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	<title>The PT Symmeter &#187; Universitat Darmstadt</title>
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		<title>Scattering Experiments with Microwave Billiards at an Exceptional Point under Broken Time Reversal Invariance</title>
		<link>http://ptsymmetry.net/?p=1595&#038;utm_source=rss&#038;utm_medium=rss&#038;utm_campaign=scattering-experiments-with-microwave-billiards-at-an-exceptional-point-under-broken-time-reversal-invariance</link>
		<comments>http://ptsymmetry.net/?p=1595#comments</comments>
		<pubDate>Fri, 14 Feb 2014 02:06:52 +0000</pubDate>
		<dc:creator>dwh</dc:creator>
				<category><![CDATA[Kyoto University]]></category>
		<category><![CDATA[Universitat Darmstadt]]></category>

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		<description><![CDATA[S.Bittner, B.Dietz, H.L.Harney, M.Miski-Oglu, A.Richter, F. Schäfer Scattering experiments with microwave cavities were performed and the effects of broken time-reversal invariance (TRI), induced by means of a magnetized ferrite placed inside the cavity, on an isolated doublet of nearly degenerate resonances were investigated. All elements of the effective Hamiltonian of this two-level system were extracted.&#8230;]]></description>
			<content:encoded><![CDATA[<p>S.Bittner, B.Dietz, H.L.Harney, M.Miski-Oglu, A.Richter, F. Schäfer<span style="background-color: transparent;"> </span></p>
<p>Scattering experiments with microwave cavities were performed and the effects of broken time-reversal invariance (TRI), induced by means of a magnetized ferrite placed inside the cavity, on an isolated doublet of nearly degenerate resonances were investigated. All elements of the effective Hamiltonian of this two-level system were extracted. As a function of two experimental parameters, the doublet and also the associated eigenvectors could be tuned to coalesce at a so-called exceptional point (EP). The behavior of the eigenvalues and eigenvectors when encircling the EP in parameter space was studied, including the geometric amplitude that builds up in the case of broken TRI. A one-dimensional subspace of parameters was found where the differences of the eigenvalues are either real or purely imaginary. There, the Hamiltonians were found PT-invariant under the combined operation of parity (P) and time reversal (T) in a generalized sense. The EP is the point of transition between both regions. There a spontaneous breaking of PT occurs.</p>
<p><a href="http://arxiv.org/abs/1402.3537" target="_blank">http://arxiv.org/abs/1402.3537</a><br />
<span style="background-color: transparent;">Chaotic Dynamics (nlin.CD)</span></p>
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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>
		<comments>http://ptsymmetry.net/?p=509#comments</comments>
		<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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