2017
DOI: 10.1103/physreve.95.012136
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Markovian quantum master equation beyond adiabatic regime

Abstract: By introducing a temporal change timescale τA(t) for the time-dependent system Hamiltonian, a general formulation of the Markovian quantum master equation is given to go well beyond the adiabatic regime. In appropriate situations, the framework is well justified even if τA(t) is faster than the decay timescale of the bath correlation function. An application to the dissipative LandauZener model demonstrates this general result. The findings are applicable to a wide range of fields, providing a basis for quantu… Show more

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Cited by 46 publications
(36 citation statements)
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“…We consider an externally driven system interacting with the heat bath, described by the following Lindblad type master equation [27][28][29]…”
Section: Lindblad Master Equationmentioning
confidence: 99%
“…We consider an externally driven system interacting with the heat bath, described by the following Lindblad type master equation [27][28][29]…”
Section: Lindblad Master Equationmentioning
confidence: 99%
“…4 we show the time dependence Q LZ (t) calculated by numerical solution of Eq. (17) for particular value G ω = 0.6, when the Bessel function J 0 (4G/ω) turns to zero. We see that, for this coupling, Q LZ (t) does not change with time in a certain domain around t = 0 suggesting that the effective gap is zero.…”
Section: Fast Oscillatormentioning
confidence: 95%
“…As a final remark, note that by assuming L t (ω β (H t )) = 0 we are neglecting non-adiabatic contributions to L t , which is justified whenever the bath dynamics are fast compared to the driving rate of the system Hamiltonian [28][29][30]. For slow driving of H t , we can assume that the state is always close to the equilibrium one: ρ t = ω β (H t ) + δω t .…”
Section: Metric Structure In Open Quantum Systemsmentioning
confidence: 99%