2010
DOI: 10.1103/physreva.81.042103
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Exact master equations for the non-Markovian decay of a qubit

Abstract: Exact master equations describing the decay of a two-state system into a structured reservoir are constructed. Employing the exact solution for the model we determine analytical expressions for the memory kernel of the Nakajima-Zwanzig master equation and for the generator of the corresponding time-convolutionless master equation. This approach allows a detailed investigation and comparison of the convergence behavior of the corresponding perturbation expansions. Moreover, we find that the structure of widely … Show more

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Cited by 129 publications
(143 citation statements)
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“…Besides, we can see from Eqs. (16) and (17) that for a sufficiently high-temperature environment, i.e.,hω c k B T , the phase-damping factor, which is the main agent responsible for the decoherence, behaves as (t,T ) ≈ ηω T t, causing an exponential decay of the off-diagonal elements of the density operator. Moreover, as the phase factor (t) implies an oscillation with frequency ηω c , this time evolution is always slightly underdamped.…”
Section: Exact Dissipative Dynamicsmentioning
confidence: 99%
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“…Besides, we can see from Eqs. (16) and (17) that for a sufficiently high-temperature environment, i.e.,hω c k B T , the phase-damping factor, which is the main agent responsible for the decoherence, behaves as (t,T ) ≈ ηω T t, causing an exponential decay of the off-diagonal elements of the density operator. Moreover, as the phase factor (t) implies an oscillation with frequency ηω c , this time evolution is always slightly underdamped.…”
Section: Exact Dissipative Dynamicsmentioning
confidence: 99%
“…The state fidelity (24) will present an oscillatory behavior in the quantum regime (ω c ω T ), where the exponential decay factor (17) plays a minor role compared to the oscillatory factor (16), and the quantum vacuum fluctuations contribute predominantly. Although Eq.…”
Section: Fidelity Dynamics In An Mbqcmentioning
confidence: 99%
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“…In the context, the general exponential memory kernel function is considered as f (t) = A exp(−γt) where A is the amplitude of the kernel and γ represents the memory decaying rate. This kind of memory kernel can be physically modeled by [30]. The definite expression of the matrix P can be obtained by…”
Section: The Completely Positive Reduced Dynamical Mapmentioning
confidence: 99%
“…72,73,79 There are also numerous non-Markovian generalizations of the master equation. [80][81][82][83] In the above derivation it was assumed that the system is weakly coupled to the environment. Indeed, for practical purposes this is the most interesting case: if the coupling of the system to the environment is strong, the system behaves classically and can be described with classical equations of motion, while if the coupling is absent altogether, eqn (1) is valid.…”
Section: This Journal Is C the Owner Societies 2010mentioning
confidence: 99%