These are introductory lectures on application of the free field representation (bosonization) techniques to the solid-on-\S olid (SOS) and eight-vertex models.We start from the very beginnings, including the physical badcground of lattice models and some basic information on quantum integrability.After definitions of the eight-vertex and SOS models, we describe their relation known as the vertex-face correspondence.Then, skipping the Bethe ansatz solution, wc turn to the problem of calculation of correlation functions by mcaiis of the fit.cficld rcprcscntation.We explain, how the vertex-face correspondence works on the level of vertex operators and bosonization, making it possible to express the correlation functions of the eight-vertex model in terms of the free field representation aimed to describe the SOS model.1 Eight-vertex model arid commuting traxisfer Ilatl
⋅ ice.\'Since we shall speak about some models of physical importance.let us formulate first the general physical framework.Consider a classical system of interacting particles.Let
C be a state of this system, which can run some (generally infinite) set of admissible states.Let
E(C) be the energy of the state C. defined by usual IIamiltonian mechanics.Suppose that the system weakly interacts with a thermal bath of the temperature
T .The most fundamental postulate of statistical mechanics, the Gibbs law, says that the probability of the state
C is given by
w(C)=Z1e−B(C)/T .(1.1) lt is easy to understand, what is the proportionality coefficient
1/Z .As the total probability for thc system to be in any state is unity.we have for the partition functions of the system
Z=∑ce−F(C)/7 .(1.2) Since the space of configurations can be continu$ \mathit{0}\prime 18,$
†,11e\sum may turn out to be an
itιtegra↓↓ion , but we shall not consider this general case in these lectures.The partition function encodes the most fundamental observable thermodynamic function of the model, the free eneryy:
F=E−TS=−Tlog Z.(1.3)Here
E is the total energy of the system,
E=∑E(C)w(c,)=Z(T)dTT∼d,Z(T)=−T2dTTdF=F−TdTdF , while
S=−∑w(c,)logw(C)=−dTdΓ′is the entropy.The first equality in (1.3) is the thermodynamic definition of the free energy, which, in principle, was established before Gibbs, while the second equality provides its statistical interpretation.Let
fi⟨C ) be some functions of the state of the system.The correlation functions are generic expectation values
⟨f1…fr′)=∑c∣ι)(C)fι(C)…fn(C) .
The continuous limit of the eight-vertex model is shown to give solely the Massive Thirring Model (MTM). More precisely, using the light-cone lattice approach we find a whole class of lattice spacing (a) dependences in the eight vertex parameters (θ, γ, k) yielding a relative field theory in the a=0 limit. This turns out to be the MTM with no dependence on k. The exact excitation spectrum calculation presented here lead to these conclusions. Analogous results are reached from a perturbative renormalization group study of the anisotropic current-current continuum fermion field theory.
It is shown that a proper analytic continuation of eigenvalues of a special inhomogeneous eight-vertex system determines the "phases" and the spectrum of a one-dimensional fermion gas model, and thus provides a particular example of the long suspected connection between factorized
S matrices and lattice statistical systems.