Abstract
We study the time-evolution operator in a family of local quantum circuits with random fields in a fixed direction. We argue that the presence of quantum chaos implies that at large times the time-evolution operator becomes effectively a random matrix in the many-body Hilbert space. To quantify this phenomenon, we compute analytically the squared magnitude of the trace of the evolution operator-the generalized spectral form factor-and compare it with the prediction of random matrix theory. We show that for the systems under consideration, the generalized spectral form factor can be expressed in terms of dynamical correlation functions of local observables in the infinite temperature state, linking chaotic and ergodic properties of the systems. This also provides a connection between the many-body Thouless time τ_{th}-the time at which the generalized spectral form factor starts following the random matrix theory prediction-and the conservation laws of the system. Moreover, we explain different scalings of τ_{th} with the system size observed for systems with and without the conservation laws.
Highlights
The concept of chaos is very natural in classical systems
We show that for the systems under consideration, the generalized spectral form factor can be expressed in terms of dynamical correlation functions of local observables in the infinite temperature state, linking chaotic and ergodic properties of the systems
This provides a connection between the many-body Thouless time τth—the time at which the generalized spectral form factor starts following the random matrix theory prediction—and the conservation laws of the system
Summary
We study the time-evolution operator in a family of local quantum circuits with random fields in a fixed direction. In the recent comeback of quantum chaos, an important role has been played by driven systems, as they furnish a simpler modelization of many interesting dynamical phenomena [23,24,25,26,27] For these systems, in the generic instance of aperiodic driving, the spectral statistics is not well defined (their time-evolution operator is time dependent), and the chaotic regime has been identified by looking at some features of the quantum many-body dynamics—seeking a quantum many-body analog of the butterfly effect. Some of the most studied features have been the spreading of support of local operators
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