Large fluctuations of the KPZ equation in a half-space

We investigate the short-time regime of the KPZ equation in $1+1$ dimensions and develop a unifying method to obtain the height distribution in this regime, valid whenever an exact solution exists in the form of a Fredholm Pfaffian or determinant. These include the droplet and stationary initial...

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Main Author: Alexandre Krajenbrink, Pierre Le Doussal
Format: Article
Language:English
Published: SciPost 2018-10-01
Series:SciPost Physics
Online Access:https://scipost.org/SciPostPhys.5.4.032
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spelling doaj-3058ea5dd0d44a10b9dd569e2e9453d12020-11-24T21:04:00ZengSciPostSciPost Physics2542-46532018-10-015403210.21468/SciPostPhys.5.4.032Large fluctuations of the KPZ equation in a half-spaceAlexandre Krajenbrink, Pierre Le DoussalWe investigate the short-time regime of the KPZ equation in $1+1$ dimensions and develop a unifying method to obtain the height distribution in this regime, valid whenever an exact solution exists in the form of a Fredholm Pfaffian or determinant. These include the droplet and stationary initial conditions in full space, previously obtained by a different method. The novel results concern the droplet initial condition in a half space for several Neumann boundary conditions: hard wall, symmetric, and critical. In all cases, the height probability distribution takes the large deviation form $P(H,t) \sim \exp( - \Phi(H)/\sqrt{t})$ for small time. We obtain the rate function $\Phi(H)$ analytically for the above cases. It has a Gaussian form in the center with asymmetric tails, $|H|^{5/2}$ on the negative side, and $H^{3/2}$ on the positive side. The amplitude of the left tail for the half-space is found to be half the one of the full space. As in the full space case, we find that these left tails remain valid at all times. In addition, we present here (i) a new Fredholm Pfaffian formula for the solution of the hard wall boundary condition and (ii) two Fredholm determinant representations for the solutions of the hard wall and the symmetric boundary respectively.https://scipost.org/SciPostPhys.5.4.032
collection DOAJ
language English
format Article
sources DOAJ
author Alexandre Krajenbrink, Pierre Le Doussal
spellingShingle Alexandre Krajenbrink, Pierre Le Doussal
Large fluctuations of the KPZ equation in a half-space
SciPost Physics
author_facet Alexandre Krajenbrink, Pierre Le Doussal
author_sort Alexandre Krajenbrink, Pierre Le Doussal
title Large fluctuations of the KPZ equation in a half-space
title_short Large fluctuations of the KPZ equation in a half-space
title_full Large fluctuations of the KPZ equation in a half-space
title_fullStr Large fluctuations of the KPZ equation in a half-space
title_full_unstemmed Large fluctuations of the KPZ equation in a half-space
title_sort large fluctuations of the kpz equation in a half-space
publisher SciPost
series SciPost Physics
issn 2542-4653
publishDate 2018-10-01
description We investigate the short-time regime of the KPZ equation in $1+1$ dimensions and develop a unifying method to obtain the height distribution in this regime, valid whenever an exact solution exists in the form of a Fredholm Pfaffian or determinant. These include the droplet and stationary initial conditions in full space, previously obtained by a different method. The novel results concern the droplet initial condition in a half space for several Neumann boundary conditions: hard wall, symmetric, and critical. In all cases, the height probability distribution takes the large deviation form $P(H,t) \sim \exp( - \Phi(H)/\sqrt{t})$ for small time. We obtain the rate function $\Phi(H)$ analytically for the above cases. It has a Gaussian form in the center with asymmetric tails, $|H|^{5/2}$ on the negative side, and $H^{3/2}$ on the positive side. The amplitude of the left tail for the half-space is found to be half the one of the full space. As in the full space case, we find that these left tails remain valid at all times. In addition, we present here (i) a new Fredholm Pfaffian formula for the solution of the hard wall boundary condition and (ii) two Fredholm determinant representations for the solutions of the hard wall and the symmetric boundary respectively.
url https://scipost.org/SciPostPhys.5.4.032
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