Erratum: Asymmetric nuclear matter in a parity doublet model with hidden local symmetry [Phys. Rev. C 92, 025201 (2015)]

Figure 1

(a) Density dependence of the binding energy. (b) The pressure for $m_0=500\mathrm{MeV}.{\rho }_B$ is the baryon number density, and ${\rho }_n$ is the neutron number density: ${\rho }_n/{\rho }_B=0.5$ implies symmetric nuclear matter, and ${\rho }_n/{\rho }_B=1$ implies pure neutron matter.

Figure 2

(a) Baryon number chemical potential dependence of ${\sigma }_0$. (b) Chemical potential dependence of ${\rho }_B$ for $m_0=500$ and ${\mu }_I=0\mathrm{MeV}$.

Figure 3

Density dependence of the effective nucleon masses for $m_0=500\mathrm{MeV}$ at ${\mu }_I=0\mathrm{MeV}$.

Figure 4

Phase diagrams for $m_0=900\mathrm{MeV}$ at (a) ${\mu }_I=0\mathrm{MeV}$ and (b) ${\mu }_I=100\mathrm{MeV}$. The solid line is for the first-order phase transition, the dashed line is for the crossover, and the point is for the critical point (second order).

Figure 5

Phase diagrams for $m_0=500\mathrm{MeV}$.