English

A near-optimal zero-free disk for the Ising model

Combinatorics 2024-04-24 v2 Discrete Mathematics Data Structures and Algorithms Mathematical Physics math.MP

Abstract

The partition function of the Ising model of a graph G=(V,E)G=(V,E) is defined as ZIsing(G;b)=σ:V{0,1}bm(σ)Z_{\text{Ising}}(G;b)=\sum_{\sigma:V\to \{0,1\}} b^{m(\sigma)}, where m(σ)m(\sigma) denotes the number of edges e={u,v}e=\{u,v\} such that σ(u)=σ(v)\sigma(u)=\sigma(v). We show that for any positive integer Δ\Delta and any graph GG of maximum degree at most Δ\Delta, ZIsing(G;b)0Z_{\text{Ising}}(G;b)\neq 0 for all bCb\in \mathbb{C} satisfying b1b+11oΔ(1)Δ1|\frac{b-1}{b+1}| \leq \frac{1-o_\Delta(1)}{\Delta-1} (where oΔ(1)0o_\Delta(1) \to 0 as Δ\Delta\to \infty). This is optimal in the sense that 1oΔ(1)Δ1\tfrac{1-o_\Delta(1)}{\Delta-1} cannot be replaced by cΔ1\tfrac{c}{\Delta-1} for any constant c>1c > 1 subject to a complexity theoretic assumption. To prove our result we use a standard reformulation of the partition function of the Ising model as the generating function of even sets. We establish a zero-free disk for this generating function inspired by techniques from statistical physics on partition functions of a polymer models. Our approach is quite general and we discuss extensions of it to a certain types of polymer models.

Cite

@article{arxiv.2311.05574,
  title  = {A near-optimal zero-free disk for the Ising model},
  author = {Viresh Patel and Guus Regts and Ayla Stam},
  journal= {arXiv preprint arXiv:2311.05574},
  year   = {2024}
}

Comments

12 pages; we have added a few propositions in Section 2 and reorganized the section to clarify the proof of Lemma 3.1. Some other small modifications have also been made as per suggestion of two referees

R2 v1 2026-06-28T13:16:35.007Z