Chapman-Enskog theory and crossover between diffusion and superdiffusion for nearly integrable quantum gases

Fuente: arXiv
Saved in:
Bibliographic Details
Main Authors: Łebek, Maciej, Panfil, Miłosz
Format: Preprint
Published: 2024
Subjects:
Online Access:
Tags: Add Tag
No Tags, Be the first to tag this record!
_version_ 1866908409674072064
author Łebek, Maciej
Panfil, Miłosz
author_facet Łebek, Maciej
Panfil, Miłosz
contents Integrable systems feature an infinite number of conserved charges and on hydrodynamic scales are described by generalised hydrodynamics (GHD). This description breaks down when the integrability is weakly broken and sufficiently large space-time-scales are probed. The emergent hydrodynamics depends then on the charges conserved by the perturbation. We focus on nearly-integrable Galilean-invariant systems with conserved particle number, momentum and energy. Basing on the Boltzmann approach to integrability-breaking we describe dynamics of the system with GHD equation supplemented with a collision term. The limit of large space-time-scales is addressed using Chapman-Enskog expansion adapted to the GHD equation. For length scales larger than $\sim λ^{-2}$, where $λ$ is integrability-breaking parameter, we recover Navier-Stokes equations and find transport coefficients: viscosity and thermal conductivity. At even larger length scales, this description crosses over to Kardar-Parisi-Zhang universality class, characteristic to generic non-integrable one-dimensional fluids. Employing nonlinear fluctuating hydrodynamics we estimate this crossover length scale as $ \sim λ^{-4}$.
format Preprint
id arxiv_https___arxiv_org_abs_2410_23209
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Chapman-Enskog theory and crossover between diffusion and superdiffusion for nearly integrable quantum gases
Łebek, Maciej
Panfil, Miłosz
Statistical Mechanics
Quantum Gases
Exactly Solvable and Integrable Systems
Integrable systems feature an infinite number of conserved charges and on hydrodynamic scales are described by generalised hydrodynamics (GHD). This description breaks down when the integrability is weakly broken and sufficiently large space-time-scales are probed. The emergent hydrodynamics depends then on the charges conserved by the perturbation. We focus on nearly-integrable Galilean-invariant systems with conserved particle number, momentum and energy. Basing on the Boltzmann approach to integrability-breaking we describe dynamics of the system with GHD equation supplemented with a collision term. The limit of large space-time-scales is addressed using Chapman-Enskog expansion adapted to the GHD equation. For length scales larger than $\sim λ^{-2}$, where $λ$ is integrability-breaking parameter, we recover Navier-Stokes equations and find transport coefficients: viscosity and thermal conductivity. At even larger length scales, this description crosses over to Kardar-Parisi-Zhang universality class, characteristic to generic non-integrable one-dimensional fluids. Employing nonlinear fluctuating hydrodynamics we estimate this crossover length scale as $ \sim λ^{-4}$.
title Chapman-Enskog theory and crossover between diffusion and superdiffusion for nearly integrable quantum gases
topic Statistical Mechanics
Quantum Gases
Exactly Solvable and Integrable Systems
url https://arxiv.org/abs/2410.23209