Table 4.
Summary of the strongest, volume-integrated cooling powers compared to the injected magnetar power for model he12p00 at 2200 d.
| Process | Power [erg s−1] | [%] | |
|---|---|---|---|
| Magnetar | 1.00(39) | 96.91 | |
| Art. HT | 3.19(37) | 3.09 | |
| Ne II | COL | 5.71(38) | 55.30 |
| O II | NT | 6.42(37) | 6.22 |
| O II | COL | 5.60(37) | 5.42 |
| O I | NT | 5.48(37) | 5.31 |
| Fe II | COL | 4.98(37) | 4.82 |
| Ar II | COL | 4.85(37) | 4.70 |
| Ni II | COL | 4.53(37) | 4.39 |
| O I | COL | 4.12(37) | 3.99 |
| O III | COL | 3.01(37) | 2.91 |
| Si II | COL | 1.76(37) | 1.71 |
| C II | COL | 1.67(37) | 1.62 |
| Fe III | COL | 1.61(37) | 1.56 |
| Fe I | COL | 8.73(36) | 0.85 |
| He I | NT | 5.65(36) | 0.55 |
| Si II | NT | 4.27(36) | 0.41 |
| S I | COL | 3.52(36) | 0.34 |
| Ni I | COL | 2.33(36) | 0.23 |
Notes. The list is ordered from the strongest to the weakest power out of the 17 top cooling powers ejecta-wide. The first two columns lists all cooling processes (“COL” for collisional excitation and “NT” for nonthermal excitation) balancing the heating from the magnetar power injected. The term “Art. HT” corresponds to an artificial heating component introduced to prevent the temperature from dropping below a floor temperature of 1000 K (this occurs at sporadic locations). The third column gives the corresponding power in erg s−1. The last column gives that quantity as the percentage fraction of the total cooling power. Numbers in parenthesis correspond to powers of ten.
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