English

Exploring axial $U(1)$ restoration in a modified 2+1 flavor Polyakov quark meson model

High Energy Physics - Phenomenology 2020-10-29 v2 Nuclear Theory

Abstract

We report on the UA(1)U_{A}(1) symmetry restoration resulting due to temperature dependence of the coefficient c(T) for the Kobayashi-Maskawa-'t Hooft determinant (KMT) term in a modified 2+1 flavor Polyakov loop quark meson model having fermionic vacuum correction term (PQMVT).Temperature dependence of KMT coupling c(T) drives the non-strange condensate melting to significantly smaller temperatures in comparison to the constant c case.Further due to c(T), mηm_{\eta^{\prime}} decreases from its vacuum value by 220 MeV near T=176 MeV after the chiral transition (Tcχ=154.9T_{c}^{\chi}=154.9 MeV).This is similar to the η\eta^{\prime} in-medium mass drop of at least 200 MeV as reported by Csorgo and Vertesi in Ref (Phys Rev Lett 105:182301,2010; Phys Rev C 83:054903,2011), as an experimental signature of the effective restoration of UA(1)U_A(1) symmetry. The pseudoscalar mixing angle θp\theta_p achieves anti-ideal mixing in the influence of c(T). The η\eta meson becomes light quark system (ηNS \eta_{NS} ) at T=176 MeV and changes its identity with η \eta' meson which becomes strange quark system (ηS \eta_{S} ). The degenerated temperature variations of σ\sigma, π\pi meson masses merges with the temperature variations of the masses of degenerated a0a_{0}, η\eta mesons near 275 MeV. It means that for c(T) when mσ=400m_{\sigma}=400 MeV, the UA(1)U_{A}(1) restoration takes place at 1.75 TcχT_{c}^{\chi}=275 MeV.

Keywords

Cite

@article{arxiv.1812.06786,
  title  = {Exploring axial $U(1)$ restoration in a modified 2+1 flavor Polyakov quark meson model},
  author = {Suraj Kumar Rai and Vivek Kumar Tiwari},
  journal= {arXiv preprint arXiv:1812.06786},
  year   = {2020}
}

Comments

20 pages, 14 figures. arXiv admin note: text overlap with arXiv:1301.3717