Open Access
Table A.3.
SNIa yield models used in this work via the abunfit package (continues on next pages, see below for references).
| Category | Name | Ref. | Remarks |
|---|---|---|---|
| SNIa | |||
| Input | Th03 | 1 | 1D deflagration |
| Bravo | DDTa | 2 | 1D delayed-detonation, fits the Tycho SNR, ρT, 7 = 3.9 |
| DDTb | 2 | (priv. comm., does not fit Tycho SNR, unpublished) | |
| DDTc | 2 | 1D delayed-detonation, fits the Tycho SNR, ρT, 7 = 2.2 | |
| DDTd | 2 | (priv. comm., does not fit Tycho SNR, unpublished) | |
| DDTe | 2 | 1D delayed-detonation, fits the Tycho SNR, ρT, 7 = 1.3 | |
| DDTf | 2 | (priv. comm., does not fit Tycho SNR, unpublished) | |
| Ca-rich gap | CO.45HE.2 | 3 | Ca-rich SNe, MCO = 0.45, MHe = 0.2 |
| CO.55HE.2 | 3 | Ca-rich SNe, MCO = 0.55, MHe = 0.2 | |
| CO.5HE.15 | 3 | Ca-rich SNe, MCO = 0.50, MHe = 0.15 | |
| CO.5HE.2 | 3 | Ca-rich SNe, MCO = 0.50, MHe = 0.2 | |
| CO.5HE.2C.3 | 3 | Ca-rich SNe, MCO = 0.50, MHe = 0.2, 30% mixing He-core layer | |
| CO.5HE.2N.02 | 3 | Ca-rich SNe, MCO = 0.50, MHe = 0.2, 2% N in He layer | |
| CO.5HE.3 | 3 | Ca-rich SNe, MCO = 0.50, MHe = 0.3 | |
| CO.6HE.2 | 3 | Ca-rich SNe, MCO = 0.60, MHe = 0.2 | |
| 2D | C-DEF | 4 | 2D deflagration ρ9 = 2.9 |
| C-DDT | 4 | 2D delayed-detonation ρ9 = 2.9, ρT, 7 = 1.0 | |
| O-DDT | 4 | 2D delayed-detonation ρ9 = 2.9, ρT, 7 = 1.0, off-center ignition | |
| 3D | N1def | 5 | 3D deflagration ρ9 = 2.9, 1 ignition spot |
| N3def | 5 | 3D deflagration ρ9 = 2.9, 3 ignition spots | |
| N5def | 5 | 3D deflagration ρ9 = 2.9, 5 ignition spots | |
| N10def | 5 | 3D deflagration ρ9 = 2.9, 10 ignition spots | |
| N20def | 5 | 3D deflagration ρ9 = 2.9, 20 ignition spots | |
| N40def | 5 | 3D deflagration ρ9 = 2.9, 40 ignition spots | |
| N100Hdef | 5 | 3D deflagration ρ9 = 1.0, 100 ignition spots | |
| N100def | 5 | 3D deflagration ρ9 = 2.9, 100 ignition spots | |
| N100Ldef | 5 | 3D deflagration ρ9 = 5.5, 100 ignition spots | |
| N150def | 5 | 3D deflagration ρ9 = 2.9, 150 ignition spots | |
| N200def | 5 | 3D deflagration ρ9 = 2.9, 200 ignition spots | |
| N300Cdef | 5 | 3D deflagration ρ9 = 2.9, 300 centred ignition spots | |
| N1600def | 5 | 3D deflagration ρ9 = 2.9, 1600 ignition spots | |
| N1600Cdef | 5 | 3D deflagration ρ9 = 2.9, 1600 centred ignition spots | |
| 3D | N1 | 6 | 3D delayed-detonation ρ9 = 2.9, 1 ignition spot |
| N3 | 6 | 3D delayed-detonation ρ9 = 2.9, 3 ignition spots | |
| N5 | 6 | 3D delayed-detonation ρ9 = 2.9, 5 ignition spots | |
| N10 | 6 | 3D delayed-detonation ρ9 = 2.9, 10 ignition spots | |
| N20 | 6 | 3D delayed-detonation ρ9 = 2.9, 20 ignition spots | |
| N40 | 6 | 3D delayed-detonation ρ9 = 2.9, 40 ignition spots | |
| N100H | 6 | 3D delayed-detonation ρ9 = 1.0, 100 ignition spots | |
| N100 | 6 | 3D delayed-detonation ρ9 = 2.9, 100 ignition spots | |
| N100L | 6 | 3D delayed-detonation ρ9 = 5.5, 100 ignition spots | |
