Abstract
We study the competition between induced symmetry breaking (ISB), Cooper pairing (superconductivity) and chiral condensation at finite non-asymptotic density. Using a quantum mechanical model studied recently by Ilieva and Thirring, we analyze the expectation value of the fermion number density $\la a^*a\ra$ in the presence of chemical potential and discuss relevance of the ISB phenomenon in the model. By Bogoliubov transformation, we obtain the ground state energy and find that a phase with both superconducting and mean field gap is a true ground state. We also study the effective potentials of a two-dimensional field theory model for competitions between $\la\barψψ\ra$, $\laψψ\ra$ and $\laψ^\daggerψ\ra$. We find that in the regime , where is found to be around with being the renormalizaton point of chiral condensate, we have a chiral symmetry-breaking phase with almost zero fermion number density and in the case of the system sits in the mixed phase characterized by $\la ψ^\daggerψ\ra\neq 0$ and $\la ψψ\ra\neq 0$ as long as the renormalization point, , corresponding to a superconducting gap is not zero, .
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