2019
DOI: 10.1016/j.aop.2019.03.027
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Obtaining phase-optimized states from superpositions of coherent states in phase-sensitive attenuating/amplifying reservoirs

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Cited by 2 publications
(3 citation statements)
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“…which corresponds to the amplitude-attenuated coherent state |αe −κt/2 ; this means that the coherent state |α , in the presence of a dissipating reservoir at zero-temperature, evolves in time remaining a pure coherent state but with an exponentially damped intensity, the mean number of photons (the energy) given by a † a = |α| 2 e −κt . Exactly the same result is achieved by solving the master equation (5) in the Wigner representation, using the Green's function method [3][4][5].…”
Section: Time Evolution In a Dissipative Environmentmentioning
confidence: 94%
“…which corresponds to the amplitude-attenuated coherent state |αe −κt/2 ; this means that the coherent state |α , in the presence of a dissipating reservoir at zero-temperature, evolves in time remaining a pure coherent state but with an exponentially damped intensity, the mean number of photons (the energy) given by a † a = |α| 2 e −κt . Exactly the same result is achieved by solving the master equation (5) in the Wigner representation, using the Green's function method [3][4][5].…”
Section: Time Evolution In a Dissipative Environmentmentioning
confidence: 94%
“…[75,76] Recently, the generation of a superposition of CSs, which can approximately be regarded as the ideal phase states, has been examined in high-Q microwave cavity. [77] To discuss the phase properties of a given state of a singlemode quantized field, both Susskind-Glogower and Pegg-Barnett constructions may be applied. Based on the latter, [78] observables are described in an (s + 1)-dimensional Hilbert space and as a result, the complete set of (s + 1) orthonormal phase states is defined by wherêdetermines the density operator of the field.…”
Section: Phase Entropic Squeezingmentioning
confidence: 99%
“…[ 75,76 ] Recently, the generation of a superposition of CSs, which can approximately be regarded as the ideal phase states, has been examined in high‐Q microwave cavity. [ 77 ]…”
Section: Conditions For Nonclassicalitymentioning
confidence: 99%