2015
DOI: 10.1103/physreva.92.042110
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Dynamics of noisy quantum systems in the Heisenberg picture: Application to the stability of fractional charge

Abstract: Based on the Heisenberg-picture analog of the master equation, we develop a method for computing the exact time dependence of noise-averaged observables for general noninteracting fermionic systems with noisy fluctuations. Upon noise averaging, these fluctuations generate effective interactions, limiting analytical approaches. While the short-time dynamics can be studied with Langevin-type numerical simulations, the long-time limit is not amenable to such simulations. Our results provide access to this long-ti… Show more

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Cited by 9 publications
(7 citation statements)
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“…This is due to the linearity of the dynamical equation (8). A decoherence operator F β can represent either noise in the Hamiltonian parameters (in which case, F β is Hermitian [38,39]) or an engineered bath [40]. In the former case, f β 's are constant rates of noise processes and in the latter, f β (t)'s are control knobs that the Pontryagin's minimum principle says should vary in bang-bang form for an optimal protocol.…”
Section: B Presence Of Decoherencementioning
confidence: 99%
“…This is due to the linearity of the dynamical equation (8). A decoherence operator F β can represent either noise in the Hamiltonian parameters (in which case, F β is Hermitian [38,39]) or an engineered bath [40]. In the former case, f β 's are constant rates of noise processes and in the latter, f β (t)'s are control knobs that the Pontryagin's minimum principle says should vary in bang-bang form for an optimal protocol.…”
Section: B Presence Of Decoherencementioning
confidence: 99%
“…Note that white noise is a good approximation to ubiquitous colored noise with exponentially decaying correlations. We set W as a small value for the stochastic perturbation, which ensures the validity of noise-average density matrix technique 49 . We consider the system Hamiltonian containing two parts in a general form 48…”
Section: Anti-kz Behavior Of a Noisy Transverse-field Xy Chainmentioning
confidence: 99%
“…where |1 ≡ c † |0 , yielding the initial density matrix ρ 0 = 1 2 (|0 0| + |0 1| + |1 0| + |1 1|), which is then evolved and averaged over noise to obtain ρ(τ), by solving the master equation 38,43,44 ,…”
Section: Random White Noisementioning
confidence: 99%