2006
DOI: 10.1103/physreva.73.022313
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Complete disentanglement by partial pure dephasing

Abstract: We study the effect of pure dephasing on the entanglement of a pair of two-level subsystems (qubits). We show that partial dephasing induced by a super-Ohmic reservoir, corresponding to well-established properties of confined charge states and phonons in semiconductors, may lead to complete disentanglement. We show also that the disentanglement effect increases with growing distance between the two subsystems.Comment: Final, considerably extended version, 6 pages, 4 figure

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Cited by 100 publications
(52 citation statements)
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References 38 publications
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“…Let us notice that the pure dephasing serves as a good approximation of various models studied in wide range of contexts [19,21,22]. Relationship between temperature dependence of the fidelity and the particular choice of initial preparation is well visible in, otherwise not very interesting for teleportation, long time limit lim t→∞ F. In Fig.…”
Section: F(∞)mentioning
confidence: 99%
“…Let us notice that the pure dephasing serves as a good approximation of various models studied in wide range of contexts [19,21,22]. Relationship between temperature dependence of the fidelity and the particular choice of initial preparation is well visible in, otherwise not very interesting for teleportation, long time limit lim t→∞ F. In Fig.…”
Section: F(∞)mentioning
confidence: 99%
“…29 holds true when ω(t) attains its limits ω ± sufficiently fast for t → ±∞, respectively. The quantity σ in (29) can be obtained from the long-time solution x(t) of the equation of motion x + ω 2 (t)x = 0 of a classical oscillator with the frequency ω(t) by imposing a proper boundary condition for x(t) as t → −∞. Because ω(t) → ω + for t → ∞, we expect that for t → ∞ the solution takes the form…”
Section: Non-linear Couplingmentioning
confidence: 98%
“…The operators H ± characterize the subsystem E as well as the details of the interaction between Q and E [2,18]. Note that in a general case the qubit is asymmetrically coupled to the subsystem E. Despite its simplicity, this model has already been applied to study a wide spectrum of various problems like a quantum kicked rotator, chaotic dynamics of a periodically driven superconducting single electron transistor and the Josephson flux qubit [12,24,27,29]. The evolution operator U (t, t 0 ) of the composite system can explicitly be evaluated since the block-diagonal form for the time-shift operator is preserved:…”
Section: Reduced Dynamics and Scattering Operatorsmentioning
confidence: 98%
“…This phenomenon is called entanglement sudden death (ESD). The surprising phenomenon of ESD, contrary to intuition which is based on experience about qubit decoherence, has attracted much attention recently [7][8][9][10][11][12][13][14].…”
Section: Introductionmentioning
confidence: 99%