"><img class="alignleft size-full wp-image-510" title="Fig2_kl" src="http://ptsymmetry.net/wp-content/uploads/2011/07/Fig2_kl.jpg" alt="" width="200" height="92" /></a>We demonstrate the presence of parity-time (PT) symmetry for the non-Hermitian two-state Hamiltonian of a dissipative microwave billiard in the vicinity of an exceptional point (EP). The shape of the billiard depends on two parameters. The Hamiltonian is determined from the measured resonance spectrum on a fine grid in the parameter plane. On a curve, which passes through the EP, the Hamiltonian has either real or complex conjugate eigenvalues. An appropriate basis choice reveals its PT symmetry. Spontaneous symmetry breaking occurs at the EP.</p>
<p><a href="http://arxiv.org/abs/1107.4256" target="_blank">http://arxiv.org/abs/1107.4256</a><br />
Quantum Physics (quant-ph); Mathematical Physics (math-ph)</p>
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