Table 4.
Spectral representation of all the employed RMF EOS.
| EOS | γ0 | γ1 | γ2 | γ3 | p0 | % RE |
|---|---|---|---|---|---|---|
| EOS1 | 0.9368 | 0.5084 | –0.1512 | 0.0100 | 2.3e+33 | 0.5023 |
| EOS2 | 0.6425 | 0.7209 | –0.2287 | 0.0172 | 2.4e+33 | 0.0518 |
| EOS3 | 0.6488 | 0.7571 | –0.2360 | 0.0175 | 2.2e+33 | 0.0721 |
| EOS4 | 1.0026 | 0.4939 | –0.1660 | 0.0119 | 1.4e+33 | 0.0439 |
| EOS5 | 0.8759 | 0.5776 | –0.1959 | 0.0147 | 1.9e+33 | 0.0542 |
| EOS6 | 1.1172 | 0.1133 | –0.0317 | 0.0012 | 1.1e+33 | 0.0799 |
| EOS7 | 1.1334 | 0.0755 | –0.0249 | 0.0009 | 1.4e+33 | 0.0634 |
| EOS8 | 1.2349 | 0.0871 | –0.0326 | 0.0013 | 1.3e+33 | 0.1359 |
| EOS9 | 1.3365 | 0.0650 | –0.0342 | 0.0021 | 1.0e+33 | 0.2074 |
| EOS10 | 1.4053 | –0.0054 | –0.0168 | 0.0007 | 1.1e+33 | 0.0948 |
| EOS11 | 0.7885 | 0.3558 | –0.0918 | 0.0048 | 2.2e+33 | 0.2113 |
| EOS12 | 1.1019 | 0.1633 | –0.0494 | 0.0023 | 1.6e+33 | 0.0668 |
| EOS13 | 0.6199 | 0.5032 | –0.1221 | 0.0071 | 2.5e+33 | 0.2778 |
| EOS14 | 1.0968 | 0.2814 | –0.0868 | 0.0049 | 1.3e+33 | 0.1851 |
| EOS15 | 1.1175 | 0.2604 | –0.0715 | 0.0034 | 1.0e+33 | 0.3341 |
| EOS16 | 0.9500 | 0.3657 | –0.1142 | 0.0073 | 1.7e+33 | 0.1548 |
| EOS17 | 0.6207 | 0.5822 | –0.1499 | 0.0091 | 2.3e+33 | 0.2642 |
| EOS18 | 0.6025 | 0.6341 | –0.1615 | 0.0098 | 2.0e+33 | 0.2765 |
| EOS19 | 0.6244 | 0.6703 | –0.1802 | 0.0115 | 1.8e+33 | 0.2340 |
| EOS20 | 0.7339 | 0.6448 | –0.1634 | 0.0097 | 1.2e+33 | 0.2055 |
| EOS21 | 0.9125 | 0.5346 | –0.1416 | 0.0088 | 1.2e+33 | 0.4828 |
Notes. The conversion of the 21 EOSs to the spectral representation format Lindblom (2010) is in pressure based forms, where ϵ0/c2 = 2.03 × 1014 g/cm3 and xmax = 10. These are the parameters that have been fitted, along with the highest relative error, referred to as “RE”. The unit of p0 is dyne × cm−2.
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