Table 9.

Same as Table 6, but with both rotation (⁠|$\Omega=6\times10^{2}$| Hz) and magnetic fields (⁠|$B_0=2.5\times 10^{18}$|  |$\rm{G}$|⁠).

EoS|$M_{\rm{max}}$||$R^p_{1.4\,M_\odot}$||$R^e_{1.4\,M_\odot}$||$e$|
GM12.05013.8913.930.083
TM1-a1.88414.4214.480.095
TM1-b2.06114.4314.500.096
TM2|$\omega \rho$|-a1.98013.5413.620.11
TM2|$\omega \rho$|-b2.13613.5413.620.11
NL3-a2.31414.5114.540.064
NL3-b2.48714.7214.760.074
NL3|$\omega \rho$|-a2.36013.6713.730.094
NL3|$\omega \rho$|-b2.51313.6713.730.094
DDME2-a2.34614.2314.310.11
DDME2-b2.50614.2314.310.11
EoS|$M_{\rm{max}}$||$R^p_{1.4\,M_\odot}$||$R^e_{1.4\,M_\odot}$||$e$|
GM12.05013.8913.930.083
TM1-a1.88414.4214.480.095
TM1-b2.06114.4314.500.096
TM2|$\omega \rho$|-a1.98013.5413.620.11
TM2|$\omega \rho$|-b2.13613.5413.620.11
NL3-a2.31414.5114.540.064
NL3-b2.48714.7214.760.074
NL3|$\omega \rho$|-a2.36013.6713.730.094
NL3|$\omega \rho$|-b2.51313.6713.730.094
DDME2-a2.34614.2314.310.11
DDME2-b2.50614.2314.310.11
Table 9.

Same as Table 6, but with both rotation (⁠|$\Omega=6\times10^{2}$| Hz) and magnetic fields (⁠|$B_0=2.5\times 10^{18}$|  |$\rm{G}$|⁠).

EoS|$M_{\rm{max}}$||$R^p_{1.4\,M_\odot}$||$R^e_{1.4\,M_\odot}$||$e$|
GM12.05013.8913.930.083
TM1-a1.88414.4214.480.095
TM1-b2.06114.4314.500.096
TM2|$\omega \rho$|-a1.98013.5413.620.11
TM2|$\omega \rho$|-b2.13613.5413.620.11
NL3-a2.31414.5114.540.064
NL3-b2.48714.7214.760.074
NL3|$\omega \rho$|-a2.36013.6713.730.094
NL3|$\omega \rho$|-b2.51313.6713.730.094
DDME2-a2.34614.2314.310.11
DDME2-b2.50614.2314.310.11
EoS|$M_{\rm{max}}$||$R^p_{1.4\,M_\odot}$||$R^e_{1.4\,M_\odot}$||$e$|
GM12.05013.8913.930.083
TM1-a1.88414.4214.480.095
TM1-b2.06114.4314.500.096
TM2|$\omega \rho$|-a1.98013.5413.620.11
TM2|$\omega \rho$|-b2.13613.5413.620.11
NL3-a2.31414.5114.540.064
NL3-b2.48714.7214.760.074
NL3|$\omega \rho$|-a2.36013.6713.730.094
NL3|$\omega \rho$|-b2.51313.6713.730.094
DDME2-a2.34614.2314.310.11
DDME2-b2.50614.2314.310.11
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