2006
DOI: 10.1088/0305-4470/39/35/007
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Generation and some nonclassical properties of a nonlinear finite-dimensional pair coherent state

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Cited by 18 publications
(16 citation statements)
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“…For this reason it is convenient to use the phase distribution formalism introduced by Barnett and Pegg [24,25,28,[30][31][32][33][34][35]. It is well known that the phase operator is defined as the projection operator on a particular phase state multiplied by the corresponding value of the phase.…”
Section: Phase Propertiesmentioning
confidence: 99%
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“…For this reason it is convenient to use the phase distribution formalism introduced by Barnett and Pegg [24,25,28,[30][31][32][33][34][35]. It is well known that the phase operator is defined as the projection operator on a particular phase state multiplied by the corresponding value of the phase.…”
Section: Phase Propertiesmentioning
confidence: 99%
“…On the other hand, the finite dimensional PCS has been studied recently by [24,25] as the eigenstate of the pair operators (â †b + ζ q+1 (âb † ) q (q!) 2 ) and the sum of the photon number operators for the two modes (Q =n a +n b ).…”
Section: Introductionmentioning
confidence: 99%
“…Moreover, their some nonclassical properties have been investigated. The differences in phenomenon between two classes of finite-dimensional PCSs [23,24], the standard PCSs [22] and NLPCSs [25] have also been found. Nonlinear extensions of the single-mode squeezed vacuum and squeezed coherent states are constructed.…”
Section: Introductionmentioning
confidence: 77%
“…Practicaly, the measurement can be performed by photon detectors based on photoelectric effect [23,24]. Theoretically, the nonclassical behavior of the system can be done by examination of its second-order correlation function.…”
Section: Sub-poissonian Distributionsmentioning
confidence: 99%
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