Table 4: Pressure coefficient $\kappa$ , adiabatic index $\gamma$ and baryon mass $M_{\rm B}$ for polytropic NSs having the same compactness parameter and mass ( $M=1.35~{M}_\odot$ ) than NSs described by realistic EOSs (Table 1) ( $\hat{\rho}:=1.66$ $\times$ $10^{14}~{\rm g/cm^3}$ and $\hat{n}:=0.1~{\rm fm^{-3}}$ ).
corresponding EOS $\gamma$ $\kappa \ [\hat{\rho}c^2 \hat{n}^{-\gamma}]$ $M_{\rm B} [M_{\odot}]$

GNH3 2. 0.02645 1.44802

2. 0.02037 1.47016

APR

2.5 0.01094 1.49561

BPAL12 2. 0.01908 1.47742

**Table 4:** Pressure coefficient $\kappa$ , adiabatic index $\gamma$ and baryon mass $M_{\rm B}$ for polytropic NSs having the same compactness parameter and mass ( $M=1.35~{M}_\odot$ ) than NSs described by realistic EOSs (Table 1) ( $\hat{\rho}:=1.66$ $\times$ $10^{14}~{\rm g/cm^3}$ and $\hat{n}:=0.1~{\rm fm^{-3}}$ ).
corresponding EOS	$\gamma$	$\kappa \ [\hat{\rho}c^2 \hat{n}^{-\gamma}]$	$M_{\rm B} [M_{\odot}]$
GNH3	2.	0.02645	1.44802
	2.	0.02037	1.47016
APR
	2.5	0.01094	1.49561
BPAL12	2.	0.01908	1.47742

Source LaTeX | All tables | In the text

	1 Introduction
	2 Description of the equations of state
	3 Numerical method
	4 Numerical results
	5 Concluding remarks
	References