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	<title>The PT Symmeter &#187; Ananya Ghatak</title>
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	<link>http://ptsymmetry.net</link>
	<description>PT Symmetry articles and information</description>
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		<title>Reciprocity in parity violating non-Hermitian systems</title>
		<link>http://ptsymmetry.net/?p=1852&#038;utm_source=rss&#038;utm_medium=rss&#038;utm_campaign=reciprocity-in-parity-violating-non-hermitian-systems</link>
		<comments>http://ptsymmetry.net/?p=1852#comments</comments>
		<pubDate>Thu, 30 Oct 2014 20:53:59 +0000</pubDate>
		<dc:creator>dwh</dc:creator>
				<category><![CDATA[Banaras Hindu University]]></category>
		<category><![CDATA[Ananya Ghatak]]></category>
		<category><![CDATA[Bhabani Prasad Mandal (BHU)]]></category>
		<category><![CDATA[Brijesh Kumar Mourya]]></category>
		<category><![CDATA[Raka Dona Ray Mandal]]></category>

		<guid isPermaLink="false">http://ptsymmetry.net/?p=1852</guid>
		<description><![CDATA[Ananya Ghatak, Brijesh Kumar Mourya, Raka Dona Ray Mandal, Bhabani Prasad Mandal (BHU) Reciprocity is shown so far only when the scattering potential is either real or parity symmetric complex. We extend this result for parity violating complex potential by considering several explicit examples: (i) we show reciprocity for a PT symmetric (hence parity violating)&#8230;]]></description>
			<content:encoded><![CDATA[<p>Ananya Ghatak, Brijesh Kumar Mourya, Raka Dona Ray Mandal, Bhabani Prasad Mandal (BHU)</p>
<p>Reciprocity is shown so far only when the scattering potential is either real or parity symmetric complex. We extend this result for parity violating complex potential by considering several explicit examples: (i) we show reciprocity for a PT symmetric (hence parity violating) complex potential which admits penetrating state solutions analytically for all possible values of incidence energy and (ii) reciprocity is shown to hold at certain discrete energies for two other parity violating complex potentials.</p>
<p><a href="http://arxiv.org/abs/1410.7886" target="_blank">http://arxiv.org/abs/1410.7886</a><br />
Quantum Physics (quant-ph); High Energy Physics &#8211; Theory (hep-th)</p>
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		<title>Critical coupling and coherent perfect absorption for ranges of energies due to a complex gain and loss symmetric system</title>
		<link>http://ptsymmetry.net/?p=1563&#038;utm_source=rss&#038;utm_medium=rss&#038;utm_campaign=critical-coupling-and-coherent-perfect-absorption-for-ranges-of-energies-due-to-a-complex-gain-and-loss-symmetric-system</link>
		<comments>http://ptsymmetry.net/?p=1563#comments</comments>
		<pubDate>Tue, 04 Mar 2014 10:20:02 +0000</pubDate>
		<dc:creator>dwh</dc:creator>
				<category><![CDATA[Banaras Hindu University]]></category>
		<category><![CDATA[Ananya Ghatak]]></category>
		<category><![CDATA[Bhabani Prasad Mandal]]></category>
		<category><![CDATA[Mohammad Hasan]]></category>

