Emergence of Tricritical Point and Liquid-Gas Phase in the Massless 2+1 Dimensional Gross-Neveu Model
arXiv:0705.0676 · doi:10.1103/PhysRevD.76.045020
Abstract
A complete thermodynamical analysis of the 2+1 dimensional massless Gross-Neveu model is performed using the optimized perturbation theory. This is a non-perturbative method that allows us to go beyond the known large-N results already at lowest order. Our results, for a finite number of fermion species, N, show the existence of a tricritical point in the temperature and chemical potential phase diagram for discrete chiral phase transition allowing us to precisely to locate it. By studying the phase diagram in the pressure and inverse density plane, we also show the existence of a liquid-gas phase, which, so far, was unknown to exist in this model. Finally, we also derive N dependent analytical expressions for the fermionic mass, critical temperature and critical chemical potential.
26 pages, 15 eps figures. Replaced with version that matches the published one
References in corpus (3)
- Asymptotically Improved Convergence of Optimized Perturbation Theory in the Bose-Einstein Condensation Problem
- Non-universal Critical Quantities from Variational Perturbation Theory and Their Application to the BEC Temperature Shift
- Critical and Tricritical Points for the Massless 2d Gross-Neveu Model Beyond Large N
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