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Deterministic approximate counting of colorings with fewer than $2Δ$ colors via absence of zeros

Ferenc Bencs, Khallil Berrekkal, Guus Regts

TL;DR

The paper proves a new zero-free region for the antiferromagnetic Potts model partition function $Z_G(q; w)$ that persists for all graphs with maximum degree $\Delta$ when $q\ge (2-\eta)\Delta$ with a fixed $\eta\ge 0.002$. This enables a deterministic polynomial-time algorithm, via Barvinok\'s interpolation, to approximate the number of proper $q$-colorings for such graphs, thereby breaking the longstanding $q=2\Delta$ barrier. The approach hinges on a careful analysis of log-ratios of colorings, induction on partially colored graphs, and gradient-based control of perturbations, augmented by refined local bounds on root marginals. The results also yield local central limit-type consequences for the number of monochromatic edges and open avenues for extensions to multivariate Potts, list-colorings, and small-degree regimes, with potential improvements for triangle-free graphs. Overall, the work advances deterministic approximate counting in graph coloring by leveraging a refined zero-free region and locality-aware inductive techniques.

Abstract

Let $Δ,q\geq 3$ be integers. We prove that there exists $η\geq 0.002$ such that if $q\geq (2-η)Δ$, then there exists an open set $\mathcal{U}\subset \mathbb{C}$ that contains the interval $[0,1]$ such that for each $w\in \mathcal{U}$ and any graph $G=(V,E)$ of maximum degree at most $Δ$, the partition function of the anti-ferromagnetic $q$-state Potts model evaluated at $w$ does not vanish. This provides a (modest) improvement on a result of Liu, Sinclair, and Srivastava, and breaks the $q=2Δ$-barrier for this problem. As a direct consequence we obtain via Barvinok's interpolation method a deterministic polynomial time algorithm to approximate the number of proper $q$-colorings of graphs of maximum degree at most $Δ$, provided $q\geq (2-η)Δ$.

Deterministic approximate counting of colorings with fewer than $2Δ$ colors via absence of zeros

TL;DR

The paper proves a new zero-free region for the antiferromagnetic Potts model partition function that persists for all graphs with maximum degree when with a fixed . This enables a deterministic polynomial-time algorithm, via Barvinok\'s interpolation, to approximate the number of proper -colorings for such graphs, thereby breaking the longstanding barrier. The approach hinges on a careful analysis of log-ratios of colorings, induction on partially colored graphs, and gradient-based control of perturbations, augmented by refined local bounds on root marginals. The results also yield local central limit-type consequences for the number of monochromatic edges and open avenues for extensions to multivariate Potts, list-colorings, and small-degree regimes, with potential improvements for triangle-free graphs. Overall, the work advances deterministic approximate counting in graph coloring by leveraging a refined zero-free region and locality-aware inductive techniques.

Abstract

Let be integers. We prove that there exists such that if , then there exists an open set that contains the interval such that for each and any graph of maximum degree at most , the partition function of the anti-ferromagnetic -state Potts model evaluated at does not vanish. This provides a (modest) improvement on a result of Liu, Sinclair, and Srivastava, and breaks the -barrier for this problem. As a direct consequence we obtain via Barvinok's interpolation method a deterministic polynomial time algorithm to approximate the number of proper -colorings of graphs of maximum degree at most , provided .
Paper Structure (21 sections, 17 theorems, 33 equations, 1 figure)

This paper contains 21 sections, 17 theorems, 33 equations, 1 figure.

Key Result

Theorem 1.1

There exists a constant $\eta\geq 0.002$ such that for all integers $\Delta\geq 3$ and $q\geq (2-\eta)\Delta$ there exists an open set $\mathcal{U}\subset \mathbb{C}$ containing the interval $[0,1]$ such that for each $w\in \mathcal{U}$ and graph $G$ of maximum degree at most $\Delta$, $Z_G(q,w)\neq

Figures (1)

  • Figure 4: Pictorial depiction of how the ratio $Z^{\ell_1}_{G,v}(w) /Z^{\ell_2}_{G,v}(w)$ is expressed as a telescoping product of the ratios $Z^{\ell_1}_{\hat{G}_i,\hat{v}_i}(w) / Z^{\ell_2}_{\hat{G}_i,\hat{v}_i}(w)$.

Theorems & Definitions (23)

  • Theorem 1.1
  • corollary 1.2
  • Theorem 2.1
  • remark 2.2
  • Lemma 2.3
  • Lemma 3.1
  • remark 3.2
  • Lemma 3.3
  • Lemma 4.1
  • proposition 4.2
  • ...and 13 more