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	<title>The PT Symmeter &#187; I. Vitebskiy</title>
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		<title>PT-Symmetric Talbot Effects</title>
		<link>http://ptsymmetry.net/?p=964&#038;utm_source=rss&#038;utm_medium=rss&#038;utm_campaign=pt-symmetric-talbot-effects</link>
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		<pubDate>Wed, 12 Sep 2012 11:39:24 +0000</pubDate>
		<dc:creator>dwh</dc:creator>
				<category><![CDATA[Air Force Research Laboratory]]></category>
		<category><![CDATA[Max-Planck-Institute for Dynamics and Self-Organization]]></category>
		<category><![CDATA[University of Central Florida]]></category>
		<category><![CDATA[Wesleyan University]]></category>
		<category><![CDATA[D. N. Christodoulides]]></category>
		<category><![CDATA[Hamidreza Ramezani]]></category>
		<category><![CDATA[I. Vitebskiy]]></category>
		<category><![CDATA[Tsampikos Kottos]]></category>
		<category><![CDATA[V. Kovanis]]></category>

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		<description><![CDATA[Hamidreza Ramezani, D. N. Christodoulides, V. Kovanis, I. Vitebskiy, Tsampikos Kottos We show that complex PT-symmetric photonic lattices can lead to a new class of self-imaging Talbot effects. For this to occur, we find that the input field pattern, has to respect specific periodicities which are dictated by the symmetries of the system. While at&#8230;]]></description>
			<content:encoded><![CDATA[<p>Hamidreza Ramezani, D. N. Christodoulides, V. Kovanis, I. Vitebskiy, Tsampikos Kottos</p>
<p>We show that complex PT-symmetric photonic lattices can lead to a new class of self-imaging Talbot effects. For this to occur, we find that the input field pattern, has to respect specific periodicities which are dictated by the symmetries of the system. While at the spontaneous PT-symmetry breaking point, the image revivals occur at Talbot lengths governed by the characteristics of the passive lattice, at the exact phase it depends on the gain and loss parameter thus allowing one to control the imaging process.<br />
<a href=" http://arxiv.org/abs/1209.2349" target="_blank"></p>
<p>http://arxiv.org/abs/1209.2349</a></p>
<p>Optics (physics.optics); Other Condensed Matter (cond-mat.other); Quantum Physics (quant-ph)</p>
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