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	<title>The PT Symmeter &#187; Surendranath College</title>
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		<title>CPT-conserved effective mass Hamiltonians through first and higher order charge operator C in a supersymmetric framework</title>
		<link>http://ptsymmetry.net/?p=1063&#038;utm_source=rss&#038;utm_medium=rss&#038;utm_campaign=cpt-conserved-effective-mass-hamiltonians-through-first-and-higher-order-charge-operator-c-in-a-supersymmetric-framework</link>
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		<pubDate>Thu, 13 Dec 2012 22:26:13 +0000</pubDate>
		<dc:creator>dwh</dc:creator>
				<category><![CDATA[S.N. Bose National Centre for Basic Sciences]]></category>
		<category><![CDATA[Surendranath College]]></category>
		<category><![CDATA[University of Calcutta]]></category>
		<category><![CDATA[A. Banerjee]]></category>
		<category><![CDATA[A. Ganguly]]></category>
		<category><![CDATA[B. Bagchi]]></category>

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		<description><![CDATA[B. Bagchi, A. Banerjee, A. Ganguly This paper examines the features of a generalized position-dependent mass Hamiltonian in a supersymmetric framework in which the constraints of pseudo-Hermiticity and CPT are naturally embedded. Different representations of the charge operator are considered that lead to new mass-deformed superpotentials which are inherently PT-symmetric. The qualitative spectral behavior of&#8230;]]></description>
			<content:encoded><![CDATA[<p>B. Bagchi, A. Banerjee, A. Ganguly</p>
<p>This paper examines the features of a generalized position-dependent mass Hamiltonian in a supersymmetric framework in which the constraints of pseudo-Hermiticity and CPT are naturally embedded. Different representations of the charge operator are considered that lead to new mass-deformed superpotentials which are inherently PT-symmetric. The qualitative spectral behavior of the Hamiltonian is studied and several interesting consequences are noted.</p>
<p><a href="http://arxiv.org/abs/1212.2122" target="_blank">http://arxiv.org/abs/1212.2122</a><br />
Quantum Physics (quant-ph); High Energy Physics &#8211; Theory (hep-th); Mathematical Physics (math-ph)</p>
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		<title>A generalized non-Hermitian Pais-Uhlenbeck quantum Hamiltonian, its Hermitian equivalence and position-dependent mass correspondence</title>
		<link>http://ptsymmetry.net/?p=1059&#038;utm_source=rss&#038;utm_medium=rss&#038;utm_campaign=a-generalized-non-hermitian-pais-uhlenbeck-quantum-hamiltonian-its-hermitian-equivalence-and-position-dependent-mass-correspondence</link>
		<comments>http://ptsymmetry.net/?p=1059#comments</comments>
		<pubDate>Thu, 13 Dec 2012 22:16:02 +0000</pubDate>
		<dc:creator>dwh</dc:creator>
				<category><![CDATA[S.N. Bose National Centre for Basic Sciences]]></category>
		<category><![CDATA[Surendranath College]]></category>
		<category><![CDATA[University of Calcutta]]></category>
		<category><![CDATA[A. Ghose Choudhury]]></category>
		<category><![CDATA[B. Bagchi]]></category>
		<category><![CDATA[Partha Guha]]></category>

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		<description><![CDATA[B. Bagchi, A. Ghose Choudhury, Partha Guha We explore the Jacobi Last Multiplier as a means for deriving the Lagrangian of a fourth-order differential equation. In particular we consider the classical problem of the Pais-Uhlenbeck oscillator and write down the accompanying Hamiltonian. We then compare such an expression with an alternative derivation of the Hamiltonian&#8230;]]></description>
			<content:encoded><![CDATA[<p>B. Bagchi, A. Ghose Choudhury, Partha Guha</p>
<p>We explore the Jacobi Last Multiplier as a means for deriving the Lagrangian of a fourth-order differential equation. In particular we consider the classical problem of the Pais-Uhlenbeck oscillator and write down the accompanying Hamiltonian. We then compare such an expression with an alternative derivation of the Hamiltonian that makes use of the Ostrogradski&#8217;s method and show that a mapping from the one to the other is achievable by variable transformations. Assuming canonical quantization procedure to be valid we go for the operator version of the Hamiltonian that represents a pair of uncoupled oscillators. This motivates us to propose a generalized Pais-Uhlenbeck Hamiltonian in terms of the usual harmonic oscillator creation and annihilation operators by including terms quadratic and linear in them. Such a Hamiltonian turns out to be essentially non-Hermitian but has an equivalent Hermitian representation which is reducible to a typically position-dependent reduced mass form.<br />
<a href=" http://arxiv.org/abs/1212.2092" target="_blank"></p>
<p>http://arxiv.org/abs/1212.2092</a></p>
<p>Mathematical Physics (math-ph); Quantum Physics (quant-ph)</p>
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