Critical quench dynamics of random quantum spin chains: ultra-slow relaxation from initial order and delayed ordering from initial disorder

By means of free fermionic techniques combined with multiple precision arithmetic we study the time evolution of the average magnetization, $\overline{m}(t)$ , of the random transverse-field Ising chain after global quenches. We observe different relaxation behaviors for quenches starting from diffe...

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Main Authors: Gergö Roósz, Yu-Cheng Lin, Ferenc Iglói
Format: Article
Language:English
Published: IOP Publishing 2017-01-01
Series:New Journal of Physics
Subjects:
Online Access:https://doi.org/10.1088/1367-2630/aa60e6
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author Gergö Roósz
Yu-Cheng Lin
Ferenc Iglói
author_facet Gergö Roósz
Yu-Cheng Lin
Ferenc Iglói
author_sort Gergö Roósz
collection DOAJ
description By means of free fermionic techniques combined with multiple precision arithmetic we study the time evolution of the average magnetization, $\overline{m}(t)$ , of the random transverse-field Ising chain after global quenches. We observe different relaxation behaviors for quenches starting from different initial states to the critical point. Starting from a fully ordered initial state, the relaxation is logarithmically slow described by $\overline{m}(t)\sim {\mathrm{ln}}^{a}t$ , and in a finite sample of length L the average magnetization saturates at a size-dependent plateau ${\overline{m}}_{p}(L)\sim {L}^{-b};$ here the two exponents satisfy the relation $b/a=\psi =1/2$ . Starting from a fully disordered initial state, the magnetization stays at zero for a period of time until $t={t}_{{\rm{d}}}$ with $\mathrm{ln}{t}_{{\rm{d}}}\sim {L}^{\psi }$ and then starts to increase until it saturates to an asymptotic value ${\overline{m}}_{p}(L)\sim {L}^{-b^{\prime} }$ , with $b^{\prime} \approx 1.5$ . For both quenching protocols, finite-size scaling is satisfied in terms of the scaled variable $\mathrm{ln}t/{L}^{\psi }$ . Furthermore, the distribution of long-time limiting values of the magnetization shows that the typical and the average values scale differently and the average is governed by rare events. The non-equilibrium dynamical behavior of the magnetization is explained through semi-classical theory.
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spelling doaj.art-16a9b61202b74e1dba804be3ceb03dbd2023-08-08T14:38:33ZengIOP PublishingNew Journal of Physics1367-26302017-01-0119202305510.1088/1367-2630/aa60e6Critical quench dynamics of random quantum spin chains: ultra-slow relaxation from initial order and delayed ordering from initial disorderGergö Roósz0Yu-Cheng Lin1Ferenc Iglói2Wigner Research Centre, Institute for Solid State Physics and Optics , H-1525 Budapest, PO Box 49, Hungary; Institute of Theoretical Physics, Szeged University , H-6720 Szeged, HungaryGraduate Institute of Applied Physics, National Chengchi University , Taipei, TaiwanWigner Research Centre, Institute for Solid State Physics and Optics , H-1525 Budapest, PO Box 49, Hungary; Institute of Theoretical Physics, Szeged University , H-6720 Szeged, HungaryBy means of free fermionic techniques combined with multiple precision arithmetic we study the time evolution of the average magnetization, $\overline{m}(t)$ , of the random transverse-field Ising chain after global quenches. We observe different relaxation behaviors for quenches starting from different initial states to the critical point. Starting from a fully ordered initial state, the relaxation is logarithmically slow described by $\overline{m}(t)\sim {\mathrm{ln}}^{a}t$ , and in a finite sample of length L the average magnetization saturates at a size-dependent plateau ${\overline{m}}_{p}(L)\sim {L}^{-b};$ here the two exponents satisfy the relation $b/a=\psi =1/2$ . Starting from a fully disordered initial state, the magnetization stays at zero for a period of time until $t={t}_{{\rm{d}}}$ with $\mathrm{ln}{t}_{{\rm{d}}}\sim {L}^{\psi }$ and then starts to increase until it saturates to an asymptotic value ${\overline{m}}_{p}(L)\sim {L}^{-b^{\prime} }$ , with $b^{\prime} \approx 1.5$ . For both quenching protocols, finite-size scaling is satisfied in terms of the scaled variable $\mathrm{ln}t/{L}^{\psi }$ . Furthermore, the distribution of long-time limiting values of the magnetization shows that the typical and the average values scale differently and the average is governed by rare events. The non-equilibrium dynamical behavior of the magnetization is explained through semi-classical theory.https://doi.org/10.1088/1367-2630/aa60e6quantum ising chainsdisorder effectsquantum quench dynamics
spellingShingle Gergö Roósz
Yu-Cheng Lin
Ferenc Iglói
Critical quench dynamics of random quantum spin chains: ultra-slow relaxation from initial order and delayed ordering from initial disorder
New Journal of Physics
quantum ising chains
disorder effects
quantum quench dynamics
title Critical quench dynamics of random quantum spin chains: ultra-slow relaxation from initial order and delayed ordering from initial disorder
title_full Critical quench dynamics of random quantum spin chains: ultra-slow relaxation from initial order and delayed ordering from initial disorder
title_fullStr Critical quench dynamics of random quantum spin chains: ultra-slow relaxation from initial order and delayed ordering from initial disorder
title_full_unstemmed Critical quench dynamics of random quantum spin chains: ultra-slow relaxation from initial order and delayed ordering from initial disorder
title_short Critical quench dynamics of random quantum spin chains: ultra-slow relaxation from initial order and delayed ordering from initial disorder
title_sort critical quench dynamics of random quantum spin chains ultra slow relaxation from initial order and delayed ordering from initial disorder
topic quantum ising chains
disorder effects
quantum quench dynamics
url https://doi.org/10.1088/1367-2630/aa60e6
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