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Exact short-time height distribution in 1D KPZ equation and edge fermions at high temperature

Published 10 Mar 2016 in cond-mat.stat-mech, cond-mat.dis-nn, math-ph, math.MP, and math.PR | (1603.03302v2)

Abstract: We consider the early time regime of the Kardar-Parisi-Zhang (KPZ) equation in $1+1$ dimensions in curved (or droplet) geometry. We show that for short time $t$, the probability distribution $P(H,t)$ of the height $H$ at a given point $x$ takes the scaling form $P(H,t) \sim \exp{\left(-\Phi_{\rm drop}(H)/\sqrt{t} \right)}$ where the rate function $\Phi_{\rm drop}(H)$ is computed exactly. While it is Gaussian in the center, i.e., for small $H$, the PDF has highly asymmetric non-Gaussian tails which we characterize in detail. This function $\Phi_{\rm drop}(H)$ is surprisingly reminiscent of the large deviation function describing the stationary fluctuations of finite size models belonging to the KPZ universality class. Thanks to a recently discovered connection between KPZ and free fermions, our results have interesting implications for the fluctuations of the rightmost fermion in a harmonic trap at high temperature and the full couting statistics at the edge.

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