2019
DOI: 10.1103/physreve.99.052139
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Quantum chaotic fluctuation-dissipation theorem: Effective Brownian motion in closed quantum systems

Abstract: We analytically describe the decay to equilibrium of generic observables of a non-integrable system after a perturbation in the form of a random matrix. We further obtain an analytic form for the time-averaged fluctuations of an observable in terms of the rate of decay to equilibrium. Our result shows the emergence of a Fluctuation-Dissipation theorem corresponding to a classical Brownian process, specifically, the Ornstein-Uhlenbeck process. Our predictions can be tested in quantum simulation experiments, thu… Show more

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Cited by 32 publications
(83 citation statements)
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“…Results similar to Eq. (8) have been obtained even in the nonperturbative regime in the context of thermalization [31,32], giving evidence of the broad validity of the predicted behavior for δ(A, t).…”
Section: A Evolution Under Weak Random Perturbationsmentioning
confidence: 72%
“…Results similar to Eq. (8) have been obtained even in the nonperturbative regime in the context of thermalization [31,32], giving evidence of the broad validity of the predicted behavior for δ(A, t).…”
Section: A Evolution Under Weak Random Perturbationsmentioning
confidence: 72%
“…Our results may be of particular importance in setups allowing environmental monitoring and feedback control [50,51,[62][63][64][65][66][67], and for quantum thermal devices working in nonequilibrium steady-state conditions [68][69][70][71][72][73][74][75]. It would be also interesting to explore connections with path-integral approaches [76], one-shot quantum thermodynamics [77][78][79][80], and quantum information [81][82][83][84][85]. Finally, we remark that some of our results could be applied to classical systems where knowledge of system's state is incomplete e.g.…”
mentioning
confidence: 71%
“…Continuing, we assume that the initial state for the quantum quench is an eigenstate of H 0 , |ψ (0) = |φ α 0 , with eigenenergy E α 0 , though the formalism is easily extended to more general cases [32]. We focus local observables that are diagonal in the free basis, O αβ ∝ δ αβ .…”
Section: Chaotic Wave Functions and Random Matrix Theorymentioning
confidence: 99%
“…The study of quantum nonequilibrium dynamics has only recently become experimentally feasible [8][9][10][11][12][13], raising questions surrounding the process and conditions in which isolated many-body quantum systems equilibrate to a thermal state [14][15][16][17][18][19][20][21][22], a process known as quantum thermalization [23][24][25][26][27]. Important related questions remain surrounding relaxation timescales and the route to equilibrium of complex quantum systems [28][29][30][31][32][33][34][35][36], as well as the emergence of thermodynamical laws [37][38][39][40]. A useful approach to the description of generic nonintegrable quantum systems can be developed from quantum chaos [41,42] and the eigenstate thermalization hypothesis (ETH), which in turn can be derived from an underlying random matrix theory (RMT) [32,33,[43][44][45][46].…”
Section: Introductionmentioning
confidence: 99%
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