Critical Behaviour in the Single Flavor Thirring Model in 2+1d

Abstract

Results of a lattice field theory simulation of the single-flavor Thirring model in 2+1 spacetime dimensions are presented. The lattice model is formulated using domain wall fermions as a means to recover the correct U(2) symmetries of the continuum model in the limit where wall separation $L_s\to \infty$. Simulations on $12^3,16^3\times L_s$, varying self-interaction strength $g^2$ and bare mass $m$ are performed with $L_s=8,\dots 48$, and the results for the bilinear condensate $⟨\bar{\psi }\psi ⟩$ fitted to a model equation of state assuming a U(2)$\to$U(1)$\otimes$U(1) symmetry-breaking phase transition at a critical $g_c^2$. First estimates for $g^{-2}a$ and critical exponents are presented, showing small but significant departures from mean-field values. The results confirm that a symmetry-breaking transition does exist and therefore the critical number of flavors for the Thirring model $N_c>1$. Results for both condensate and associated susceptibility are also obtained in the broken phase on $16^3\times 48$, suggesting that here the $L_s\to \infty$ extrapolation is not yet under control. We also present results obtained with the associated 2+1$d$ truncated overlap operator DOL demonstrating exponential localisation, a necessary condition for the recovery of U(2) global symmetry, but that recovery of the Ginsparg-Wilson condition as $L_s\to \infty$ is extremely slow in the broken phase.

Comments: 25 pages, 16 figures, a reference added and 2 figure captions amended