Please use this identifier to cite or link to this item: http://hdl.handle.net/10316/7697
Title: Path integral bosonization of the ‘t Hooft determinant: quasi-classical corrections
Authors: Osipov, A. A. 
Hiller, B. 
Issue Date: 2004
Citation: The European Physical Journal C - Particles and Fields. 35:2 (2004) 223-241
Abstract: The many-fermion Lagrangian which includes the ‘t Hooft six-quark flavor mixing interaction ( N f = 3) and the U L(3) x U R(3) chiral symmetric four-quark Nambu-Jona-Lasinio- (NJL-) type interactions is bosonized by the path integral method. The method of the steepest descents is used to derive the effective quark-mesonic Lagrangian with linearized many-fermion vertices. We obtain, additionally to the known lowest order stationary phase result of Reinhardt and Alkofer, the next to leading order (NLO) contribution arising from quantum fluctuations of auxiliary bosonic fields around their stationary phase trajectories (the Gaussian integral contribution). Using the gap equation we construct the effective potential, from which the structure of the vacuum can be settled. For some set of parameters the effective potential has several extrema, that in the case of SU(2) I x U(1) Y flavor symmetry can be understood on topological grounds. With increasing strength of the fluctuations the spontaneously broken phase gets unstable and the trivial vacuum is restored. The effective potential reveals furthermore the existence of logarithmic singularities at certain field expectation values, signalizing caustic regions.
URI: http://hdl.handle.net/10316/7697
DOI: 10.1140/epjc/s2004-01779-3
Rights: openAccess
Appears in Collections:FCTUC Física - Artigos em Revistas Internacionais

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