		<guid isPermaLink="false">http://ptsymmetry.net/?p=1563</guid>
		<description><![CDATA[Mohammad Hasan, Ananya Ghatak, Bhabani Prasad Mandal We consider a non-Hermitian medium with a gain and loss symmetric, exponentially damped potential distribution to demonstrate different scattering features analytically. The condition for critical coupling (CC) for unidirectional wave and coherent perfect absorption (CPA) for bidirectional waves are obtained analytically for this system. The energy points at&#8230;]]></description>
			<content:encoded><![CDATA[<p>Mohammad Hasan, Ananya Ghatak, Bhabani Prasad Mandal</p>
<p>We consider a non-Hermitian medium with a gain and loss symmetric, exponentially damped potential distribution to demonstrate different scattering features analytically. The condition for critical coupling (CC) for unidirectional wave and coherent perfect absorption (CPA) for bidirectional waves are obtained analytically for this system. The energy points at which total absorption occurs are shown to be the spectral singular points for the time reversed system. The possible energies at which CC occurs for left and right incidence are different. We further obtain periodic intervals with increasing periodicity of energy for CC and CPA to occur in this system.<br />
<a href=" http://arxiv.org/abs/1403.0539" target="_blank"></p>
<p>http://arxiv.org/abs/1403.0539</a></p>
<p>Quantum Physics (quant-ph)</p>
]]></content:encoded>
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		<title>Various Scattering Properties of a New PT-symmetric non-Hermitian potential</title>
		<link>http://ptsymmetry.net/?p=1400&#038;utm_source=rss&#038;utm_medium=rss&#038;utm_campaign=various-scattering-properties-of-a-new-pt-symmetric-non-hermitian-potential</link>
		<comments>http://ptsymmetry.net/?p=1400#comments</comments>
		<pubDate>Wed, 30 Oct 2013 10:29:07 +0000</pubDate>
		<dc:creator>dwh</dc:creator>
				<category><![CDATA[Banaras Hindu University]]></category>
		<category><![CDATA[Rajghat Besant School]]></category>
		<category><![CDATA[Ananya Ghatak]]></category>
		<category><![CDATA[Bhabani Prasad Mandal (BHU)]]></category>
		<category><![CDATA[Raka Dona Ray Mandal]]></category>

		<guid isPermaLink="false">http://ptsymmetry.net/?p=1400</guid>
		<description><![CDATA[Ananya Ghatak, Raka Dona Ray Mandal, Bhabani Prasad Mandal (BHU) We complexify a 1-d potential which exhibits bound, reflecting and free states to study various properties of a non-Hermitian system. This potential turns out a PT-symmetric non-Hermitian potential when one of the parameters becomes imaginary. For one PT-symmetric case we have entire real bound state&#8230;]]></description>
			<content:encoded><![CDATA[<p>Ananya Ghatak, Raka Dona Ray Mandal, Bhabani Prasad Mandal (BHU)</p>
<p>We complexify a 1-d potential which exhibits bound, reflecting and free states to study various properties of a non-Hermitian system. This potential turns out a PT-symmetric non-Hermitian potential when one of the parameters becomes imaginary. For one PT-symmetric case we have entire real bound state spectrum. Explicit scattering states are constructed to show reciprocity at certain discrete values of energy even though the potential is not parity symmetric. Coexistence of deep energy minima of transmissivity with the multiple spectral singularities (MSS) is observed. We further show that this potential becomes invisible from left (or right) at certain discrete energies. The penetrating states in the other PT-symmetric configuration are always reciprocal even though it is PT-invariant and no spectral singularity (SS) is present in this case. Presence of MSS and reflectionlessness are also discussed for the free states in the later case.<br />
<a href=" http://arxiv.org/abs/1310.7752" target="_blank"></p>
<p>http://arxiv.org/abs/1310.7752</a></p>
<p>Quantum Physics (quant-ph)</p>
]]></content:encoded>
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		<title>Comparison of different approaches of finding the positive definite metric in pseudo-Hermitian theories</title>
		<link>http://ptsymmetry.net/?p=1222&#038;utm_source=rss&#038;utm_medium=rss&#038;utm_campaign=comparison-of-different-approaches-of-finding-the-positive-definite-metric-in-pseudo-hermitian-theories</link>
		<comments>http://ptsymmetry.net/?p=1222#comments</comments>
		<pubDate>Fri, 10 May 2013 18:47:40 +0000</pubDate>
		<dc:creator>dwh</dc:creator>
				<category><![CDATA[Banaras Hindu University]]></category>
		<category><![CDATA[Ananya Ghatak]]></category>
		<category><![CDATA[Bhabani Prasad Mandal]]></category>

