2023
DOI: 10.1002/cpa.22110
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Fluctuation exponents of the KPZ equation on a large torus

Abstract: We study the one‐dimensional KPZ equation on a large torus, started at equilibrium. The main results are optimal variance bounds in the super‐relaxation regime and part of the relaxation regime.

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Cited by 2 publications
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“…then implies 〈e sh(x,t) 〉 ≍ e t F (s) with F (s) = lim λ→∞ λ −1 F λ (s) the generating function of the stationary cumulants c st k = F (k) (0). At the KPZ fixed point with periodic boundary condition, the variance c st 2 = π/2 was first obtained in [348] for TASEP, see also [349] for a rigorous approach from the stochastic heat equation ( 4). An explicit parametric expression was eventually obtained for F (s) [186,226,[350][351][352][353][354] from various exactly solvable microscopic models.…”
Section: Stationary Large Deviationsmentioning
confidence: 99%
“…then implies 〈e sh(x,t) 〉 ≍ e t F (s) with F (s) = lim λ→∞ λ −1 F λ (s) the generating function of the stationary cumulants c st k = F (k) (0). At the KPZ fixed point with periodic boundary condition, the variance c st 2 = π/2 was first obtained in [348] for TASEP, see also [349] for a rigorous approach from the stochastic heat equation ( 4). An explicit parametric expression was eventually obtained for F (s) [186,226,[350][351][352][353][354] from various exactly solvable microscopic models.…”
Section: Stationary Large Deviationsmentioning
confidence: 99%