| N150 | 6 | 3D delayed-detonation ρ9 = 2.9, 150 ignition spots | |
| N200 | 6 | 3D delayed-detonation ρ9 = 2.9, 200 ignition spots | |
| N300C | 6 | 3D delayed-detonation ρ9 = 2.9, 300 centred ignition spots | |
| N1600 | 6 | 3D delayed-detonation ρ9 = 2.9, 1600 ignition spots | |
| N1600C | 6 | 3D delayed-detonation ρ9 = 2.9, 1600 centred ignition spots | |
| N100_Z0.5 | 6 | 3D delayed-detonation ρ9 = 2.9, 100 ignition spots, Zinit = 0.5 Z⊙ | |
| N100_Z0.1 | 6 | 3D delayed-detonation ρ9 = 2.9, 100 ignition spots, Zinit = 0.1 Z⊙ | |
| N100_Z0.01 | 6 | 3D delayed-detonation ρ9 = 2.9, 100 ignition spots, Zinit = 0.01 Z⊙ | |
| 3D | N100_c50 | 7 | N100 with WD homogeneous core with 50% C (mass) |
| N100_rpc20 | 7 | N100 with WD C-depleted core with 20% C (mass) | |
| N100_rpc32 | 7 | N100 with WD C-depleted core with 32% C (mass) | |
| N100_rpc40 | 7 | N100 with WD C-depleted core with 40% C (mass) | |
| LN18 | 050-1-c3-1P | 12 | 2D deflagr., ρ9 = 0.5, centred ignition, Zinit = 1 Z⊙ |
| 100-1-c3-1P | 12 | 2D deflagr., ρ9 = 1.0, centred ignit., Zinit = 1 Z⊙ | |
| 100-0-c3 | 12 | 2D del.-det., ρ9 = 1.0, centred ignit., Zinit = 0 Z⊙ | |
| 100-0.1-c3 | 12 | 2D del.-det., ρ9 = 1.0, centred ignit., Zinit = 0.1 Z⊙ | |
| 100-0.5-c3 | 12 | 2D del.-det., ρ9 = 1.0, centred ignit., Zinit = 0.5 Z⊙ | |
| 100-1-c3 | 12 | 2D del.-det., ρ9 = 1.0, centred ignit., Zinit = 1 Z⊙ | |
| 100-2-c3 | 12 | 2D del.-det., ρ9 = 1.0, centred ignit., Zinit = 2 Z⊙ | |
| 100-3-c3 | 12 | 2D del.-det., ρ9 = 1.0, centred ignit., Zinit = 3 Z⊙ | |
| 100-5-c3 | 12 | 2D del.-det., ρ9 = 1.0, centred ignit., Zinit = 5 Z⊙ | |
| 300-1-c3-1P | 12 | 2D deflagr., ρ9 = 3.0, centred ignit., Zinit = 1 Z⊙ | |
| 300-0-c3 | 12 | 2D del.-det., ρ9 = 3.0, centred ignit., Zinit = 0 Z⊙ | |
| 300-0.1-c3 | 12 | 2D del.-det., ρ9 = 3.0, centred ignit., Zinit = 0.1 Z⊙ | |
| 300-0.5-c3 | 12 | 2D del.-det., ρ9 = 3.0, centred ignit., Zinit = 0.5 Z⊙ | |
| 300-1-c3 | 12 | 2D del.-det., ρ9 = 3.0, centred ignit., Zinit = 1 Z⊙ | |
| 300-2-c3 | 12 | 2D del.-det., ρ9 = 3.0, centred ignit., Zinit = 2 Z⊙ | |
| 300-3-c3 | 12 | 2D del.-det., ρ9 = 3.0, centred ignit., Zinit = 3 Z⊙ | |
| 300-5-c3 | 12 | 2D del.-det., ρ9 = 3.0, centred ignit., Zinit = 5 Z⊙ | |
| 500-1-c3-1P | 12 | 2D deflagr., ρ9 = 5.0, centred ignit., Zinit = 1 Z⊙ | |
| 500-0-c3 | 12 | 2D del.-det., ρ9 = 5.0, centred ignit., Zinit = 0 Z⊙ | |
| 500-0.1-c3 | 12 | 2D del.-det., ρ9 = 5.0, centred ignit., Zinit = 0.1 Z⊙ | |
| 500-0.5-c3 | 12 | 2D del.-det., ρ9 = 5.0, centred ignit., Zinit = 0.5 Z⊙ | |
| 500-1-c3 | 12 | 2D del.-det., ρ9 = 5.0, centred ignit., Zinit = 1 Z⊙ | |
| 500-2-c3 | 12 | 2D del.-det., ρ9 = 5.0, centred ignit., Zinit = 2 Z⊙ | |
| 500-3-c3 | 12 | 2D del.-det., ρ9 = 5.0, centred ignit., Zinit = 3 Z⊙ | |
| 500-5-c3 | 12 | 2D del.-det., ρ9 = 5.0, centred ignit., Zinit = 5 Z⊙ | |
| HWD | N5_hy | 8 | Hybrid WD (CO and ONe layers) |
