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	<title>The PT Symmeter &#187; Jia-wen Deng</title>
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		<title>General PT-Symmetric Matrices</title>
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		<pubDate>Tue, 11 Dec 2012 13:08:26 +0000</pubDate>
		<dc:creator>dwh</dc:creator>
				<category><![CDATA[Helmholtz-Zentrum Dresden-Rossendorf]]></category>
		<category><![CDATA[National University of Singapore]]></category>
		<category><![CDATA[Jia-wen Deng]]></category>
		<category><![CDATA[Qing-hai Wang]]></category>
		<category><![CDATA[Uwe Guenther]]></category>

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		<description><![CDATA[Jia-wen Deng, Uwe Guenther, Qing-hai Wang Three ways of constructing a non-Hermitian matrix with possible all real eigenvalues are discussed. They are PT symmetry, pseudo-Hermiticity, and generalized PT symmetry. Parameter counting is provided for each class. All three classes of matrices have more real parameters than a Hermitian matrix with the same dimension. The generalized&#8230;]]></description>
			<content:encoded><![CDATA[<p>Jia-wen Deng, Uwe Guenther, Qing-hai Wang</p>
<p>Three ways of constructing a non-Hermitian matrix with possible all real eigenvalues are discussed. They are PT symmetry, pseudo-Hermiticity, and generalized PT symmetry. Parameter counting is provided for each class. All three classes of matrices have more real parameters than a Hermitian matrix with the same dimension. The generalized PT-symmetric matrices are most general among the three. All self-adjoint matrices process a generalized PT symmetry. For a given matrix, it can be both PT-symmetric and P&#8217;-pseudo-Hermitian with respect to some P&#8217; operators. The relation between corresponding P and P&#8217; operators is established. The Jordan block structures of each class are discussed. Explicit examples in 2&#215;2 are shown.</p>
<p><a href="http://arxiv.org/abs/1212.1861" target="_blank">http://arxiv.org/abs/1212.1861</a><br />
Quantum Physics (quant-ph); Mathematical Physics (math-ph)</p>
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