Integrable Gross-Neveu models with fermion-fermion and fermion-antifermion pairing
arXiv:1408.5506 · doi:10.1103/PhysRevD.90.105017
Abstract
The massless Gross-Neveu and chiral Gross-Neveu models are well known examples of integrable quantum field theories in 1+1 dimensions. We address the question whether integrability is preserved if one either replaces the four-fermion interaction in fermion-antifermion channels by a dual interaction in fermion-fermion channels, or if one adds such a dual interaction to an existing integrable model. The relativistic Hartree-Fock-Bogoliubov approach is adequate to deal with the large N limit of such models. In this way, we construct and solve three integrable models with Cooper pairing. We also identify a candidate for a fourth integrable model with maximal kinematic symmetry, the "perfect" Gross-Neveu model. This type of field theories can serve as exactly solvable toy models for color superconductivity in quantum chromodynamics.
16 pages, 4 figures
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Cited by in corpus (6)
- Inhomogeneous charged pion condensation in chiral asymmetric dense quark matter in the framework of NJL model
- Duality between chiral symmetry breaking and charged pion condensation at large : Consideration of an NJL model with baryon-, isospin- and chiral isospin chemical potentials
- Interplay between superconductivity and chiral symmetry breaking in a (2+1)-dimensional model with compactified spatial coordinate
- Gross-Neveu model with O(2)O(2) chiral symmetry: Duality with Zakharov-Mikhailov model and large solution
- Dark solitons of the Gross-Neveu model
- Detecting inhomogeneous chiral condensation from the bosonic two-point function in the -dimensional Gross-Neveu model in the mean-field approximation