Table 1.
Initial conditions for our radiation-hydrodynamics calculations.
Model name | Ṁ | RCSM | βw | V∞ | MCSM | τCSM | Rphot | CMFGEN |
---|---|---|---|---|---|---|---|---|
[M⊙ yr−1] | [1014 cm] | [km s−1] | [M⊙] | [1014 cm] | ||||
mdot0p01/rcsm2e14 | 0.01 | 2 | 2 | 50 | 0.0231 | 322.7 | 1.68 | Yes |
mdot0p01/rcsm4e14 | 0.01 | 4 | 2 | 50 | 0.0347 | 334.5 | 3.06 | Yes |
mdot0p01/rcsm6e14 | 0.01 | 6 | 2 | 50 | 0.0435 | 337.9 | 4.14 | Yes |
mdot0p01/rcsm8e14 | 0.01 | 8 | 2 | 50 | 0.0576 | 340.6 | 5.78 | Yes |
mdot0p01/rcsm1e15 | 0.01 | 10 | 2 | 50 | 0.0710 | 342.0 | 7.32 | Yes |
mdot0p001/rcsm8e14/bw2/vinf5e6 | 0.001 | 8 | 2 | 50 | 0.0249 | 447.0 | 3.19 | Yes |
mdot0p01/rcsm8e14/bw2/vinf5e6 | 0.01 | 8 | 2 | 50 | 0.1155 | 1313.8 | 5.53 | No |
mdot0p1/rcsm8e14/bw2/vinf5e6 | 0.1 | 8 | 2 | 50 | 0.7187 | 4424.5 | 6.39 | Yes |
mdot0p01/rcsm8e14/bw1/vinf5e6 | 0.01 | 8 | 1 | 50 | 0.0634 | 515.7 | 5.50 | No |
mdot0p01/rcsm8e14/bw2/vinf5e6 | 0.01 | 8 | 2 | 50 | 0.1155 | 1313.8 | 5.53 | No |
mdot0p01/rcsm8e14/bw4/vinf5e6 | 0.01 | 8 | 4 | 50 | 0.3063 | 3606.9 | 5.63 | No |
mdot0p01/rcsm8e14/bw2/vinf2e6 | 0.01 | 8 | 2 | 20 | 0.2332 | 2049.2 | 6.02 | Yes |
mdot0p01/rcsm8e14/bw2/vinf8e6 | 0.01 | 8 | 2 | 80 | 0.0813 | 1032.6 | 5.22 | No |
mdot0p01/rcsm8e14/bw2/vinf1p2e7 | 0.01 | 8 | 2 | 120 | 0.0612 | 855.5 | 4.90 | Yes |
Notes. Three groups of models are explored corresponding to variations in a RCSM, Ṁ, and wind velocity profile. All models correspond to the explosion of a 15 M⊙ star initially, evolved to core collapse at solar metallicity, and exploded to yield an ejecta with a kinetic energy of 1.2 × 1051 erg. The mass loss rate indicated in this table refers to the high-density CSM at the surface of the star, which drops rapidly to 10−6 M⊙ yr−1 beyond RCSM (see Fig. 1). The wind velocity profile is characterized by parameters βw and V∞, and an adjustable base velocity V0 to smoothly connect to the density at R⋆. The next three columns indicate the CSM mass, optical depth τCSM, and the corresponding photospheric radius. For τCSM, we integrate from R⋆ to infinity and adopt an opacity of 0.34 cm2 g−1. With this approach, the bulk of the optical depth arises from the denser, deeper regions near R⋆. The last column indicates whether the HERACLES simulation of the model was post-processed with CMFGEN. Model mdot0p01/rcsm8e14 is a close analog of model mdot0p01/rcsm8e14/bw2/vinf5e6, for which we therefore skipped the calculation with CMFGEN.
Current usage metrics show cumulative count of Article Views (full-text article views including HTML views, PDF and ePub downloads, according to the available data) and Abstracts Views on Vision4Press platform.
Data correspond to usage on the plateform after 2015. The current usage metrics is available 48-96 hours after online publication and is updated daily on week days.
Initial download of the metrics may take a while.