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Quench, thermalization and residual entropy across a non-Fermi liquid to Fermi liquid transition

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arxiv 1903.09652 v3 pith:YDPWKHQF submitted 2019-03-22 cond-mat.str-el hep-th

classification cond-mat.str-elhep-th
keywords fermionsliquidquenchentropyresidualthermalizationtransitionacross
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abstract

We study the thermalization, after sudden and slow quenches, of an interacting model having a quantum phase transition from a Sachdev-Ye-Kitaev (SYK) non-Fermi liquid (NFL) to a Fermi liquid (FL). The model has SYK fermions coupled to non-interacting lead fermions and can be realized in a graphene flake connected to external leads. After a sudden quench to the NFL, a thermal state is reached rapidly via collapse-revival oscillations of the quasiparticle residue of the lead fermions. In contrast, the quench to the FL, across the NFL-FL transition, leads to multiple prethermal regimes and much slower thermalization. In the slow quench performed over a time $\tau$, we find that the excitation energy generated has a remarkable intermediate-$\tau$ non-analytic power-law dependence, $\tau^{-\eta}$ with $\eta<1$, which seemingly masks the dynamical manifestation of the initial residual entropy of the SYK fermions. The power-law scaling is expected to eventually break down for $\tau\to\infty$, signaling a violation of adiabaticity, due to the residual entropy present in the SYK fermions.

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  1. Hot wormholes and chaos dynamics in a two-coupled SYK model

    hep-th 2025-01 conditional novelty 6.0 of 10

    First numerical Lyapunov exponents for the unstable hot wormhole phase of the two-coupled SYK model, obtained via cooling and periodic-driving protocols.

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