TY - JOUR

T1 - Dynamical phase transition in large-deviation statistics of the Kardar-Parisi-Zhang equation

AU - Janas, Michael

AU - Kamenev, Alex

AU - Meerson, Baruch

N1 - Publisher Copyright:
© 2016 American Physical Society.
Copyright:
Copyright 2017 Elsevier B.V., All rights reserved.

PY - 2016/9/27

Y1 - 2016/9/27

N2 - We study the short-time behavior of the probability distribution P(H,t) of the surface height h(x=0,t)=H in the Kardar-Parisi-Zhang (KPZ) equation in 1+1 dimension. The process starts from a stationary interface: h(x,t=0) is given by a realization of two-sided Brownian motion constrained by h(0,0)=0. We find a singularity of the large deviation function of H at a critical value H=Hc. The singularity has the character of a second-order phase transition. It reflects spontaneous breaking of the reflection symmetry x↔-x of optimal paths h(x,t) predicted by the weak-noise theory of the KPZ equation. At |H| |Hc| the corresponding tail of P(H) scales as -lnP∼|H|3/2/t1/2 and agrees, at any t>0, with the proper tail of the Baik-Rains distribution, previously observed only at long times. The other tail of P scales as -lnP∼|H|5/2/t1/2 and coincides with the corresponding tail for the sharp-wedge initial condition.

AB - We study the short-time behavior of the probability distribution P(H,t) of the surface height h(x=0,t)=H in the Kardar-Parisi-Zhang (KPZ) equation in 1+1 dimension. The process starts from a stationary interface: h(x,t=0) is given by a realization of two-sided Brownian motion constrained by h(0,0)=0. We find a singularity of the large deviation function of H at a critical value H=Hc. The singularity has the character of a second-order phase transition. It reflects spontaneous breaking of the reflection symmetry x↔-x of optimal paths h(x,t) predicted by the weak-noise theory of the KPZ equation. At |H| |Hc| the corresponding tail of P(H) scales as -lnP∼|H|3/2/t1/2 and agrees, at any t>0, with the proper tail of the Baik-Rains distribution, previously observed only at long times. The other tail of P scales as -lnP∼|H|5/2/t1/2 and coincides with the corresponding tail for the sharp-wedge initial condition.

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U2 - 10.1103/PhysRevE.94.032133

DO - 10.1103/PhysRevE.94.032133

M3 - Article

C2 - 27739741

AN - SCOPUS:84990194603

VL - 94

JO - Physical Review E - Statistical, Nonlinear, and Soft Matter Physics

JF - Physical Review E - Statistical, Nonlinear, and Soft Matter Physics

SN - 1539-3755

IS - 3

M1 - 032133

ER -