Survival probability in Generalized Rosenzweig-Porter random matrix ensemble

We study analytically and numerically the dynamics of the generalized Rosenzweig-Porter model, which is known to possess three distinct phases: ergodic, multifractal and localized phases. Our focus is on the survival probability $R(t)$, the probability of finding the initial state after time $t$...

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Main Author: Giuseppe De Tomasi, Mohsen Amini, Soumya Bera, Ivan M. Khaymovich, Vladimir E. Kravtsov
Format: Article
Language:English
Published: SciPost 2019-01-01
Series:SciPost Physics
Online Access:https://scipost.org/SciPostPhys.6.1.014
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spelling doaj-d66e5a3994be4c01abf39c8ddad73e682020-11-25T01:25:44ZengSciPostSciPost Physics2542-46532019-01-016101410.21468/SciPostPhys.6.1.014Survival probability in Generalized Rosenzweig-Porter random matrix ensembleGiuseppe De Tomasi, Mohsen Amini, Soumya Bera, Ivan M. Khaymovich, Vladimir E. KravtsovWe study analytically and numerically the dynamics of the generalized Rosenzweig-Porter model, which is known to possess three distinct phases: ergodic, multifractal and localized phases. Our focus is on the survival probability $R(t)$, the probability of finding the initial state after time $t$. In particular, if the system is initially prepared in a highly-excited non-stationary state (wave packet) confined in space and containing a fixed fraction of all eigenstates, we show that $R(t)$ can be used as a dynamical indicator to distinguish these three phases. Three main aspects are identified in different phases. The ergodic phase is characterized by the standard power-law decay of $R(t)$ with periodic oscillations in time, surviving in the thermodynamic limit, with frequency equals to the energy bandwidth of the wave packet. In multifractal extended phase the survival probability shows an exponential decay but the decay rate vanishes in the thermodynamic limit in a non-trivial manner determined by the fractal dimension of wave functions. Localized phase is characterized by the saturation value of $R(t\to\infty)=k$, finite in the thermodynamic limit $N\rightarrow\infty$, which approaches $k=R(t\to 0)$ in this limit.https://scipost.org/SciPostPhys.6.1.014
collection DOAJ
language English
format Article
sources DOAJ
author Giuseppe De Tomasi, Mohsen Amini, Soumya Bera, Ivan M. Khaymovich, Vladimir E. Kravtsov
spellingShingle Giuseppe De Tomasi, Mohsen Amini, Soumya Bera, Ivan M. Khaymovich, Vladimir E. Kravtsov
Survival probability in Generalized Rosenzweig-Porter random matrix ensemble
SciPost Physics
author_facet Giuseppe De Tomasi, Mohsen Amini, Soumya Bera, Ivan M. Khaymovich, Vladimir E. Kravtsov
author_sort Giuseppe De Tomasi, Mohsen Amini, Soumya Bera, Ivan M. Khaymovich, Vladimir E. Kravtsov
title Survival probability in Generalized Rosenzweig-Porter random matrix ensemble
title_short Survival probability in Generalized Rosenzweig-Porter random matrix ensemble
title_full Survival probability in Generalized Rosenzweig-Porter random matrix ensemble
title_fullStr Survival probability in Generalized Rosenzweig-Porter random matrix ensemble
title_full_unstemmed Survival probability in Generalized Rosenzweig-Porter random matrix ensemble
title_sort survival probability in generalized rosenzweig-porter random matrix ensemble
publisher SciPost
series SciPost Physics
issn 2542-4653
publishDate 2019-01-01
description We study analytically and numerically the dynamics of the generalized Rosenzweig-Porter model, which is known to possess three distinct phases: ergodic, multifractal and localized phases. Our focus is on the survival probability $R(t)$, the probability of finding the initial state after time $t$. In particular, if the system is initially prepared in a highly-excited non-stationary state (wave packet) confined in space and containing a fixed fraction of all eigenstates, we show that $R(t)$ can be used as a dynamical indicator to distinguish these three phases. Three main aspects are identified in different phases. The ergodic phase is characterized by the standard power-law decay of $R(t)$ with periodic oscillations in time, surviving in the thermodynamic limit, with frequency equals to the energy bandwidth of the wave packet. In multifractal extended phase the survival probability shows an exponential decay but the decay rate vanishes in the thermodynamic limit in a non-trivial manner determined by the fractal dimension of wave functions. Localized phase is characterized by the saturation value of $R(t\to\infty)=k$, finite in the thermodynamic limit $N\rightarrow\infty$, which approaches $k=R(t\to 0)$ in this limit.
url https://scipost.org/SciPostPhys.6.1.014
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