dc.creatorMatetski, Konstantin
dc.creatorQuastel, Jeremy
dc.creatorRemenik Zisis, Daniel Ilan
dc.date.accessioned2022-03-24T16:56:15Z
dc.date.accessioned2022-10-17T14:44:43Z
dc.date.available2022-03-24T16:56:15Z
dc.date.available2022-10-17T14:44:43Z
dc.date.created2022-03-24T16:56:15Z
dc.date.issued2021
dc.identifierActa Mathematica Volume 227 Issue 1 Page 115-203 Published 2021
dc.identifier10.4310/ACTA.2021.v227.n1.a3
dc.identifierhttps://repositorio.uchile.cl/handle/2250/184452
dc.identifier.urihttps://repositorioslatinoamericanos.uchile.cl/handle/2250/4419417
dc.description.abstractAn explicit Fredholm determinant formula is derived for the multipoint distribution of the height function of the totally asymmetric simple exclusion process (TASEP) with arbitrary right-finite initial condition. The method is by solving the biorthogonal ensemble/non-intersecting path representation found by [Sas05; BFPS07]. The resulting kernel involves transition probabilities of a random walk forced to hit a curve defined by the initial data. In the KPZ 1:2:3 scaling limit the formula leads in a transparent way to a Fredholm determinant formula, in terms of analogous kernels based on Brownian motion, for the transition probabilities of the scaling invariant Markov process at the centre of the KPZ universality class. The formula readily reproduces known special self-similar solutions such as the Airy1 and Airy2 processes. The process takes values in real valued functions which look locally like Brownian motion, and is Hölder 1/3− in time. Both the KPZ fixed point and TASEP are shown to be stochastic integrable systems in the sense that the time evolution of their transition probabilities can be linearized through a new Brownian scattering transform and its discrete analogue.
dc.languageen
dc.publisherINT Press Boston
dc.rightshttp://creativecommons.org/licenses/by-nc-nd/3.0/us/
dc.rightsAttribution-NonCommercial-NoDerivs 3.0 United States
dc.sourceActa Mathematica
dc.titleThe KPZ fixed point
dc.typeArtículos de revistas


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