What if the neutron star maximum mass is beyond ∼2.3 M⊙?

By assuming the formation of a black hole soon after the merger event of GW170817, Shibata et al. updated the constraints on the maximum mass ($M_\textrm{max}$) of a stable neutron star within $\lesssim$ 2.3 $M_{\odot}$, but there is no solid evidence to rule out $M_\textrm{max}>2.3~M_{\odot}$ from the point of both microphysical and astrophysical views. In order to explain massive pulsars, it is naturally expected that the equation of state (EOS) would become stiffer beyond a specific density. In this paper, we consider the possibility of EOSs with $M_\textrm{max}>2.3~M_{\odot}$, investigating the stiffness and the transition density in a polytropic model. Two kinds of neutron stars are considered, i.e., normal neutron stars (the density vanishes on gravity-bound surface) and strange stars (a sharp density discontinuity on self-bound surface). The polytropic model has only two parameter inputs in both cases: ($\rho_{\rm t}$, $\gamma$) for gravity-bound objects, while ($\rho_{\rm s}$, $\gamma$) for self-bound ones, with $\rho_{\rm t}$ the transition density, $\rho_{\rm s}$ the surface density and $\gamma$ the polytropic exponent. In the matter of $M_\textrm{max}>2.3~M_{\odot}$, it is found that the smallest $\rho_{\rm t}$ and $\gamma$ should be $\sim 0.50~\rho_0$ and $\sim 2.65$ for normal neutron stars, respectively, whereas for strange star, we have $\gamma > 1.40$ if $\rho_{\rm s} > 1.0~\rho_0$ and $\rho_{\rm s} < 1.58~\rho_0$ if $\gamma <2.0$ ($\rho_0$ is the nuclear saturation density). These parametric results could guide further research of the real EOS with any foundation of microphysics if a pulsar mass higher than $2.3~M_{\odot}$ is measured in the future. We also derive rough results of common neutron star radius range, which is $9.8~\rm{km} < R_{1.4} < 13.8~\rm{km}$ for normal neutron stars and $10.5~\rm{km} < R_{1.4} < 12.5~\rm{km}$ for strange stars.