		<guid isPermaLink="false">http://ptsymmetry.net/?p=1222</guid>
		<description><![CDATA[Ananya Ghatak, Bhabani Prasad Mandal To develop a unitary quantum theory with probabilistic description for pseudo- Hermitian systems one needs to consider the theories in a different Hilbert space endowed with a positive definite metric operator. There are different approaches to find such metric operators. We compare the different approaches of calculating pos- itive definite&#8230;]]></description>
			<content:encoded><![CDATA[<p>Ananya Ghatak, Bhabani Prasad Mandal</p>
<p>To develop a unitary quantum theory with probabilistic description for pseudo- Hermitian systems one needs to consider the theories in a different Hilbert space endowed with a positive definite metric operator. There are different approaches to find such metric operators. We compare the different approaches of calculating pos- itive definite metric operators in pseudo-Hermitian theories with the help of several explicit examples in non-relativistic as well as in relativistic situations. Exceptional points and spontaneous symmetry breaking are also discussed in these models.</p>
<p><a href="http://arxiv.org/abs/1305.2022" target="_blank">http://arxiv.org/abs/1305.2022</a><br />
Quantum Physics (quant-ph); High Energy Physics &#8211; Theory (hep-th)</p>
]]></content:encoded>
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		<title>Spectral singularity and non-Hermitian PT-symmetric extension of \(A_{N-1}\) type Calogero model without confining potential</title>
		<link>http://ptsymmetry.net/?p=951&#038;utm_source=rss&#038;utm_medium=rss&#038;utm_campaign=spectral-singularity-and-non-hermitian-pt-symmetric-extension-of-a_n-1-type-calogero-model-without-confining-potential</link>
		<comments>http://ptsymmetry.net/?p=951#comments</comments>
		<pubDate>Wed, 05 Sep 2012 12:58:12 +0000</pubDate>
		<dc:creator>dwh</dc:creator>
				<category><![CDATA[Banaras Hindu University]]></category>
		<category><![CDATA[Ananya Ghatak]]></category>
		<category><![CDATA[Bhabani Prasad Mandal]]></category>

		<guid isPermaLink="false">http://ptsymmetry.net/?p=951</guid>
		<description><![CDATA[Bhabani Prasad Mandal, Ananya Ghatak We consider non-Hermitian PT-symmetric deformation of \(A_{N-1}\) type Calogero model without confining potential to investigate the possible existence of spectral singularity. By considering the Wronskian between asymptotic incoming and outgoing scattering state wave functions, we found that there exist no spectral singularity in this model. We further explicitly show that&#8230;]]></description>
			<content:encoded><![CDATA[<p>Bhabani Prasad Mandal, Ananya Ghatak</p>
<p>We consider non-Hermitian PT-symmetric deformation of \(A_{N-1}\) type Calogero model without confining potential to investigate the possible existence of spectral singularity. By considering the Wronskian between asymptotic incoming and outgoing scattering state wave functions, we found that there exist no spectral singularity in this model. We further explicitly show that the transmission coefficient vanishes and the reflection coefficient becomes unity for all values of the energy in such a momentum dependent non-Hermitian PT-symmetric model.</p>
<p><a href="http://arxiv.org/abs/1209.0535" target="_blank">http://arxiv.org/abs/1209.0535</a><br />
Mathematical Physics (math-ph); High Energy Physics &#8211; Theory (hep-th); Quantum Physics (quant-ph)</p>
]]></content:encoded>
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		<title>Spectral singularity and deep multiple minima in the reflectivity in non-Hermitian (complex) Ginocchio potential</title>
		<link>http://ptsymmetry.net/?p=868&#038;utm_source=rss&#038;utm_medium=rss&#038;utm_campaign=spectral-singularity-and-deep-multiple-minima-in-the-reflectivity-in-non-hermitian-complex-ginocchio-potential</link>
		<comments>http://ptsymmetry.net/?p=868#comments</comments>
		<pubDate>Tue, 10 Jul 2012 07:44:14 +0000</pubDate>
		<dc:creator>dwh</dc:creator>
				<category><![CDATA[Banaras Hindu University]]></category>
		<category><![CDATA[Bhabha Atomic Research Centre]]></category>
		<category><![CDATA[Ananya Ghatak]]></category>
		<category><![CDATA[Bhabani Prasad Mandal]]></category>
		<category><![CDATA[Zafar Ahmed]]></category>

