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	<title>The PT Symmeter &#187; Joao Caldeira</title>
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		<title>PT-symmetric quantum state discrimination</title>
		<link>http://ptsymmetry.net/?p=116&#038;utm_source=rss&#038;utm_medium=rss&#038;utm_campaign=pt-symmetric-quantum-state-discrimination</link>
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		<pubDate>Sat, 13 Nov 2010 04:18:34 +0000</pubDate>
		<dc:creator>dwh</dc:creator>
				<category><![CDATA[Imperial College London]]></category>
		<category><![CDATA[Washington University in St Louis]]></category>
		<category><![CDATA[Bernard K. Meister]]></category>
		<category><![CDATA[Carl M. Bender]]></category>
		<category><![CDATA[Dorje C. Brody]]></category>
		<category><![CDATA[Joao Caldeira]]></category>

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		<description><![CDATA[Carl M. Bender, Dorje C. Brody, Joao Caldeira, Bernard K. Meister Suppose that a system is known to be in one of two quantum states, $&#124;\psi_1 &#62; $ or $&#124;\psi_2 &#62;$. If these states are not orthogonal, then in conventional quantum mechanics it is impossible with one measurement to determine with certainty which state the&#8230;]]></description>
			<content:encoded><![CDATA[<p>Carl M. Bender, Dorje C. Brody, Joao Caldeira, Bernard K. Meister</p>
<p>Suppose that a system is known to be in one of two quantum states, $|\psi_1 &gt; $ or $|\psi_2 &gt;$. If these states are not orthogonal, then in conventional quantum mechanics it is impossible with one measurement to determine with certainty which state the system is in. However, because a non-Hermitian PT-symmetric Hamiltonian determines the inner product that is appropriate for the Hilbert space of physical states, it is always possible to choose this inner product so that the two states $|\psi_1 &gt; $ and $|\psi_2 &gt; $ are orthogonal. Thus, quantum state discrimination can, in principle, be achieved with a single measurement.</p>
<p><a href="http://arxiv.org/abs/1011.1871" target="_blank">http://arxiv.org/abs/1011.1871</a><br />
High Energy Physics &#8211; Theory (hep-th); Mathematical Physics (math-ph); Quantum Physics (quant-ph)</p>
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