Finite-range interaction on a lattice

An interaction in which local energy terms depend only on spins within a bounded distance.
Finite-range interaction on a lattice

Fix a set of spin values SS. A configuration is a σ:ZdS\sigma:\mathbb{Z}^d\to S.

An interaction (also called a potential) is a family

Φ={ΦA}AZd, A<, \Phi=\{\Phi_A\}_{A\subset \mathbb{Z}^d,\ |A|<\infty},

where each ΦA\Phi_A is a function ΦA:SAR\Phi_A:S^A\to \mathbb{R} that depends only on the spins in the finite set AA.

Given a finite region ΛZd\Lambda\subset\mathbb{Z}^d, the associated finite-volume Hamiltonian is typically written as

HΛΦ(σ)=AΛΦA(σA), H_\Lambda^\Phi(\sigma)=\sum_{\varnothing\neq A\subseteq \Lambda}\Phi_A(\sigma|_A),

where σA\sigma|_A is the restriction of σ\sigma to AA.

Finite range. The interaction Φ\Phi is finite range with range RR if

ΦA0wheneverdiam(A)>R, \Phi_A \equiv 0 \quad\text{whenever}\quad \operatorname{diam}(A)>R,

where the diameter is computed using the nearest-neighbor graph distance on Zd\mathbb{Z}^d:

diam(A):=maxx,yAdist(x,y), \operatorname{diam}(A):=\max_{x,y\in A}\operatorname{dist}(x,y),

and dist(x,y)\operatorname{dist}(x,y) is the minimal number of steps needed to go from xx to yy.

Example (nearest-neighbor interactions). A nearest-neighbor pair interaction only uses terms supported on single sites and on pairs {x,y}\{x,y\} with xyx\sim y; this is a finite-range interaction (with a small range, depending on the chosen distance convention).