A tale of three approaches: dynamical phase transitions for weakly bound Brownian particles

Fuente: arXiv
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Main Authors: Defaveri, Lucianno, Barkai, Eli, Kessler, David A.
Format: Preprint
Published: 2024
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author Defaveri, Lucianno
Barkai, Eli
Kessler, David A.
author_facet Defaveri, Lucianno
Barkai, Eli
Kessler, David A.
contents We investigate a system of Brownian particles weakly bound by attractive parity-symmetric potentials that grow at large distances as $V(x) \sim |x|^α$, with $0 < α< 1$. The probability density function $P(x,t)$ at long times reaches the Boltzmann-Gibbs equilibrium state, with all moments finite. However, the system's relaxation is not exponential, as is usual for a confining system with a well-defined equilibrium, but instead follows a stretched exponential $e^{- \mathrm{const} \, t^ν}$ with exponent $ν=α/(2+α)$. This problem is studied from three perspectives. First, we propose a straightforward and general scaling rate-function solution for $P(x,t)$. This rate-function, which is an important tool from large deviation theory, also displays anomalous time scaling and a dynamical phase transition. Second, through the eigenfunctions of the Fokker-Planck operator, we obtain, using the WKB method, more complete solutions that reproduce the rate function approach. Finally, we show how the alternative path-integral formalism allows us to recover the same results, with the above rate-function being the solution of the classical Hamilton-Jacobi equation describing the most probable path. Properties such as parity, the role of initial conditions, and the dynamical phase transition are thoroughly studied in all three approaches.
format Preprint
id arxiv_https___arxiv_org_abs_2407_16598
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle A tale of three approaches: dynamical phase transitions for weakly bound Brownian particles
Defaveri, Lucianno
Barkai, Eli
Kessler, David A.
Statistical Mechanics
We investigate a system of Brownian particles weakly bound by attractive parity-symmetric potentials that grow at large distances as $V(x) \sim |x|^α$, with $0 < α< 1$. The probability density function $P(x,t)$ at long times reaches the Boltzmann-Gibbs equilibrium state, with all moments finite. However, the system's relaxation is not exponential, as is usual for a confining system with a well-defined equilibrium, but instead follows a stretched exponential $e^{- \mathrm{const} \, t^ν}$ with exponent $ν=α/(2+α)$. This problem is studied from three perspectives. First, we propose a straightforward and general scaling rate-function solution for $P(x,t)$. This rate-function, which is an important tool from large deviation theory, also displays anomalous time scaling and a dynamical phase transition. Second, through the eigenfunctions of the Fokker-Planck operator, we obtain, using the WKB method, more complete solutions that reproduce the rate function approach. Finally, we show how the alternative path-integral formalism allows us to recover the same results, with the above rate-function being the solution of the classical Hamilton-Jacobi equation describing the most probable path. Properties such as parity, the role of initial conditions, and the dynamical phase transition are thoroughly studied in all three approaches.
title A tale of three approaches: dynamical phase transitions for weakly bound Brownian particles
topic Statistical Mechanics
url https://arxiv.org/abs/2407.16598