2010
DOI: 10.1016/j.physleta.2010.08.076
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Phase space structure of generalized Gaussian cat states

Abstract: We analyze generalized Gaussian cat states obtained by superposing arbitrary Gaussian states, e.g., a coherent state and a squeezed state. The Wigner functions of such states exhibit the typical pair of Gaussian hills plus an interference term which presents a novel structure, as compared with the standard superposition of coherent states (degenerate case). We prove that, in any dimensions, the structure of the interference term is characterized by a particular quadratic form; in one degree of freedom the phas… Show more

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Cited by 22 publications
(33 citation statements)
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“…We can however not apply directly formula (53) since S is not a Hilbert-Schmidt operator. Let us proceed as follows: in view of formula (39) in Proposition 12. The twisted Weyl symbol c σ of C is given by the absolutely convergent integral…”
Section: A General Resultsmentioning
confidence: 99%
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“…We can however not apply directly formula (53) since S is not a Hilbert-Schmidt operator. Let us proceed as follows: in view of formula (39) in Proposition 12. The twisted Weyl symbol c σ of C is given by the absolutely convergent integral…”
Section: A General Resultsmentioning
confidence: 99%
“…However, any quantum state can be expanded as a superposition of (Gaussian) coherent states, thus this method can be applied to the propagation of any initial state [9,32]. An example for the propagation of states under a non-linear (and classically chaotic) Hamiltonian dynamics is given in [39].…”
Section: Discussion and Perspectivesmentioning
confidence: 99%
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“…(See the appendix C or [36][37][38][39] for the derivation.) From here, the application of the map in an infinitesimal time δt can be identified as:…”
Section: Fdt For Lindbladian Master Equationsmentioning
confidence: 99%
“…Being quadratic the master equation Eq. (3) evolves Gaussian states to Gaussian states [62][63][64]. Eq.…”
Section: Introductionmentioning
confidence: 99%