Table 2.
Parameter values calculated for the two NS models used in this study.
| Variable | Units | Model M | Model D |
|---|---|---|---|
| M | M⊙ | 1.44 | 1.76 |
| R | km | 11.5 | 11.8 |
| R∞ | km | 14.4 | 15.8 |
 |
erg s−1 K−q | 2.69 × 10−32 | 6.18 × 10−8 |
 |
erg s−1 K−q | 1.82 × 10−32 | 6.53 × 10−8 |
| Wnpe | 10−13 erg s2 | −1.70 | −1.84 |
| Wnpμ | 10−13 erg s2 | −2.22 | −2.14 |
| Znp | 10−61 erg | 3.04 | 2.70 |
| Znpe | 10−61 erg | 8.70 | 7.52 |
| Znpμ | 10−61 erg | 10.7 | 9.02 |
| Ke | 1047 s2 | 2.74 | 3.58 |
| Kμ | 1047 s2 | 3.34 | 3.69 |
| K | 1047 s2 | 6.09 | 7.27 |
Notes. Model M, with the equation of state A18+δv+UIX* (Akmal et al. 1998), allows only Murca reactions (for which the exponent q = 8), whereas Model D is based on the equation of state BPAL32 (Prakash et al. 1988) and allows Durca reactions (q = 6). The first three parameters in the list are the NS mass M, the coordinate radius R, and the redshifted radius R∞; the remaining parameters are defined by the equations of Sect. 4.1.
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