		<guid isPermaLink="false">http://ptsymmetry.net/?p=868</guid>
		<description><![CDATA[Ananya Ghatak, Bhabani Prasad Mandal, Zafar Ahmed We bring out the existence of at most one spectral singularity (SS) and deep multiple minima in the reflectivity of the non-Hermitian (complex) Ginocchio potential. We find a parameter dependent single spectral singularity in this potential provided the imaginary part is emissive (not absorptive). The reflectionlessness of the&#8230;]]></description>
			<content:encoded><![CDATA[<p>Ananya Ghatak, Bhabani Prasad Mandal, Zafar Ahmed</p>
<p>We bring out the existence of at most one spectral singularity (SS) and deep multiple minima in the reflectivity of the non-Hermitian (complex) Ginocchio potential. We find a parameter dependent single spectral singularity in this potential provided the imaginary part is emissive (not absorptive). The reflectionlessness of the real Hermitian Ginocchio&#8217;s potential at discrete positive energies gives way to deep multiple minima in reflectivity when this potential is perturbed and made non-Hermitian (complex). A novel co-existence of a SS with deep minima in reflectivity is also revealed wherein the first reflectivity zero of the Hermitian case changes to become a SS for the non-Hermitian case.<br />
<a href=" http://arxiv.org/abs/1207.1979" target="_blank"></p>
<p>http://arxiv.org/abs/1207.1979</a></p>
<p>Quantum Physics (quant-ph)</p>
]]></content:encoded>
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		<title>Entangled Quantum State Discrimination using Pseudo-Hermitian System</title>
		<link>http://ptsymmetry.net/?p=709&#038;utm_source=rss&#038;utm_medium=rss&#038;utm_campaign=entangled-quantum-state-discrimination-using-pseudo-hermitian-system</link>
		<comments>http://ptsymmetry.net/?p=709#comments</comments>
		<pubDate>Tue, 14 Feb 2012 16:40:04 +0000</pubDate>
		<dc:creator>dwh</dc:creator>
				<category><![CDATA[Banaras Hindu University]]></category>
		<category><![CDATA[Ananya Ghatak]]></category>
		<category><![CDATA[Bhabani Prasad Mandal]]></category>

		<guid isPermaLink="false">http://ptsymmetry.net/?p=709</guid>
		<description><![CDATA[Ananya Ghatak, Bhabani Prasad Mandal We demonstrate how to discriminate two non-orthogonal, entangled quantum state which are slightly different from each other by using pseudo-Hermitian system. The positive definite metric operator which makes the pseudo-Hermitian systems fully consistent quantum theory is used for such a state discrimination. We further show that non-orthogonal states can evolve&#8230;]]></description>
			<content:encoded><![CDATA[<p>Ananya Ghatak, Bhabani Prasad Mandal</p>
<p>We demonstrate how to discriminate two non-orthogonal, entangled quantum state which are slightly different from each other by using pseudo-Hermitian system. The positive definite metric operator which makes the pseudo-Hermitian systems fully consistent quantum theory is used for such a state discrimination. We further show that non-orthogonal states can evolve through a suitably constructed pseudo-Hermitian Hamiltonian to orthogonal states. Such evolution ceases at exceptional points of the pseudo-Hermitian system.</p>
<p><a href="http://arxiv.org/abs/1202.2413" target="_blank">http://arxiv.org/abs/1202.2413</a><br />
Quantum Physics (quant-ph); Mathematical Physics (math-ph)</p>
]]></content:encoded>
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