A Class of Gaussian Fields on $\mathbb{Z}_q^d$
Robert Griffiths, Shuhei Mano
TL;DR
This paper constructs and analyzes a broad class of Gaussian fields indexed by ${\cal V}_{q,d}$ arising from reversible long-range random walks on ${\cal Z}_q^d$ with killing parameter $\alpha$. It develops spectral decompositions via circulant structures, extends to continuous-state tori and infinite dimensions via de Finetti exchangeability, and establishes central limit limits to Gaussian fields on $\mathbb{R}^d$; it also derives a transform with a simpler covariance and a Hamiltonian leading to a partition-function limit. The work unifies Green-function/killing techniques, de Finetti mixtures, and multivariate Krawtchouk polynomials to obtain explicit eigenstructures for both discrete and continuous models, including torus and infinite-dimensional settings. It further connects these Gaussian fields to Hamiltonians and partition-functions, and discusses Potts-model-type interpretations and free-energy implications in large dimension. The results provide a versatile framework for analyzing Gaussian fields linked to long-range random-walk structures and their thermodynamic limits, with potential applications to spin-glass-type phenomena on discrete and continuous spaces.
Abstract
Gaussian fields $(g_x)$ on $\mathbb{Z}_q^d$ are constructed from a class of reversible long range random walks $(X_t)_{t\in \mathbb{N}}$ on $\mathbb{Z}_q^d$ in arXiv:2510.22554. The construction is from taking the covariance function of $(g_x)$ as $(1-α)G(x,y;α)$, where $G(x,y;α)$ is the Green function of a random walk with killing in each transition at rate $1-α$. A decomposition of the Gaussian field into a sum of independent Gaussian random variables is made. By letting $q\to \infty$ the Gaussian field becomes defined from an infinite-dimensional random walk on a torus. The random walk model is also extended to $d=\infty$ by considering a de Finetti random walk where entries in the increments of the random walk are exchangeable. A limit Gaussian field on $\mathbb{R}^d$ arises from a central limit theorem approach. The transform of this Gaussian field, which is again a Gaussian field, is calculated. It has a simpler covariance matrix than the original field. The Hamiltonian connected to the Gaussian field is calculated. A limit theorem for the partition function arising from the Hamiltonian is found.
