Phase Space Representation for Open Quantum Systems within the Lindblad Theory

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dc.creatorIsar, A.
dc.creatorSandulescu, A.
dc.creatorScheid, W.
dc.date1996-05-29
dc.date.accessioned2026-07-07T10:59:06Z
dc.date.available2026-07-07T10:59:06Z
dc.descriptionThe Lindblad master equation for an open quantum system with a Hamiltonian containing an arbitrary potential is written as an equation for the Wigner distribution function in the phase space representation. The time derivative of this function is given by a sum of three parts: the classical one, the quantum corrections and the contribution due to the opening of the system. In the particular case of a harmonic oscillator, quantum corrections do not exist.
dc.description19 pages, Latex, accepted for publication in Int. J. Mod. Phys. B
dc.identifierhttps://arxiv.org/abs/quant-ph/9605041
dc.identifierhttp://arxiv.org/abs/quant-ph/9605041
dc.identifierInt.J.Mod.Phys.B10:2767,1996
dc.identifierdoi:10.1142/S0217979296001240
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/187336
dc.subjectQuantum Physics
dc.titlePhase Space Representation for Open Quantum Systems within the Lindblad Theory
dc.typetext

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