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	<title>The PT Symmeter &#187; O. Cherbal</title>
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		<title>Supersymmetric extension of non-Hermitian su(2) Hamiltonians and supercoherent states</title>
		<link>http://ptsymmetry.net/?p=68&#038;utm_source=rss&#038;utm_medium=rss&#038;utm_campaign=supersymmetric-extension-of-non-hermitian-su2-hamiltonians-and-supercoherent-states</link>
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		<pubDate>Tue, 28 Sep 2010 10:28:35 +0000</pubDate>
		<dc:creator>dwh</dc:creator>
				<category><![CDATA[Institute of Nuclear Research in Sofia]]></category>
		<category><![CDATA[Setif University]]></category>
		<category><![CDATA[USTHB]]></category>
		<category><![CDATA[D.A. Trifonov]]></category>
		<category><![CDATA[M. Drir]]></category>
		<category><![CDATA[M. Maamache]]></category>
		<category><![CDATA[O. Cherbal]]></category>

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		<description><![CDATA[O. Cherbal, M. Drir, M. Maamache, D.A. Trifonov A new class of non-Hermitian Hamiltonians with real spectrum, which are written as a real linear combination of su(2) generators is analyzed. The metric which allows the transition to the equivalent Hermitian Hamiltonian is established. A pseudo-Hermitian supersymmetic extension of such Hamiltonians is performed, which correspond to&#8230;]]></description>
			<content:encoded><![CDATA[<p>O. Cherbal, M. Drir, M. Maamache, D.A. Trifonov</p>
<p>A new class of non-Hermitian Hamiltonians with real spectrum, which are written as a real linear combination of su(2) generators is analyzed. The metric which allows the transition to the equivalent Hermitian Hamiltonian is established. A pseudo-Hermitian supersymmetic extension of such Hamiltonians is performed, which correspond to the pseudo-Hermitian supersymmetric system of the boson-phermion oscillator. We extend the supercoherent states formalism to such supersymmetic systems via the pseudo-unitary supersymmetric displacement operator method. The constructed family of these supercoherent states consists of two dual subfamilies that form a bi-overcomplete and bi-normal system in the boson-phermion Fock space. The states of each subfamily are eigenvectors of the boson annihilation operator and of one of the two phermion lowering operators.</p>
<p><a target="_blank" href="http://arxiv.org/abs/1009.5293">http://arxiv.org/abs/1009.5293</a><br />
Quantum Physics (quant-ph)</p>
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