Unifying Kibble–Zurek Mechanism in Weakly Driven Processes

A description of the Kibble-Zurek mechanism with linear response theory has been done previously, but ad hoc hypotheses were used, such as the rate-dependent impulse window via the Zurek equation in the context of no driving in the relaxation time. In this work, I present a new framework where such hypotheses are unnecessary while preserving all the characteristics of the phenomenon. The Kibble-Zurek scaling obtained for the excess work is close to 2/5, a result that holds for open and thermally isolated systems with relaxation time that diverges at the critical point and the first zero of the relaxation function is finite. I exemplify the results using four different but significant types of scaling functions.

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Publication Details

Journal
Entropy
Published
2026-01-06
DOI
https://doi.org/10.3390/e28010066
Primary Topic
Advanced Thermodynamics and Statistical Mechanics
Type
article
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article

Unifying Kibble–Zurek Mechanism in Weakly Driven Processes

Pierre Nazé
Entropy
Advanced Thermodynamics and Statistical Mechanics
article

Unifying Kibble–Zurek Mechanism in Weakly Driven Processes

Pierre Nazé
article en

Abstract

A description of the Kibble-Zurek mechanism with linear response theory has been done previously, but ad hoc hypotheses were used, such as the rate-dependent impulse window via the Zurek equation in the context of no driving in the relaxation time. In this work, I present a new framework where such hypotheses are unnecessary while preserving all the characteristics of the phenomenon. The Kibble-Zurek scaling obtained for the excess work is close to 2/5, a result that holds for open and thermally isolated systems with relaxation time that diverges at the critical point and the first zero of the relaxation function is finite. I exemplify the results using four different but significant types of scaling functions.

EntropyVol. 28(1)
Universidade Federal do Pará (BR)
Openalex Percentile: Top 94%
Advanced Thermodynamics and Statistical Mechanics
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