2017
DOI: 10.1103/physrevb.96.205123
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Quantum quench of the Sachdev-Ye-Kitaev model

Abstract: We describe the non-equilibrium quench dynamics of the Sachdev-Ye-Kitaev models of fermions with random all-to-all interactions. These provide tractable models of the dynamics of quantum systems without quasiparticle excitations. The Kadanoff-Baym equations show that the final state is thermal, and their numerical analysis is consistent with a thermalization rate proportional to the absolute temperature of the final state. We also obtain an exact analytic solution of the quench dynamics in the large q limit of… Show more

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Cited by 122 publications
(160 citation statements)
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“…Interacting Sachdev-Ye-Kitaev models (SYK 4 ), for example, contain correlated pair hopping terms of random strengths. The relaxation dynamics and level spacing statistics of SYK 4 models have been studied recently [92,[148][149][150]. However, these models have no spatial structure, so there are no transport/spreading effects.…”
Section: Discussion and Contextmentioning
confidence: 99%
“…Interacting Sachdev-Ye-Kitaev models (SYK 4 ), for example, contain correlated pair hopping terms of random strengths. The relaxation dynamics and level spacing statistics of SYK 4 models have been studied recently [92,[148][149][150]. However, these models have no spatial structure, so there are no transport/spreading effects.…”
Section: Discussion and Contextmentioning
confidence: 99%
“…For our purposes we chose a typical grid-size of the t 1 − t 2 plane of 8000 × 8000 and set δ = 10 −8 . The initial conditions are found by iterating the SDE in frequency space [32,37].…”
Section: Supplemental Materialmentioning
confidence: 99%
“…Grey lines denote the free Green's function, G 0 ; black lines the disorder averaged full Green's function, G(t, t ) = −i T C {c i (t)c † j (t )} (where T C denotes contour time ordering); and dotted lines represent disorder averages of K ij and J ij;kl , respectively. The precise form of our KBE's is read off from the diagrams to be(2) As initial conditions we fix the Green's function in the lower quadrant of the two-time plane (t, t ) with low temperature initial states, that are determined by numerically iterating the equilibrium Schwinger-Dyson equations [32,36,37].We then switch on the drive at time t = 0 and follow the evolution of the system. The resulting equations are integrated numerically employing a predictor-corrector scheme; see supplementary material for details [38].…”
mentioning
confidence: 99%
“…A recent study addressed these matters directly in a zero-density 1 þ 1D CFT relating the Vaidya shell to structure realized in the large central charge limit [22,23], suggesting that the instantaneous thermalization might be a large N artifact. Another recent study addressed thermalization of fermionic Green's functions after a quench in the Sachdev-Ye-Kitaev model [24], which is believed to be a quantum system with a holographic dual. For q-fermion interactions with q → ∞, instantaneous thermalization was also found, consistent with an AdS 2 -Vaidya dual.…”
Section: Introductionmentioning
confidence: 99%