2015
DOI: 10.1103/physreve.92.032123
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Dissipative dynamics in a quantum bistable system: Crossover from weak to strong damping

Abstract: The dissipative dynamics of a quantum bistable system coupled to a Ohmic heat bath is investigated beyond the spin-boson approximation. Within the path-integral approach to quantum dissipation, we propose an approximation scheme which exploits the separation of time scales between intra-and interwell (tunneling) dynamics. The resulting generalized master equation for the populations in a space localized basis enables us to investigate a wide range of temperatures and system-environment coupling strengths. A ph… Show more

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Cited by 21 publications
(27 citation statements)
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“…In [46], by using a beyond-NIBA scheme we have investigated this crossover dynamical regime in the Ohmic case down to temperatures for which NIBA-like approximations break down.…”
Section: J Stat Mech (2016) 054016mentioning
confidence: 99%
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“…In [46], by using a beyond-NIBA scheme we have investigated this crossover dynamical regime in the Ohmic case down to temperatures for which NIBA-like approximations break down.…”
Section: J Stat Mech (2016) 054016mentioning
confidence: 99%
“…Equation (17) does not capture transient oscillations and is accurate only in the fully incoherent regime. Nevertheless it gives a good estimate for the relaxation time also in the crossover dynamical regime [46]. The master equation (17) has been used to obtain the dynamics and stationary populations in the presence of an external driving [47] and to address the problem of the escape from a quantum metastable state, starting from a nonequilibrium initial condition, with a strongly asymmetric bistable potential and Ohmic dissipation [48].…”
Section: J Stat Mech (2016) 054016mentioning
confidence: 99%
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“…At strong coupling this process is well approximated [171] by the incoherent relaxation captured by the master equation [172] …”
Section: Strong Dissipation: Analytical Approachmentioning
confidence: 99%
“…Note that spatial continuity is recovered for M → ∞, i.e., removing the upper bound on the energies taken into account. The existence of intermediate localized states in the generalization of the two-state system treatment accomplished by the DVR is reflected by the multiple time scales resulting from the inclusion of energy levels above the first doublet and accounts for tunneling and intra-well relaxation [87,171].…”
Section: Discrete Variable Representationmentioning
confidence: 99%