1993
DOI: 10.1088/0031-8949/1993/t48/021
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Phase properties of Schrödinger cat states of light decaying in phase-sensitive reservoirs

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Cited by 18 publications
(7 citation statements)
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“…2(a) one can see that P (Θ 1 ) exhibits two-peak structure for both collapse time (with two maxima around Θ 1 ≃ ±2π/3) and secondary-revival time (with two maxima around Θ 1 ≃ ±π/2), however, those of the latter are border and shorter than those of the former. In fact such behavior (, i.e., the occurrence of the two-peak structure in the phase distribution) is quite similar to that of the even (odd) coherent states [43]. Furthermore, this behavior is representative to the standard JCM indicating generation of the cat states.…”
Section: B Phase Distributionsupporting
confidence: 57%
“…2(a) one can see that P (Θ 1 ) exhibits two-peak structure for both collapse time (with two maxima around Θ 1 ≃ ±2π/3) and secondary-revival time (with two maxima around Θ 1 ≃ ±π/2), however, those of the latter are border and shorter than those of the former. In fact such behavior (, i.e., the occurrence of the two-peak structure in the phase distribution) is quite similar to that of the even (odd) coherent states [43]. Furthermore, this behavior is representative to the standard JCM indicating generation of the cat states.…”
Section: B Phase Distributionsupporting
confidence: 57%
“…Actually, the phase distribution is insensitive to the interference in phase space, i.e. the phase distribution of the even, odd, Yurke-Stoler and the statistical-mixture coherent states are almost similar [34]. This leads to the fact that the phase distribution is insensitive to the values of ∆, which can change cat states to the statistical-mixture coherent states (see the discussion given in section 3 for the W function).…”
Section: Phase Distribution and Its Variancementioning
confidence: 99%
“…For this reason, in this paper we suggest a new master equation for "isotropic" phase-number squeezing, which is much more efficient in preserving coherence of any general superposition compared to an anisotropic squeezed bath. We analyze coherence by observing the phase (quasi)probability that is marginal of the Wigner function [18][19][20]…”
Section: Introductionmentioning
confidence: 99%