Operator spreading and the emergence of dissipative hydrodynamics under unitary evolution with conservation laws

TL;DR

This paper investigates how conserved quantities like charge or energy influence operator spreading and dissipation in chaotic quantum systems, revealing a diffusive-to-ballistic transition and a hydrodynamic framework.

Contribution

It introduces a random circuit model with conservation laws to explain the emergence of dissipative hydrodynamics from unitary evolution, highlighting the role of conserved operators in operator spreading.

Findings

Conserved parts of operators spread diffusively, emitting nonconserved parts that spread ballistically.

Dissipation occurs via conversion of conserved to nonconserved operators at a rate set by diffusion.

OTOCs develop a diffusive tail and approach their late-time value as a power law.

Abstract

We study the scrambling of local quantum information in chaotic many-body systems in the presence of a locally conserved quantity like charge or energy that moves diffusively. The interplay between conservation laws and scrambling sheds light on the mechanism by which unitary quantum dynamics, which is reversible, gives rise to diffusive hydrodynamics, which is a dissipative process. We obtain our results in a random quantum circuit model that is constrained to have a conservation law. We find that a generic spreading operator consists of two parts: (i) a conserved part which comprises the weight of the spreading operator on the local conserved densities, whose dynamics is described by diffusive charge spreading. This conserved part also acts as a source that steadily emits a flux of (ii) non-conserved operators. This emission leads to dissipation in the operator hydrodynamics, with the dissipative process being the conversion of operator weight from local conserved operators to nonconserved, at a rate set by the local diffusion current. The emitted nonconserved parts then spread ballistically at a butterfly speed, thus becoming highly nonlocal and hence essentially non-observable, thereby acting as the "reservoir" that facilitates the dissipation. In addition, we find that the nonconserved component develops a power law tail behind its leading ballistic front due to the slow dynamics of the conserved components. This implies that the out-of-time-order commutator (OTOC) between two initially separated operators grows sharply upon the arrival of the ballistic front but, in contrast to systems with no conservation laws, it develops a diffusive tail and approaches its asymptotic late-time value only as a power of time instead of exponentially. We also derive these results within an effective hydrodynamic description which contains multiple coupled diffusion equations.