2009
DOI: 10.1088/1367-2630/11/2/025002
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Decoherence in qubits due to low-frequency noise

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Cited by 139 publications
(187 citation statements)
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“…The signal decay is calculated by dividing the probability distribution to partial probabilities, p(φ, t) = p + (φ, t) + p − (φ, t), to accumulate phase φ while the TLF is in the up or down state: 33,45 χ(t) = dφp(φ, t)e iφ .…”
Section: A Single Fluctuatormentioning
confidence: 99%
“…The signal decay is calculated by dividing the probability distribution to partial probabilities, p(φ, t) = p + (φ, t) + p − (φ, t), to accumulate phase φ while the TLF is in the up or down state: 33,45 χ(t) = dφp(φ, t)e iφ .…”
Section: A Single Fluctuatormentioning
confidence: 99%
“…It is therefore of considerate importance for applications to mitigate this noise effectively. 1/f noise can be understood as arising from the collective effect of multiple sources of telegraph noise that are coupled to the quantum system of interest, with the weight of each source scaling as the inverse characteristic decay-rate of that source [16,20].…”
Section: Examplesmentioning
confidence: 99%
“…The diagonal matrix elements of noise, λ nn , are responsible for decoherence, and the offdiagonal matrix elements, λ mn (m = n), lead to the relaxation processes. In what follows, we use a spinfluctuator model of noise, modeling the noise by an ensemble of fluctuators [34][35][36]. The evolution of the average diagonal components of the density matrix is described by the following system of integro-differential equations (see Appendix B):…”
Section: Noise-assisted Electron Transfer To the Sinkmentioning
confidence: 99%