Influences of magnetic field on the coexistence of diquark and chiral condensates in the Nambu–Jona–Lasinio model with axial anomaly

Xiao-Bing Zhang(张小兵),Fu-Ping Peng(彭富平),Yun-Ben Wu(吴云奔),Yi Zhang(张一)

Figure 6. Strong-field result of $H^{\prime} $ required for BECI transition. This is obtained at a given quark chemical potential, and $H^{\prime} $ is normalized with respect to its zero-field value ${H}_{0}^{{\prime} }$ .