2010
DOI: 10.1007/s11128-010-0165-2
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Disentanglement and decoherence from classical non-Markovian noise: random telegraph noise

Abstract: We calculate the two-qubit disentanglement due to classical random telegraph noise using the quasi-Hamiltonian method. This allows us to obtain analytical results even for strong coupling and mixed noise, important when the qubits have tunable working point. We determine when entanglement sudden death and revival occur as functions of qubit working point, noise coupling strength and initial state entanglement. For extended Werner states, we show that the concurrence is related to the difference of two function… Show more

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Cited by 65 publications
(59 citation statements)
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“…This model has in common with the one considered in Ref. [19] that the environments are unaffected by the system of interest. However, here the element of randomness is introduced in the phase which can assume only two possible values with assigned and fixed probabilities without switching between them.…”
Section: Modelmentioning
confidence: 99%
See 2 more Smart Citations
“…This model has in common with the one considered in Ref. [19] that the environments are unaffected by the system of interest. However, here the element of randomness is introduced in the phase which can assume only two possible values with assigned and fixed probabilities without switching between them.…”
Section: Modelmentioning
confidence: 99%
“…In Ref. [19] qubits are subject to random telegraph noise, where instead it is the coupling that switches between two values during the evolution.…”
Section: Modelmentioning
confidence: 99%
See 1 more Smart Citation
“…It is worth to notice that the evolved state ρ(t) belongs to the Hilbert space spanned by the Bell states |φ ± = 1 √ 2 (|00 ± |11 ), therefore the entanglement of formation equals the entanglement cost [28]. In the strong coupling regime, g = v/γ > 1 [21,23] entanglement revivals occur during the system dynamics [9,13].…”
Section: Entanglement Dynamicsmentioning
confidence: 99%
“…In some cases, this phenomenon is due to the fact that entanglement is transferred to quantum environments, and then back-transferred to the system [7,8]. In other cases, the environment can be modelled as a classical system [9,11,13] and no entanglement between the system and the environment is established at any time. In the latter cases, the occurrence of entanglement revivals may appear paradoxical, since the effect of the noise is analogous to a local operation on a subsystem.…”
Section: Introductionmentioning
confidence: 99%