Green-Kubo formula for weakly coupled system with dynamical noise.
- Others:
- Laboratoire Jean Alexandre Dieudonné (LJAD) ; Université Nice Sophia Antipolis (1965 - 2019) (UNS) ; COMUE Université Côte d'Azur (2015-2019) (COMUE UCA)-COMUE Université Côte d'Azur (2015-2019) (COMUE UCA)-Centre National de la Recherche Scientifique (CNRS)-Université Côte d'Azur (UCA)
- CEntre de REcherches en MAthématiques de la DEcision (CEREMADE) ; Université Paris Dauphine-PSL ; Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)
- Center for Mathematical Sciences Research ; Rutgers, The State University of New Jersey [New Brunswick] (RU) ; Rutgers University System (Rutgers)-Rutgers University System (Rutgers)
- Dipartimento di Matematica [Roma II] (DIPMAT) ; Università degli Studi di Roma Tor Vergata [Roma]
- European Project: 246953,EC:FP7:ERC,ERC-2009-AdG,MALADY(2010)
Description
We consider an infinite system of cells coupled into a chain by a smooth nearest neighbor potential $\ve V$. The uncoupled system (cells) evolve according to Hamiltonian dynamics perturbed stochastically with an energy conserving noise of strenght $\noise$. We study the Green-Kubo (GK) formula $\kappa(\ve,\noise)$ for the heat conductivity of this system which exists and is finite for $\noise >0$, by formally expanding $\kappa(\ve,\noise)$ in a power series in $\ve$, $\kappa(\ve,\noise) = \sum_{n\ge 2} \ve^n \kappa_n(\noise)$. We show that $\kappa_2(\noise)$ is the same as the conductivity obtained in the weak coupling (van Hove) limit where time is rescaled as $\ve^{-2}t$. $\kappa_2(\noise)$ is conjectured to approach as $\noise \to 0$ a value proportional to that obtained for the weak coupling limit of the purely Hamiltonian chain. We also show that the $\kappa_2(\noise)$ from the GK formula, is the same as the one obtained from the flux of an open system in contact with Langevin reservoirs. Finally we show that the limit $\noise\to 0$ of $\kappa_2(\noise)$ is finite for the pinned anharmonic oscillators due to phase mixing caused by the non-resonating frequencies of the neighboring cells. This limit is bounded for coupled rotors and vanishes for harmonic chain with random pinning.
Abstract
International audience
Additional details
- URL
- https://hal.science/hal-00911148
- URN
- urn:oai:HAL:hal-00911148v1
- Origin repository
- UNICA