# The gradient condition and the contribution of the dynamical part of   Green-Kubo formula to the diffusion coefficient

**Authors:** Makiko Sasada

arXiv: 1704.03745 · 2017-05-01

## TL;DR

This paper investigates whether the vanishing of the dynamical part of the Green-Kubo formula implies the gradient condition in symmetric interacting particle systems, providing conditions under which the converse holds.

## Contribution

It establishes that if the equilibrium measure is a product measure with a separable L^2 space, then zero dynamical contribution implies the gradient condition.

## Key findings

- The dynamical part of Green-Kubo formula can be zero without the gradient condition, under certain measure conditions.
- The converse holds if the equilibrium measure is product and L^2 space is separable.
- Application to energy transport models demonstrates the theoretical results.

## Abstract

In the diffusive hydrodynamic limit for a symmetric interacting particle system (such as the exclusion process, the zero range process, the stochastic Ginzburg-Landau model, the energy exchange model), a possibly non-linear diffusion equation is derived as the hydrodynamic equation. The bulk diffusion coefficient of the limiting equation is given by Green-Kubo formula and it can be characterized by a variational formula. In the case the system satisfies the gradient condition, the variational problem is explicitly solved and the diffusion coefficient is given from the Green-Kubo formula through a static average only. In other words, the contribution of the dynamical part of Green-Kubo formula is 0. In this paper, we consider the converse, namely if the contribution of the dynamical part of Green-Kubo formula is 0, does it imply the system satisfies the gradient condition or not. We show that if the equilibrium measure {\mu} is product and {L^2} space of its single site marginal is separable, then the converse also holds. As an application of the result, we consider a class of stochastic models for energy transport studied by Gaspard and Gilbert in [1, 2], where the exact problem is discussed for this specific model.

## Full text

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## References

8 references — full list in the complete paper: https://tomesphere.com/paper/1704.03745/full.md

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Source: https://tomesphere.com/paper/1704.03745