2021
DOI: 10.1103/physreve.103.032109
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Characterizing the Lipkin-Meshkov-Glick model excited-state quantum phase transition using dynamical and statistical properties of the diagonal entropy

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Cited by 18 publications
(12 citation statements)
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“…They are somehow linked to thermal phase transitions [21,22] and dynamical phase transitions [23,24]. They can be identified by their consequences in the classical [25] and semiclassical [26,27] phase-space dynamics [28,29], as in the singularities of the density of states [30]. Its signatures have been theoretically and experimentally observed in several physical systems [31][32][33][34][35][36], and its connections with quantum Lyapunov exponents have been explored [37][38][39].…”
mentioning
confidence: 99%
“…They are somehow linked to thermal phase transitions [21,22] and dynamical phase transitions [23,24]. They can be identified by their consequences in the classical [25] and semiclassical [26,27] phase-space dynamics [28,29], as in the singularities of the density of states [30]. Its signatures have been theoretically and experimentally observed in several physical systems [31][32][33][34][35][36], and its connections with quantum Lyapunov exponents have been explored [37][38][39].…”
mentioning
confidence: 99%
“…pinpointing and studying ESQPTs and the symmetry-breaking effects [38]. The qualitative features exhibited when the system is initialized in the ground state were shown to largely extend to initially excited states, with some notable changes, in particular, the emergence of a bimodal distribution for the work that is nevertheless sensitive to quenches to the ESQPT.…”
Section: Discussionmentioning
confidence: 97%
“…Such impact is also visible as a cusp in the work distribution, leading to complex survival probability dynamics [12]. Remarkably, the ESQPT yields critical signatures in other quantities, such as in out-of-time correlators [35], decoherence rates [17,18], or in phase-space quasiprobability distributions [36], and such signatures hold under different protocols, either under infinitesimal [37] or time-dependent quenches [38]. Yet, although second-order QPTs and ESQPTs are intimately related to spontaneous symmetry breaking, the impact of such fundamental process in these dynamical quantities has so far been overlooked, with the notable exceptions in the realm of dynamical quantum phase transitions [39], where symmetry breaking upon a sudden quench is key for the emerging nonanalytical behavior [19,[40][41][42][43][44][45][46].…”
Section: Introductionmentioning
confidence: 99%
“…To quantify the distance between P(x) and P 2 (x), we use two different deviation measures, namely the square root of the Kullback-Leibler divergence (SKLD) [123,124] and the root-mean-square error (RMSE) [125,126]. For the observed distribution P(x) and predicted distribution P ν (x), the SKLD (RMSE), denoted as D…”
Section: Multifractality Of Coherent Statesmentioning
confidence: 99%