Kibble-Zurek Behavior in the Boundary-obstructed Phase Transitions

Fuente: arXiv
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Main Authors: Deng, Menghua, Sun, Zhoujian, Li, Fuxiang
Format: Preprint
Published: 2024
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author Deng, Menghua
Sun, Zhoujian
Li, Fuxiang
author_facet Deng, Menghua
Sun, Zhoujian
Li, Fuxiang
contents We study the nonadiabatic dynamics of a two-dimensional higher-order topological insulator when the system is slowly quenched across the boundary-obstructed phase transition, which is characterized by edge band gap closing. We find that the number of excitations produced after the quench exhibits power-law scaling behaviors with the quench rate. Boundary conditions can drastically modify the scaling behaviors: The scaling exponent is found to be $α=1/2$ for hybridized and fully open boundary conditions, and $α=2$ for periodic boundary condition. We argue that the exponent $α=1/2$ cannot be explained by the Kibble-Zurek mechanism unless we adopt an effective dimension $d^{\rm eff}=1$ instead of the real dimension $d=2$. For comparison, we also investigate the slow quench dynamics across the bulk-obstructed phase transitions and a single multicritical point, which obeys the Kibble-Zurek mechanism with dimension $d=2$.
format Preprint
id arxiv_https___arxiv_org_abs_2407_18256
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Kibble-Zurek Behavior in the Boundary-obstructed Phase Transitions
Deng, Menghua
Sun, Zhoujian
Li, Fuxiang
Statistical Mechanics
Mesoscale and Nanoscale Physics
Quantum Gases
Strongly Correlated Electrons
Quantum Physics
We study the nonadiabatic dynamics of a two-dimensional higher-order topological insulator when the system is slowly quenched across the boundary-obstructed phase transition, which is characterized by edge band gap closing. We find that the number of excitations produced after the quench exhibits power-law scaling behaviors with the quench rate. Boundary conditions can drastically modify the scaling behaviors: The scaling exponent is found to be $α=1/2$ for hybridized and fully open boundary conditions, and $α=2$ for periodic boundary condition. We argue that the exponent $α=1/2$ cannot be explained by the Kibble-Zurek mechanism unless we adopt an effective dimension $d^{\rm eff}=1$ instead of the real dimension $d=2$. For comparison, we also investigate the slow quench dynamics across the bulk-obstructed phase transitions and a single multicritical point, which obeys the Kibble-Zurek mechanism with dimension $d=2$.
title Kibble-Zurek Behavior in the Boundary-obstructed Phase Transitions
topic Statistical Mechanics
Mesoscale and Nanoscale Physics
Quantum Gases
Strongly Correlated Electrons
Quantum Physics
url https://arxiv.org/abs/2407.18256