Hyperbolic $O (N)$ linear sigma model and its mean-field limit
Ruoyuan Liu, Shao Liu, Tadahiro Oh
TL;DR
This work analyzes the large-$N$ behavior of the hyperbolic $O(N)$ linear sigma model on the 2D torus, establishing pathwise global well-posedness for the coupled SdNLW system and proving convergence to a mean-field SdNLW with a nonlocal nonlinear term. The authors develop a renormalized framework via Wick powers, construct enhanced data sets, and implement a hybrid $I$-method to obtain uniform-in-$N$ global control and convergence results, including a law-of-large-numbers mechanism that replaces empirical averages by expectations. They also extend the analysis to invariant Gibbs dynamics, proving convergence to the mean-field Gibbs dynamics and demonstrating propagation of chaos, with a convergence rate of $N^{-1/2+\varepsilon}$ on large time intervals and under higher moment assumptions a rate $N^{-1/2+\varepsilon_0}$. The results contribute a rigorous dynamical understanding of large-$N$ limits for hyperbolic stochastic quantization models and their Gibbsian equilibria, connecting stochastic damped wave dynamics with mean-field and propagation-of-chaos phenomena in a dispersive setting.
Abstract
We study large $N$ limits of the hyperbolic $O(N)$ linear sigma model ($\text{HLSM}_N$) on the two-dimensional torus $\mathbb T^2$, namely, a system of $N$ interacting stochastic damped nonlinear wave equations (SdNLW) with coupled cubic nonlinearities. After establishing (pathwise) global well-posedness of $\text{HLSM}_N$ and the limiting equation, called the mean-field SdNLW, we first establish convergence of $\text{HLSM}_N$ to the mean-field SdNLW with general initial data (under a suitable assumption). In particular, for the local-in-time convergence, we obtain a convergence rate of order $N^{- \frac 12 + \varepsilon}$ for any $ \varepsilon > 0$. We then show that the invariant Gibbs dynamics for $\text{HLSM}_N$) converges to that for the mean-field SdNLW with a convergence rate of order $N^{- \frac 12 + \varepsilon}$ on any large time intervals.
