We study the solution of the Kardar-Parisi-Zhang (KPZ) equation for the stochastic growth of an interface of height (, ) on the positive half line, equivalently the free energy of the continuum directed polymer in a half space with a wall at . The boundary condition corresponds to an attractive wall for , and leads to the binding of the polymer to the wall below the critical value . Here we choose the initial condition (, 0) to be a Brownian motion in with drift . When , the solution is stationary, i.e. remains at all times a Brownian motion with the same drift, up to a global height shift (0, ). We show that the distribution of this height shift is invariant under the exchange of parameters and . For any , we provide an exact formula characterizing the distribution of (0, ) at any time , using two methods: the replica Bethe ansatz and a discretization called the log-gamma polymer, for which moment formulae were obtained. We analyze its large time asymptotics for various ranges of parameters , . In particular, when , the critical stationary case, the fluctuations of the interface are governed by a universal distribution akin to the Baik-Rains distribution arising in stationary growth on the full-line. It can be expressed in terms of a simple Fredholm determinant, or equivalently in terms of the Painlevé II transcendent. This provides an analog for the KPZ equation, of some of the results recently obtained by Betea-Ferrari-Occelli in the context of stationary half-space last-passage-percolation. From universality, we expect that limiting distributions found in both models can be shown to coincide.
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http://dx.doi.org/10.1007/s10955-020-02622-z | DOI Listing |
Phys Rev E
November 2024
Université Grenoble Alpes, CNRS, LPMMC, 38000 Grenoble, France.
A new scaling regime characterized by a z=1 dynamical critical exponent has been reported in several numerical simulations of the one-dimensional Kardar-Parisi-Zhang and noisy Burgers equations. In these works, this scaling, differing from the well-known KPZ one z=3/2, was found to emerge in the tensionless limit for the interface and in the inviscid limit for the fluid. Based on functional renormalization group, the origin of this scaling has been elucidated.
View Article and Find Full Text PDFPhys Rev E
June 2024
Université Grenoble Alpes, CNRS, LPMMC, 38000 Grenoble, France.
We consider the one-dimensional deterministic complex Ginzburg-Landau equation in the regime of phase turbulence, where the order parameter displays a defect-free chaotic phase dynamics, which maps to the Kuramoto-Sivashinsky equation, characterized by negative viscosity and a modulational instability at linear level. In this regime, the dynamical behavior of the large wavelength modes is captured by the Kardar-Parisi-Zhang (KPZ) universality class, determining their universal scaling and their statistical properties. These modes exhibit the characteristic KPZ superdiffusive scaling with the dynamical critical exponent z=3/2.
View Article and Find Full Text PDFPhys Rev E
June 2024
Theory Division, Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700064, West Bengal, India.
We elucidate the universal spatiotemporal scaling properties of the time-dependent correlation functions in a class of two-component one-dimensional (1D) driven diffusive system that consists of two coupled asymmetric exclusion processes. By using a perturbative renormalization group framework, we show that the relevant scaling exponents have values same as those for the 1D Kardar-Parisi-Zhang (KPZ) equation. We connect these universal scaling exponents with the symmetries of the model equations.
View Article and Find Full Text PDFPhys Rev Lett
May 2024
Center for Nonlinear Phenomena and Complex Systems, Université Libre de Bruxelles, CP 231, Campus Plaine, B-1050 Brussels, Belgium.
We show that lasing in flat-band lattices can be stabilized by means of the geometrical properties of the Bloch states, in settings where the single-particle dispersion is flat in both its real and imaginary parts. We illustrate a general projection method and compute the collective excitations, which display a diffusive behavior ruled by quantum geometry through a peculiar coefficient involving gain, losses and interactions, and entailing resilience against modulational instabilities. Then, we derive an equation of motion for the phase dynamics and identify a Kardar-Parisi-Zhang term of geometric origin.
View Article and Find Full Text PDFPhys Rev E
April 2024
Institut de Radioprotection et de Sûreté Nucléaire (IRSN) PSN-RES/SNC/LN, F-92260, Fontenay-aux-Roses, France.
An operating nuclear reactor is designed to maintain a sustained fission chain reaction in its core, which results from a delicate balance between neutron creations (i.e., fissions) and total absorptions.
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