Finite size effects in the Gross-Neveu model with isospin chemical potential

preprint2008arXivOpen access

Abstract

The properties of the two-flavored Gross-Neveu model in the (1+1)-dimensional R1×S1R^1\times S^1 spacetime with compactified space coordinate are investigated in the presence of the isospin chemical potential μIμ_I. The consideration is performed in the limit Nc→∞N_c\to\infty, i.e. in the case with infinite number of colored quarks. It is shown that at L=∞L=\infty (LL is the length of the circumference S1S^1) the pion condensation phase is realized for arbitrary small nonzero μIμ_I. At finite values of LL, the phase portraits of the model in terms of parameters ν∼μIν\simμ_I and λ∼1/Lλ\sim 1/L are obtained both for periodic and antiperiodic boundary conditions of the quark field. It turns out that in the plane (λ,ν)(λ,ν) there is a strip 0≤λ<λc0\leλ<λ_c which lies as a whole inside the pion condensed phase. In this phase the pion condensation gap is an oscillating function vs both λλ (at fixed νν) and νν (at fixed λλ).

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