| GCD | GCD200 | 9 | Gravity-confined detonation |
| DbleDet | CSDD-L | 10 | 2D converging-shock double-deton., MCO = 0.45 M⊙ |
| CSDD-S | 10 | 2D converging-shock double-deton., MCO = 0.58 M⊙ | |
| ELDD-L | 10 | 2D edge-lit double-detonation, MCO = 0.45 M⊙ | |
| ELDD-S | 10 | 2D edge-lit double-detonation, MCO = 0.58 M⊙ | |
| HeD-L | 10 | 2D He detonation only, MCO = 0.45 M⊙ | |
| HeD-S | 10 | 2D He detonation only, MCO = 0.58 M⊙ | |
| ONe | CO15e7 | 11 | 2D (sub-MCh) detonation carbon-oxygen WD, ρ9 = 0.15 |
| ONe10e7 | 11 | 2D (sub-MCh) detonation oxygen-neon WD, ρ9 = 0.10 | |
| ONe13e7 | 11 | 2D (sub-MCh) detonation oxygen-neon WD, ρ9 = 0.13 | |
| ONe15e7 | 11 | 2D (sub-MCh) detonation oxygen-neon WD, ρ9 = 0.15 | |
| ONe17e7 | 11 | 2D (sub-MCh) detonation oxygen-neon WD, ρ9 = 0.17 | |
| ONe20e7 | 11 | 2D (sub-MCh) detonation oxygen-neon WD, ρ9 = 0.20 | |
| Det | det_0.81 | 13 | 1D (sub-MCh) pure detonation, MCO = 0.81 M⊙, ρ7 = 1.0 |
| det_0.88 | 13 | 1D (sub-MCh) pure detonation, MCO = 0.88 M⊙, ρ7 = 1.45 | |
| det_0.97 | 13 | 1D (sub-MCh) pure detonation, MCO = 0.97 M⊙, ρ7 = 2.4 | |
| det_1.06 | 13 | 1D (sub-MCh) pure detonation, MCO = 1.06 M⊙, ρ7 = 4.15 | |
| det_1.15 | 13 | 1D (sub-MCh) pure detonation, MCO = 1.15 M⊙, ρ7 = 7.9 | |
| det_1.06_0.075Ne | 13 | 1D (sub-MCh) pure detonation, MCO = 1.06 M⊙, ρ7 = 4.15, | |
| C/O/Ne mass fraction = 0.425/0.5/0.075 | |||
| 6D | Sh18_Ma_b_Zc_d | 14 | 3D (sub-MCh) dynamically-driven double-degenerate double detonation, 159 models in total for different WD masses (Ma ∈ {0.8, 0.85, 0.9, 1.0, 1.1} M⊙), C/O compositions (b ∈ {30/70, 50/50}), metallicity Zinit (Zc ∈ {0, 0.005, 0.01, 0.02}), and normalizations of the 12C+16O reaction rate (d ∈ {0.1, 1.0}) |
| Merger | 09_09 | 15 | 3D (sub-MCh) violent WD merger (double-degen.), 0.9+0.9 M⊙ |
| 11_09 | 16 | 3D (sub-MCh) violent WD merger (double-degen.), 1.1+0.9 M⊙ | |
| Merger2 | 09_076 | 17 | 3D (sub-MCh) violent WD merger (double-degen.), 0.9+0.76 M⊙, Zinit = 1 Z⊙ |
| 09_076_Z0.01 | 17 | 3D (sub-MCh) violent WD merger (double-degen.), 0.9+0.76 M⊙, Zinit = 0.01 Z⊙ | |
Notes. The model used in our input cosmological simulations is given in bold.
References. SNIa: (1) Thielemann et al. (2003); (2) Badenes et al. (2006); (3) Waldman et al. (2011); (4) Maeda et al. (2010); (5) Fink et al. (2014); (6) Seitenzahl et al. (2013b); (7) Ohlmann et al. (2014); (8) Kromer et al. (2015); (9) Seitenzahl et al. (2016); (10) Sim et al. (2012); (11) Marquardt et al. (2015); (12) Leung & Nomoto (2018); (13) Sim et al. (2010); (14) Shen et al. (2018); (15) Pakmor et al. (2010); (16) Pakmor et al. (2012); (17) Kromer et al. (2013). SNcc: (a) Romano et al. (2010); (b) Woosley & Weaver (1995); (c) Nomoto et al. (2013); (d) Heger & Woosley (2002); (e) Heger & Woosley (2010); (f) Sukhbold et al. (2016). AGB: (α) Karakas (2010).
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