Spin Polarized versus Chiral Condensate in Quark Matter at Finite Temperature and Density
arXiv:1601.01403 · doi:10.1093/ptep/ptw055
Abstract
It is shown that the spin polarized condensate appears in quark matter at high baryon density and low temperature due to the tensor-type four-point interaction in the Nambu-Jona-Lasinio-type model as a low energy effective theory of quantum chromodynamics. It is indicated within this low energy effective model that the chiral symmetry is broken again by the spin polarized condensate as increasing the quark number density, while the chiral symmetry restoration occurs in which the chiral condensate disappears at a certain density.
25 pages, 9 figures
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Cited by in corpus (12)
- Spin polarization and color superconductivity in the Nambu--Jona-Lasinio model at finite temperature
- Spontaneous magnetization under a pseudovector interaction between quarks in high density quark matter
- Hybrid stars from the NJL model with a tensor interaction
- Spin polarized phases in strongly interacting matter: interplay between axial-vector and tensor mean fields
- Spin polarization in high density quark matter under a strong external magnetic field
- Modified dilepton production rate from charged pion-pair annihilation in the inhomogeneous chiral condensed phase
- Spin polarizations under a pseudovector interaction between quarks with the Kobayashi-Maskawa-'t Hooft term in high density quark matter
- Spin Polarization and Chiral Condensation in 2+1 flavor Nambu-Jona-Lasinio model at finite temperature and baryon chemical potential
- Hybrid stars from a three-flavor NJL model with two kinds of tensor condensates
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- A possibility of existence of a pseudovector-type quark-antiquark condensate in the quark matter and Nambu-Goldstone modes on that condensate in the Nambu-Jona-Lasinio model
- Axial-Vector and Tensor Spin Polarization and Chiral Restoration in Quark Matter