Thirring model

Not to be confused with Thirring–Wess model.

Not to be confused with Gross-Neveu model.

The Thirring model is an exactly solvable quantum field theory which describes the self-interactions of a Dirac field in two dimension.

Definition

The Thirring model is given by the Lagrangian density

$\mathcal{L}= \overline{\psi}(i\partial\!\!\!/-m)\psi -\frac{g}{2}\left(\overline{\psi}\gamma^\mu\psi\right) \left(\overline{\psi}\gamma_\mu \psi\right)\$

where $\psi=(\psi_+,\psi_-)$ is the field, g is the coupling constant, m is the mass, and $\gamma^\mu$, for $\mu = 0,1$, are the two-dimensional gamma matrices.

This is the unique model of two-dimensional, Dirac fermions with a local (self-)interaction. Indeed, since there are only 4 independent fields, because of Pauli principle, all the quartic, local interactions are equivalent; and all higher power, local interactions vanish. (Interactions containing derivatives, such as $(\bar \psi\partial\!\!\!/\psi)^2$, are not considered because non-renormalizable.)

The correlation functions of the Thirring model (massive or massless) verify the Osterwalder-Schrader axioms, and hence the theory makes sense as a quantum field theory.

Massless Case

The massless Thirring model is exactly solvable in the sense that a formula for the $n$-points field correlation is known.

Exact Solution

After it was introduced by Walter Thirring, many authors tried to solve the massless case, with confusing outcomes. The correct formula for the two and four point correlation was finally found by K. Johnson ; then C. Hagen and B. Klaiber extended the explicit solution to any multipoint correlation function of the fields.

Massive Case

The mass spectrum of the model and the scattering matrix was explicitly evaluated by Bethe Ansatz. Though, an explicit formula for the correlations is not known. J. I. Cirac, P. Maraner and J. K. Pachos applied massive Thirring model for description of optical lattices in .

Exact Solution

In one space and one time dimension the model can be solved by Bethe Ansatz. This helps to calculate exactly mass spectrum and scattering matrix. Calculation of the scattering matrix reproduce the results published earlier by Alexander Zamolodchikov. The paper with exact solution of Massive Thirring model by Bethe Ansatz was first published in Russian. The paper was then translated into English. Ultraviolet renormalization was done in the frame of Bethe ansatz. The fractional charge appears in the model during renormalization as a repulsion beyond cutoff.

Multi particle production cancels on mass shell.

Exact solution shows once again the equivalence of Thirring model and quantum sine-Gordon model. The Thirring model is S-dual to the sine-Gordon model. The fundamental fermions of the Thirring model correspond to the solitons of the sine-Gordon model.

Bosonization

S. Coleman discovered an equivalence between the Thirring and the sine-Gordon models. Despite the fact that the latter is a pure boson model, massless Thirring fermions are equivalent to free bosons; besides massive fermions are equivalent to the sine-Gordon bosons. This phenomenon is more general in two dimensions and is called bosonization.

External links

• On the equivalence between sine-Gordon Model and Thirring Model in the chirally broken phase