Critical Langevin dynamics of the O(N)-Ginzburg-Landau model with correlated noise
Julius Bonart, Leticia F. Cugliandolo, Andrea Gambassi

TL;DR
This paper investigates how correlated noise with power-law decay influences the critical dynamics of the Ginzburg-Landau model, revealing non-Markovian effects on dynamic critical exponents through renormalization group analysis.
Contribution
It introduces a perturbative renormalization group approach to analyze the impact of temporal correlations in noise on critical Langevin dynamics of the Ginzburg-Landau model, extending understanding of non-Markovian effects.
Findings
Dynamic exponents z and are affected by noise correlations for < _c(D,N).
Equilibrium critical exponents and remain unchanged by noise correlations.
Fluctuation-dissipation ratio depends on the noise correlation parameter .
Abstract
We use the perturbative renormalization group to study classical stochastic processes with memory. We focus on the generalized Langevin dynamics of the \phi^4 Ginzburg-Landau model with additive noise, the correlations of which are local in space but decay as a power-law with exponent \alpha in time. These correlations are assumed to be due to the coupling to an equilibrium thermal bath. We study both the equilibrium dynamics at the critical point and quenches towards it, deriving the corresponding scaling forms and the associated equilibrium and non-equilibrium critical exponents \eta, \nu, z and \theta. We show that, while the first two retain their equilibrium values independently of \alpha, the non-Markovian character of the dynamics affects the dynamic exponents (z and \theta) for \alpha < \alpha_c(D, N) where D is the spatial dimensionality, N the number of components of the order…
Peer Reviews
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
