Quantum to classical crossover in many-body chaos and scrambling from relaxation in a glass
arXiv:2105.13376 · doi:10.1103/PhysRevLett.128.115302
Abstract
Chaotic quantum systems with Lyapunov exponent obey an upper bound at temperature , implying a divergence of the bound in the classical limit . Following this trend, does a quantum system necessarily become `more chaotic' when quantum fluctuations are reduced? Moreover, how do symmetry breaking and associated non-trivial dynamics influence the interplay of quantum mechanics and chaos? We explore these questions by computing in the quantum spherical -spin glass model, where can be continuously varied. We find that quantum fluctuations, in general, make paramagnetic phase less and the replica symmetry-broken spin glass phase more chaotic. We show that the approach to the classical limit could be non-trivial, with non-monotonic dependence of on close to the dynamical glass transition temperature . Our results in the classical limit () naturally describe chaos in super-cooled liquid in structural glasses. We find a maximum in substantially above , concomitant with the crossover from simple to slow glassy relaxation. We further show that , with the exponent varying between 2 and 1 from quantum to classical limit, at low temperatures in the spin glass phase.
arXiv comment6 pages, 4 figures
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