2015
DOI: 10.1103/physrevlett.114.060601
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Hyperuniformity and Phase Separation in Biased Ensembles of Trajectories for Diffusive Systems

Abstract: We analyze biased ensembles of trajectories for diffusive systems. In trajectories biased either by the total activity or the total current, we use fluctuating hydrodynamics to show that these systems exhibit phase transitions into "hyperuniform" states, where large-wavelength density fluctuations are strongly suppressed. We illustrate this behavior numerically for a system of hard particles in one dimension and we discuss how it appears in simple exclusion processes. We argue that these diffusive systems gene… Show more

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Cited by 127 publications
(233 citation statements)
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References 49 publications
(132 reference statements)
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“…An important observation is that the bounds on fluctuations of a counting observable and its FPTs are controlled by the average dynamical activity, in analogy to the role played by the entropy production in the case of currents [1,13]. We hope these results will add to the growing body of work applying large deviation ideas and methods to the study of dynamics in driven systems [29][30][31][32][33][34][35][36][37][38][39][40][41], glasses [25,[42][43][44][45][46][47], protein folding and signaling networks [48][49][50][51], open quantum systems [52][53][54][55][56][57][58][59][60][61][62][63][64], and many other problems in nonequilibrium [65][66][67][68][69][70][71][72].…”
Section: Introductionmentioning
confidence: 90%
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“…An important observation is that the bounds on fluctuations of a counting observable and its FPTs are controlled by the average dynamical activity, in analogy to the role played by the entropy production in the case of currents [1,13]. We hope these results will add to the growing body of work applying large deviation ideas and methods to the study of dynamics in driven systems [29][30][31][32][33][34][35][36][37][38][39][40][41], glasses [25,[42][43][44][45][46][47], protein folding and signaling networks [48][49][50][51], open quantum systems [52][53][54][55][56][57][58][59][60][61][62][63][64], and many other problems in nonequilibrium [65][66][67][68][69][70][71][72].…”
Section: Introductionmentioning
confidence: 90%
“…(And even for driven systems it is revealing to study the dynamical phase behavior in terms of both empirical currents and activities; see e.g. [33,36,40,45]. )…”
Section: Discussionmentioning
confidence: 99%
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“…(40), the mapping between the conditioned and driven process is trivial. The driven process is obtained simply by normalising the cMPS, which amounts to shifting the escape rate R by the scaled cumulant generating function θ(s) = γ (e −s − 1), cf.…”
Section: A Examplementioning
confidence: 99%
“…On the other hand, (23) means that trajectory PTX has J τ (PTX) = J and (18) implies that dP (PTX) = dP (X). Hence, using (26), one has…”
Section: Ensembles and Pt-symmetrymentioning
confidence: 99%