Fast mixing via polymers for random graphs with unbounded degree

TL;DR

This paper introduces a new polymer model framework that relaxes the bounded-degree assumption, enabling efficient approximation algorithms for spin systems on more general graphs, including those with unbounded degrees.

Contribution

The authors develop a less restrictive polymer model framework based on the edge perspective, allowing analysis on graphs with unbounded degrees.

Findings

Applicable to random graphs with unbounded degrees from fixed degree sequences.

Provides approximation algorithms for the ferromagnetic Potts model.

Extends to more general spin systems.

Abstract

The polymer model framework is a classical tool from statistical mechanics that has recently been used to obtain approximation algorithms for spin systems on classes of bounded-degree graphs; examples include the ferromagnetic Potts model on expanders and on the grid. One of the key ingredients in the analysis of polymer models is controlling the growth rate of the number of polymers, which has been typically achieved so far by invoking the bounded-degree assumption. Nevertheless, this assumption is often restrictive and obstructs the applicability of the method to more general graphs. For example, sparse random graphs typically have bounded average degree and good expansion properties, but they include vertices with unbounded degree, and therefore are excluded from the current polymer-model framework. We develop a less restrictive framework for polymer models that relaxes the standard bounded-degree assumption, by reworking the relevant polymer models from the edge perspective. The edge perspective allows us to bound the growth rate of the number of polymers in terms of the total degree of polymers, which in turn can be related more easily to the expansion properties of the underlying graph. To apply our methods, we consider random graphs with unbounded degrees from a fixed degree sequence (with minimum degree at least 3) and obtain approximation algorithms for the ferromagnetic Potts model, which is a standard benchmark for polymer models. Our techniques also extend to more general spin systems.