# Eight-vertex model

In statistical mechanics, the eight-vertex model is a generalisation of the ice-type (six-vertex) models; it was discussed by Sutherland, and Fan & Wu, and solved by Baxter in the zero-field case.

## Description

As with the ice-type models, the eight-vertex model is a square lattice model, where each state is a configuration of arrows at a vertex. The allowed vertices have an even number of arrows pointing towards the vertex; these include the six inherited from the ice-type model (1-6), and sinks and sources (7, 8).

We consider a $N\times N$ lattice, with $N^{2}$ vertices and $2N^{2}$ edges. Imposing periodic boundary conditions requires that the states 7 and 8 occur equally often, as do states 5 and 6, and thus can be taken to have the same energy. For the zero-field case the same is true for the two other pairs of states. Each vertex $j$ has an associated energy $\epsilon _{j}$ and Boltzmann weight $w_{j}=e^{-{\frac {\epsilon _{j}}{kT}}}$ , giving the partition function over the lattice as

$Z=\sum \exp \left(-{\frac {\sum _{j}n_{j}\epsilon _{j}}{kT}}\right)$ where the summation is over all allowed configurations of vertices in the lattice. In this general form the partition function remains unsolved.

## Solution in the zero-field case

The zero-field case of the model corresponds physically to the absence of external electric fields. Hence, the model remains unchanged under the reversal of all arrows; the states 1 and 2, and 3 and 4, consequently must occur as pairs. The vertices can be assigned arbitrary weights

{\begin{aligned}w_{1}=w_{2}&=a\\w_{3}=w_{4}&=b\\w_{5}=w_{6}&=c\\w_{7}=w_{8}&=d.\end{aligned}} The solution is based on the observation that rows in transfer matrices commute, for a certain parametrisation of these four Boltzmann weights. This came about as a modification of an alternate solution for the six-vertex model; it makes use of elliptic theta functions.

### Commuting transfer matrices

{\begin{aligned}\Delta &={\frac {a^{2}+b^{2}-c^{2}-d^{2}}{2(ab+cd)}}\\\Gamma &={\frac {ab-cd}{ab+cd}}\end{aligned}} $a:b:c:d=\operatorname {snh} (\eta -u):\operatorname {snh} (\eta +u):\operatorname {snh} (2\eta ):k\operatorname {snh} (2\eta )\operatorname {snh} (\eta -u)\operatorname {snh} (\eta +u)$ {\begin{aligned}\operatorname {snh} (u)&=-i\operatorname {snh} (iu)\\{\text{where }}\operatorname {snh} (u)&={\frac {H(u)}{k^{1/2}\Theta (u)}}\end{aligned}} $T(u)T(v)=T(v)T(u).$ ### The matrix function $Q(u)$ The other crucial part of the solution is the existence of a nonsingular matrix-valued function $Q$ , such that for all complex $u$ the matrices $Q(u),Q(u')$ commute with each other and the transfer matrices, and satisfy Template:NumBlk where

{\begin{aligned}\zeta (u)&=[c^{-1}H(2\eta )\Theta (u-\eta )\Theta (u+\eta )]^{N}\\\phi (u)&=[\Theta (0)H(u)\Theta (u)]^{N}.\end{aligned}} The existence and commutation relations of such a function are demonstrated by considering pair propagations through a vertex, and periodicity relations of the theta functions, in a similar way to the six-vertex model.

### Explicit solution

The commutation of matrices in (Template:EquationNote) allow them to be diagonalised, and thus eigenvalues can be found. The partition function is calculated from the maximal eigenvalue, resulting in a free energy per site of

{\begin{aligned}f=\epsilon _{5}-2kT\sum _{n=1}^{\infty }{\frac {\sinh ^{2}((\tau -\lambda )n)(\cosh(n\lambda )-\cosh(n\alpha ))}{n\sinh(2n\tau )\cosh(n\lambda )}}\end{aligned}} for

{\begin{aligned}\tau &={\frac {\pi K'}{2K}}\\\lambda &={\frac {\pi \eta }{iK}}\\\alpha &={\frac {\pi u}{iK}}\end{aligned}} ## Equivalence with an Ising model

There is a natural correspondence between the eight-vertex model, and the Ising model with 2-spin and 4-spin nearest neighbour interactions. The states of this model are spins $\sigma =\pm 1$ on faces of a square lattice. The analogue of 'edges' in the eight-vertex model are products of spins on adjacent faces:

{\begin{aligned}\alpha _{ij}&=\sigma _{ij}\sigma _{i,j+1}\\\mu _{ij}&=\sigma _{ij}\sigma _{i+1,j}.\end{aligned}} The most general form of the energy for this model is

{\begin{aligned}\epsilon &=-\sum _{ij}(J_{h}\mu _{ij}+J_{v}\alpha _{ij}+J\alpha _{ij}\mu _{ij}+J'\alpha _{i+1,j}\mu _{ij}+J''\alpha _{ij}\alpha _{i+1,j})\end{aligned}} We denote horizontal and vertical spins (arrows on edges) in the eight-vertex model $\mu$ , $\alpha$ respectively, and define up and right as positive directions. The restriction on vertex states is that the product of four edges at a vertex is 1; this automatically holds for Ising 'edges'. Each $\sigma$ configuration then corresponds to a unique $\mu$ , $\alpha$ configuration, whereas each $\mu$ , $\alpha$ configuration gives two choices of $\sigma$ configurations.

{\begin{aligned}\epsilon _{1}&=-J_{h}-J_{v}-J-J'-J'',\quad \epsilon _{2}=J_{h}+J_{v}-J-J'-J''\\\epsilon _{3}&=-J_{h}+J_{v}+J+J'-J'',\quad \epsilon _{2}=J_{h}-J_{v}+J+J'-J''\\\epsilon _{5}&=\epsilon _{6}=J-J'+J''\\\epsilon _{7}&=\epsilon _{8}=-J+J'+J''.\end{aligned}} It follows that in the zero-field case of the eight-vertex model, the horizontal and vertical interactions in the corresponding Ising model vanish.

These relations gives the equivalence $Z_{I}=2Z_{8V}$ between the partition functions of the eight-vertex model, and the 2,4-spin Ising model. Consequently a solution in either model would lead immediately to a solution in the other.