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Evaporation dynamics of the Sachdev-Ye-Kitaev model

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arxiv 1909.10637 v2 pith:2WW7LRKU submitted 2019-09-23 cond-mat.str-el

classification cond-mat.str-el
keywords couplingenergysystemtemperaturemodelbathdynamicseffective
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abstract

In this paper, we study the evaporation dynamics of the Sachdev-Ye-Kitaev (SYK) model, with an initial temperature $T_\chi$, by coupling it to a thermal bath with lower temperature $T_\psi<T_\chi$ modeled by a larger SYK model. The coupling between the small system and the bath is turned on at time $t=0$. Then the system begins to envolve and finally becomes thermalized. Using the Keldysh approach, we analyze the relaxation process of the system for different temperatures and couplings. For marginal or irrelevant coupling, after a short-time energy absorption, we find a smooth thermalization of the small system where the energy relaxes before the system become thermalized. The relaxation rate of effective temperature is found to be bounded by $T$, while the energy thermalization rate increases without saturation when increasing the coupling strength. On the contrary, for the relevant coupling case, both energy and effective temperature show oscillations. We find this oscillations frequency to be coincident with the excitation energy of a Majorana operator.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Refining the Understanding of Operator Size Dynamics in Open Quantum Systems

    quant-ph 2025-04 conditional novelty 6.0 of 10

    In Brownian SYK models, operator size under the bath-traced Lindblad definition shows a scrambling signature only for intra-system interactions, with the same early-time critical point as the full-contour definition, ...

  2. Scrambling Enabled Entropy Accumulation in Open Quantum Systems

    quant-ph 2025-02 conditional novelty 6.0 of 10

    A weak probe coupled to an open quantum system accumulates a finite Rényi entropy increase only when the system is in the scrambling phase, vanishing in the dissipative phase as the probe coupling goes to zero.

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