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.
Highlights
One of the major frontiers in condensed-matter physics is to describe gapless phases of interacting fermions without any quasiparticles, namely non-Fermi liquids (NFL) [1]
In the slow quench performed over a time τ, we find that the excitation energy generated has a remarkable intermediate-τ nonanalytic power-law dependence, τ −η with η < 1, which seemingly masks the dynamical manifestation of the initial residual entropy of the SYK fermions
The model proposed in Ref. [6] classifies the SYK NFL and a FL as two distinct chaotic fixed points separated by a quantum phase transition (QPT)
Summary
One of the major frontiers in condensed-matter physics is to describe gapless phases of interacting fermions without any quasiparticles, namely non-Fermi liquids (NFL) [1]. The Landau description of a FL is based on the concept of adiabatic time evolution from a noninteracting system under slow switching on of the interaction, without encountering a phase transition Is it possible to evolve an NFL adiabatically to the FL and vice versa? We probe the signature of this entropy in the heat generated during nonequilibrium dynamics and characterize how the putative adiabatic limit is approached in the two phases, and across the QPT, after a slow quench with a finite rate. The study of dynamics after a quench in our model, where no quasiparticle description exists in one of the phases around the QPT, allows us to probe hitherto unexplored regime of many-body quantum dynamics. Additional details of the numerical calculations, ED, and the results are given in the Supplemental Material [31]
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