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	<title>The PT Symmeter &#187; Advanced Centre for Nonlinear and Complex Phenomena</title>
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		<title>Nonlinear localized modes in PT-symmetric optical media with competing gain and loss</title>
		<link>http://ptsymmetry.net/?p=1279&#038;utm_source=rss&#038;utm_medium=rss&#038;utm_campaign=nonlinear-localized-modes-in-pt-symmetric-optical-media-with-competing-gain-and-loss</link>
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		<pubDate>Wed, 26 Jun 2013 06:35:19 +0000</pubDate>
		<dc:creator>dwh</dc:creator>
				<category><![CDATA[Advanced Centre for Nonlinear and Complex Phenomena]]></category>
		<category><![CDATA[Indian Institute of Science Education and Research]]></category>
		<category><![CDATA[Bikashkali Midya]]></category>
		<category><![CDATA[Rajkumar Roychoudhury]]></category>

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		<description><![CDATA[Bikashkali Midya, Rajkumar Roychoudhury The existence and stability of the nonlinear spatial localized modes are investigated in parity-time symmetric optical media characterized by a generic complex hyperbolic refractive index distribution with competing gain and loss profile. The exact analytical expressions of the localized modes are found for all values of the competing parameter and in&#8230;]]></description>
			<content:encoded><![CDATA[<p>Bikashkali Midya, Rajkumar Roychoudhury</p>
<p>The existence and stability of the nonlinear spatial localized modes are investigated in parity-time symmetric optical media characterized by a generic complex hyperbolic refractive index distribution with competing gain and loss profile. The exact analytical expressions of the localized modes are found for all values of the competing parameter and in the presence of both the self-focusing and self-defocusing Kerr nonlinearity. The effect of competing gain/loss profile on the stability structure of these localized modes are discussed with the help of linear stability analysis followed by the direct numerical simulation of the governing equation. The spatial localized modes in two-dimensional geometry as well as the transverse power-flow density associated with these localized modes are also examined.<br />
<a href=" http://arxiv.org/abs/1306.5983" target="_blank"></p>
<p>http://arxiv.org/abs/1306.5983</a></p>
<p>Optics (physics.optics)</p>
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		<title>Scattering in a varying mass PT symmetric double heterojunction</title>
		<link>http://ptsymmetry.net/?p=1263&#038;utm_source=rss&#038;utm_medium=rss&#038;utm_campaign=scattering-in-a-varying-mass-pt-symmetric-double-heterojunction</link>
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		<pubDate>Tue, 11 Jun 2013 05:04:17 +0000</pubDate>
		<dc:creator>dwh</dc:creator>
				<category><![CDATA[Advanced Centre for Nonlinear and Complex Phenomena]]></category>
		<category><![CDATA[Jadavpur University]]></category>
		<category><![CDATA[Anjana Sinha]]></category>
		<category><![CDATA[R. Roychoudhury]]></category>

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		<description><![CDATA[Anjana Sinha, R. Roychoudhury We observe that the reflection and transmission coefficients of a particle within a double, PT-symmetric heterojunction with spatially varying mass, show interesting features, depending on the degree of non Hermiticity, although there is no spontaneous breakdown of PT symmetry. The potential profile in the intermediate layer is considered such that it&#8230;]]></description>
			<content:encoded><![CDATA[<p>Anjana Sinha, R. Roychoudhury</p>
<p>We observe that the reflection and transmission coefficients of a particle within a double, PT-symmetric heterojunction with spatially varying mass, show interesting features, depending on the degree of non Hermiticity, although there is no spontaneous breakdown of PT symmetry. The potential profile in the intermediate layer is considered such that it has a non vanishing imaginary part near the heterojunctions. Exact analytical solutions for the wave function are obtained, and the reflection and transmission coefficients are plotted as a function of energy, for both left as well as right incidence. As expected, the spatial dependence on mass changes the nature of the scattering solutions within the heterojunctions, and the space-time (PT) symmetry is responsible for the left-right asymmetry in the reflection and transmission coefficients. However, the non vanishing imaginary component of the potential near the heterojunctions gives new and interesting results.<br />
<a href=" http://arxiv.org/abs/1306.2226" target="_blank"></p>
<p>http://arxiv.org/abs/1306.2226</a></p>
<p>Quantum Physics (quant-ph); Mathematical Physics (math-ph)</p>
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