2016
DOI: 10.1088/1674-1056/25/9/090302
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Discord and entanglement in non-Markovian environments at finite temperatures

Abstract: The dynamics evolutions of discord and entanglement of two atoms in two independent Lorentzian reservoirs at zero or finite temperature have been investigated by using the time-convolutionless master-equation method. Our results show that, when both the non-Markovian effect and the detuning are present simultaneously, due to the memory and feedback effect of the non-Markovian reservoirs, the discord and the entanglement can be effectively protected even at nonzero temperature by increasing the non-Markovian ef… Show more

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Cited by 19 publications
(12 citation statements)
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References 45 publications
(61 reference statements)
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“…where λ is the spectral width of the reservoir and γ is the decay rate of the excited state of the qubit. The condition λ > 2γ and λ < 2γ respectively indicate the weak and strong qubit-cavity coupling regimes [57][58][59]. By substituting Eq.…”
Section: Physical Model and Analytical Solutionmentioning
confidence: 99%
“…where λ is the spectral width of the reservoir and γ is the decay rate of the excited state of the qubit. The condition λ > 2γ and λ < 2γ respectively indicate the weak and strong qubit-cavity coupling regimes [57][58][59]. By substituting Eq.…”
Section: Physical Model and Analytical Solutionmentioning
confidence: 99%
“…where λ is the spectral width of the reservoir, γ is the dissipative rate. The condition λ > 2γ means the weakcoupling regime, while the condition λ < 2γ indicates the strong-coupling regime that the non-Markovian effect is very obviously [38][39][40]. The correlation function F (t−t 1 ) can be calculated as…”
Section: Physical Model and Analytical Solutionmentioning
confidence: 99%
“…For a weak regime we mean the case λ > 2λ 0 , in this regime the behavior of dynamical evolution of the system is essentially a Markovian exponential decay controlled by λ 0 . In the strong coupling regime, for λ < 2λ 0 , non-Markovian effects become relevant [22,23,24]. We consider the spectrum is peaked on the frequency of the state |E 1− , i.e., ω 1 = ω 0 − Ω, the decay rates for the two dressed states |E 1± are respectively expressed as [26]…”
Section: Atom In Dissipative Cavitymentioning
confidence: 99%