ψψ> in both isoscalar and isovector channels. With the first derivatives being small, we find that the second derivatives are sizable close to the phase transition and that the magnitude of ψψ decreases under the influence of finite chemical potential in both channels."> Phase transition in finite density and temperature lattice QCD -
  • [1]

    Wilson K G. Phys. Rev. D, 1974, 10: 2445[2] Martin A, Richard J M et al. Phys. Lett. B, 1995, 355: 345[3] Alexandrou C, Borrelli A et al. Phys. Lett. B, 1994, 337: 340[4] Tripolt R A, Smekal L V et al. Phys. Rev. D, 2014, 90: 074031[5] DING Heng-Tong, Francis A et al. Phys. Rev. D, 2011, 83: 034504[6] Nielson H B, Ninomiya M et al. Nucl. Phys. B, 1981, 193: 173[7] Ginparg P H, Wilson K G et al. Phys. Rev. D, 1982, 25: 2649[8] Maarten F L Golterman. Nucl. Phys. B, 1986, 278: 417[9] Bali G S, Bruckmann F et al. JHEP, 2012, 1202: 044[10] GAO Jian-Hua, LIANG Zuo-Tang et al. Phys. Rev. Lett, 2012, 109: 232301[11] YU Lang, LIU Hao et al. Phys. Rev. D, 2014, 90: 074009[12] Choe S, Forcrand P D et al. Phys. Rev. D, 2002, 65: 054501

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