Detailed balance and phase transition in Nash equilibria of mean-field Ising game
Abstract
We study a finite-state mean-field game with entropic control cost. In the large population limit, we show that its stationary Nash equilibria satisfy the detailed balance condition and their distributions take the Gibbsian form with the value function playing the role of a Hamiltonian. We apply the entropic control cost to a ferromagnetic mean-field Ising game and investigate its stationary and non-stationary Nash equilibria. We find that the stationary Nash equilibria exhibit a second-order phase transition from disordered to ordered equilibria as temperature decreases. A center-manifold reduction yields non-stationary Nash equilibrium near the critical temperature and reveals the critical slowing down in the relaxation toward the stationary Nash equilibrium.
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BibTeX
@misc{hiura2026detailed,
title = {{Detailed balance and phase transition in Nash equilibria of mean-field Ising game}},
author = {Ken Hiura and Hajime Koike and Kiyoshi Kanazawa},
howpublished = {arXiv},
year = {2026},
month = oct,
doi = {10.48550/arxiv.2610.36518},
eprint = {2610.36518},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2610.36518},
}
RIS
TY - UNPB
TI - Detailed balance and phase transition in Nash equilibria of mean-field Ising game
AU - Ken Hiura
AU - Hajime Koike
AU - Kiyoshi Kanazawa
PY - 2026
DA - 2026/10/27
PB - arXiv
DO - 10.48550/arxiv.2610.36518
UR - https://arxiv.org/abs/2610.36518
AB - We study a finite-state mean-field game with entropic control cost. In the large population limit, we show that its stationary Nash equilibria satisfy the detailed balance condition and their distributions take the Gibbsian form with the value function playing the role of a Hamiltonian. We apply the entropic control cost to a ferromagnetic mean-field Ising game and investigate its stationary and non-stationary Nash equilibria. We find that the stationary Nash equilibria exhibit a second-order phase transition from disordered to ordered equilibria as temperature decreases. A center-manifold reduction yields non-stationary Nash equilibrium near the critical temperature and reveals the critical slowing down in the relaxation toward the stationary Nash equilibrium.
ER -