Quantum Chaos and Thermalization in Isolated Systems of Interacting Particles

TL;DR

This review explores how quantum chaos influences thermalization in small, isolated systems of interacting particles across various physical platforms, highlighting the emergence of statistical regularities and complex stationary states.

Contribution

It provides a comprehensive analysis of the processes leading to thermalization, combining analytical and numerical methods for realistic atomic, nuclear, and spin systems.

Findings

Signatures of quantum chaos appear in stationary states at high level density.

Complex superpositions of quasiparticle excitations characterize thermalized states.

Analytical and numerical results illustrate the transition to equilibrium in mesoscopic systems.

Abstract

This review is devoted to the problem of thermalization in a small isolated conglomerate of interacting constituents. A variety of physically important systems of intensive current interest belong to this category: complex atoms, molecules (including biological molecules), nuclei, small devices of condensed matter and quantum optics on nano- and micro-scale, cold atoms in optical lattices, ion traps. Physical implementations of quantum computers, where there are many interacting qubits, also fall into this group. Statistical regularities come into play through inter-particle interactions, which have two fundamental components: mean field, that along with external conditions, forms the regular component of the dynamics, and residual interactions responsible for the complex structure of the actual stationary states. At sufficiently high level density, the stationary states become exceedingly complicated superpositions of simple quasiparticle excitations. At this stage, regularities typical of quantum chaos emerge and bring in signatures of thermalization. We describe all the stages and the results of the processes leading to thermalization, using analytical and massive numerical examples for realistic atomic, nuclear, and spin systems, as well as for models with random parameters. The structure of stationary states, strength functions of simple configurations, and concepts of entropy and temperature in application to isolated mesoscopic systems are discussed in detail. We conclude with a schematic discussion of the time evolution of such systems to equilibrium.