Table A.25.
Powers and magnitudes for our He-star explosion models computed with CMFGEN.
| Model | fabs | Lbol | LUVOIR | U | B | V | R | I | J | H | K |
|---|---|---|---|---|---|---|---|---|---|---|---|
| [1040 erg s−1] | [mag] | [mag] | [mag] | [mag] | [mag] | [mag] | [mag] | [mag] | |||
| he2p6 | 0.19 | 0.43 | 0.41 | -9.93 | -10.18 | -10.51 | -10.62 | -10.60 | -9.73 | -10.28 | -10.84 |
| he2p9 | 0.11 | 0.56 | 0.52 | -10.07 | -10.53 | -10.83 | -10.88 | -10.97 | -9.94 | -10.75 | -10.81 |
| he3p3 | 0.15 | 1.38 | 1.31 | -10.91 | -11.53 | -11.88 | -11.95 | -12.18 | -11.12 | -11.72 | -11.59 |
| he3p5 | 0.20 | 1.17 | 1.10 | -10.61 | -11.15 | -11.62 | -11.97 | -12.16 | -11.20 | -11.59 | -11.51 |
| he4p0 | 0.19 | 1.64 | 1.53 | -10.81 | -11.44 | -11.94 | -12.43 | -12.64 | -11.62 | -11.94 | -11.85 |
| he4p5 | 0.15 | 2.93 | 2.74 | -11.81 | -12.42 | -12.71 | -12.69 | -12.96 | -11.91 | -12.44 | -12.41 |
| he5p0 | 0.15 | 3.32 | 3.04 | -11.98 | -12.53 | -12.81 | -12.82 | -13.07 | -12.03 | -12.54 | -12.57 |
| he6p0 | 0.26 | 4.21 | 3.98 | -12.15 | -12.63 | -13.09 | -13.41 | -13.44 | -12.69 | -12.97 | -12.96 |
| he7p0 | 0.27 | 6.53 | 6.26 | -12.68 | -13.17 | -13.62 | -13.85 | -13.92 | -13.18 | -13.45 | -13.37 |
| he8p0 | 0.55 | 6.97 | 6.74 | -11.90 | -12.59 | -13.56 | -14.27 | -14.34 | -13.84 | -14.07 | -13.74 |
| he12p0 | 0.76 | 12.81 | 12.47 | -12.32 | -13.05 | -14.21 | -14.95 | -15.07 | -14.74 | -14.96 | -14.60 |
| he5p0x1p5 | 0.11 | 2.91 | 2.67 | -11.80 | -12.47 | -12.69 | -12.54 | -12.92 | -11.75 | -12.40 | -12.27 |
| he6p0x1p5 | 0.16 | 4.39 | 4.13 | -12.33 | -12.90 | -13.21 | -13.03 | -13.30 | -12.36 | -12.89 | -12.74 |
| he8p0x1p5 | 0.26 | 5.96 | 5.68 | -12.68 | -13.08 | -13.54 | -13.70 | -13.77 | -13.04 | -13.35 | -13.26 |
| he9p0x1p5 | 0.34 | 9.18 | 8.91 | -13.13 | -13.49 | -14.02 | -14.23 | -14.42 | -13.67 | -13.98 | -13.72 |
| he10p0x1p5 | 0.31 | 7.23 | 6.98 | -12.84 | -13.20 | -13.74 | -14.06 | -14.14 | -13.37 | -13.66 | -13.38 |
| he11p0x1p5 | 0.34 | 2.84 | 2.70 | -10.94 | -11.57 | -12.49 | -13.53 | -13.28 | -12.48 | -12.60 | -12.29 |
| he12p0x1p5 | 0.46 | 9.63 | 9.38 | -12.92 | -13.32 | -14.03 | -14.51 | -14.57 | -13.95 | -14.20 | -13.93 |
| he13p0x1p5 | 0.40 | 11.78 | 11.45 | -13.39 | -13.72 | -14.30 | -14.60 | -14.68 | -13.98 | -14.24 | -14.12 |
| he10p0x2p0 | 0.18 | 4.98 | 4.70 | -12.51 | -13.02 | -13.35 | -13.24 | -13.60 | -12.62 | -13.11 | -12.87 |
Notes: Fractional decay power absorbed, bolometric luminosity, UVOIR luminosity (accounts for the radiation falling between 1000 Å and 2.5 μm), and optical and NIR absolute magnitudes at 200 d for the explosion models he2p6 to he12p0 (standard mass loss rate; x1p0 series), he5p0x1p5 to he13p0x1p5 (50% enhancement in mass loss rate; x1p5 series), and model he10p0x2p0 (100% enhancement in mass loss rate; x2p0 series).
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