$U_L(N)\times U_R(N)$-invariant four-fermion interactions and Nambu-Goldstone mechanism at finite temperature

Details $U_L(N)\times U_R(N)$-invariant four-fermion interactions and Nambu-Goldstone mechanism at finite temperature $U_L(N)\times U_R(N)$-invariant four-fermion interactions and Nambu-Goldstone mechanism at finite temperature

1999-01-08

arxiv.org/abs/hep-th/9901025v1

Commun.Theor.Phys.33:113-118,2000

Physics

High Energy Physics

High Energy Physics - Theory

8 pages, Latex, no figures

Scientific paper

In a chiral $U_L(N)\times U_R(N)$ fermion model of NJL-form, we prove that, if all the fermions are assumed to have equal masses and equal chemical potentials, then at the finite temperature $T$ below the symmetry restoration temperature $T_c$, there will be $N^2$ massive scalar composite particles and $N^2$ massless pseudoscalar composite particles (Nambu-Goldstone bosons). This shows that the Goldstone Theorem at finite temperature for spontaneous symmetry breaking $U_L(N)\times U_R(N) \to U_{L+R}(N)$ is consistent with the real-time formalism of thermal field theory in this model.

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