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	<title>The PT Symmeter &#187; Zhejiang University</title>
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	<description>PT Symmetry articles and information</description>
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		<title>Type II Perfect Absorption and Amplification Modes with Controllable Bandwidth in PT-Symmetric/Traditional Bragg Grating Combined Structures</title>
		<link>http://ptsymmetry.net/?p=1321&#038;utm_source=rss&#038;utm_medium=rss&#038;utm_campaign=type-ii-perfect-absorption-and-amplification-modes-with-controllable-bandwidth-in-pt-symmetrictraditional-bragg-grating-combined-structures</link>
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		<pubDate>Thu, 01 Aug 2013 01:20:25 +0000</pubDate>
		<dc:creator>dwh</dc:creator>
				<category><![CDATA[Shanghai Jiao Tong University]]></category>
		<category><![CDATA[Zhejiang University]]></category>
		<category><![CDATA[C. Y. Huang]]></category>
		<category><![CDATA[J. L. Han]]></category>
		<category><![CDATA[J. Q. Xu]]></category>
		<category><![CDATA[J. Zheng]]></category>
		<category><![CDATA[R. Zhang]]></category>

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		<description><![CDATA[C. Y. Huang, R. Zhang, J. L. Han, J. Zheng, J. Q. Xu We reveal previously unnoticed Type II perfect absorption and amplification modes of optical scattering system. These modes, in contrast to the counterparts in recent works [Phys. Rev. A 82, 031801 (2010); Phys. Rev. Lett. 106, 093902 (2011).] which could be referred as&#8230;]]></description>
			<content:encoded><![CDATA[<p>C. Y. Huang, R. Zhang, J. L. Han, J. Zheng, J. Q. Xu</p>
<p>We reveal previously unnoticed Type II perfect absorption and amplification modes of optical scattering system. These modes, in contrast to the counterparts in recent works [Phys. Rev. A 82, 031801 (2010); Phys. Rev. Lett. 106, 093902 (2011).] which could be referred as Type I modes, appear at a continuous region along the real frequency axis with any frequency. The Type II modes can be demonstrated in the PT-symmetric/traditional Bragg grating combined structures. A series of exotic nonreciprocal absorption and amplification behaviours are observed in the combined structures, making them have potential for versatile devices acting simultaneously as a perfect absorber, an amplifier, and an ultra-narrowband filter. Based on the properties of Type II modes, we also propose structures with controllable perfect absorption and amplification bandwidth at any single or multiple wavelengths.</p>
<p><a href="http://arxiv.org/abs/1307.7583" target="_blank">http://arxiv.org/abs/1307.7583</a><br />
Optics (physics.optics)</p>
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		<title>A generalized family of discrete PT-symmetric square wells</title>
		<link>http://ptsymmetry.net/?p=1134&#038;utm_source=rss&#038;utm_medium=rss&#038;utm_campaign=a-generalized-family-of-discrete-pt-symmetric-square-wells</link>
		<comments>http://ptsymmetry.net/?p=1134#comments</comments>
		<pubDate>Fri, 08 Feb 2013 08:12:40 +0000</pubDate>
		<dc:creator>dwh</dc:creator>
				<category><![CDATA[Nuclear Physics Institute in Rez]]></category>
		<category><![CDATA[Zhejiang University]]></category>
		<category><![CDATA[Junde Wu]]></category>
		<category><![CDATA[Miloslav Znojil]]></category>

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		<description><![CDATA[Miloslav Znojil, Junde Wu N-site-lattice Hamiltonians H are introduced and perceived as a set of systematic discrete approximants of a certain PT-symmetric square-well-potential model with the real spectrum and with a non-Hermiticity which is localized near the boundaries of the interval. Its strength is controlled by one, two or three parameters. The problem of the&#8230;]]></description>
			<content:encoded><![CDATA[<p>Miloslav Znojil, Junde Wu</p>
<p>N-site-lattice Hamiltonians H are introduced and perceived as a set of systematic discrete approximants of a certain PT-symmetric square-well-potential model with the real spectrum and with a non-Hermiticity which is localized near the boundaries of the interval. Its strength is controlled by one, two or three parameters. The problem of the explicit construction of a nontrivial metric which makes the theory unitary is then addressed. It is proposed and demonstrated that due to the not too complicated tridiagonal-matrix form of our input Hamiltonians the computation of the metric is straightforward and that its matrix elements prove obtainable, non-numerically, in elementary polynomial forms.</p>
<p><a href="http://arxiv.org/abs/1302.1662" target="_blank">http://arxiv.org/abs/1302.1662</a><br />
Quantum Physics (quant-ph); Mathematical Physics (math-ph)</p>
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