<table><caption>**Table A.3.** SN<sub>Ia</sub> yield models used in this work via the `abunfit` package (continues on next pages, see below for references).</caption><thead><tr><th>Category</th><th>Name</th><th>Ref.</th><th>Remarks</th></tr></thead><tbody><tr><td colspan="4" style="text-align:center; font-weight:bold;">SN<sub>Ia</sub></td></tr><tr><td colspan="4" style="text-align:center; font-weight:bold;">Input</td></tr><tr><td colspan="4" style="text-align:center; font-weight:bold;">Th03</td></tr><tr><td rowspan="6">Bravo</td><td>DDTa</td><td>2</td><td>1D delayed-detonation, fits the Tycho SNR, ρ<sub>T,7</sub> = 3.9</td></tr><tr><td>DDTb</td><td>2</td><td>(priv. comm., does not fit Tycho SNR, unpublished)</td></tr><tr><td>DDTc</td><td>2</td><td>1D delayed-detonation, fits the Tycho SNR, ρ<sub>T,7</sub> = 2.2</td></tr><tr><td>DDTd</td><td>2</td><td>(priv. comm., does not fit Tycho SNR, unpublished)</td></tr><tr><td>DDTe</td><td>2</td><td>1D delayed-detonation, fits the Tycho SNR, ρ<sub>T,7</sub> = 1.3</td></tr><tr><td>DDTf</td><td>2</td><td>(priv. comm., does not fit Tycho SNR, unpublished)</td></tr><tr><td rowspan="8">Ca-rich gap</td><td>CO.45HE.2</td><td>3</td><td>Ca-rich SNe, M<sub>CO</sub> = 0.45, M<sub>He</sub> = 0.2</td></tr><tr><td>CO.55HE.2</td><td>3</td><td>Ca-rich SNe, M<sub>CO</sub> = 0.55, M<sub>He</sub> = 0.2</td></tr><tr><td>CO.5HE.15</td><td>3</td><td>Ca-rich SNe, M<sub>CO</sub> = 0.50, M<sub>He</sub> = 0.15</td></tr><tr><td>CO.5HE.2</td><td>3</td><td>Ca-rich SNe, M<sub>CO</sub> = 0.50, M<sub>He</sub> = 0.2</td></tr><tr><td>CO.5HE.2C.3</td><td>3</td><td>Ca-rich SNe, M<sub>CO</sub> = 0.50, M<sub>He</sub> = 0.2, 30% mixing He-core layer</td></tr><tr><td>CO.5HE.2N.02</td><td>3</td><td>Ca-rich SNe, M<sub>CO</sub> = 0.50, M<sub>He</sub> = 0.2, 2% N in He layer</td></tr><tr><td>CO.5HE.3</td><td>3</td><td>Ca-rich SNe, M<sub>CO</sub> = 0.50, M<sub>He</sub> = 0.3</td></tr><tr><td>CO.6HE.2</td><td>3</td><td>Ca-rich SNe, M<sub>CO</sub> = 0.60, M<sub>He</sub> = 0.2</td></tr><tr><td rowspan="3">2D</td><td>C-DEF</td><td>4</td><td>2D deflagration ρ<sub>9</sub> = 2.9</td></tr><tr><td>C-DDT</td><td>4</td><td>2D delayed-detonation ρ<sub>9</sub> = 2.9, ρ<sub>T,7</sub> = 1.0</td></tr><tr><td>O-DDT</td><td>4</td><td>2D delayed-detonation ρ<sub>9</sub> = 2.9, ρ<sub>T,7</sub> = 1.0, off-center ignition</td></tr><tr><td rowspan="14">3D</td><td>N1def</td><td>5</td><td>3D deflagration ρ<sub>9</sub> = 2.9, 1 ignition spot</td></tr><tr><td>N3def</td><td>5</td><td>3D deflagration ρ<sub>9</sub> = 2.9, 3 ignition spots</td></tr><tr><td>N5def</td><td>5</td><td>3D deflagration ρ<sub>9</sub> = 2.9, 5 ignition spots</td></tr><tr><td>N10def</td><td>5</td><td>3D deflagration ρ<sub>9</sub> = 2.9, 10 ignition spots</td></tr><tr><td>N20def</td><td>5</td><td>3D deflagration ρ<sub>9</sub> = 2.9, 20 ignition spots</td></tr><tr><td>N40def</td><td>5</td><td>3D deflagration ρ<sub>9</sub> = 2.9, 40 ignition spots</td></tr><tr><td>N100Hdef</td><td>5</td><td>3D deflagration ρ<sub>9</sub> = 1.0, 100 ignition spots</td></tr><tr><td>N100def</td><td>5</td><td>3D deflagration ρ<sub>9</sub> = 2.9, 100 ignition spots</td></tr><tr><td>N100Ldef</td><td>5</td><td>3D deflagration ρ<sub>9</sub> = 5.5, 100 ignition spots</td></tr><tr><td>N150def</td><td>5</td><td>3D deflagration ρ<sub>9</sub> = 2.9, 150 ignition spots</td></tr><tr><td>N200def</td><td>5</td><td>3D deflagration ρ<sub>9</sub> = 2.9, 200 ignition spots</td></tr><tr><td>N300Cdef</td><td>5</td><td>3D deflagration ρ<sub>9</sub> = 2.9, 300 centred ignition spots</td></tr><tr><td>N1600def</td><td>5</td><td>3D deflagration ρ<sub>9</sub> = 2.9, 1600 ignition spots</td></tr><tr><td>N1600Cdef</td><td>5</td><td>3D deflagration ρ<sub>9</sub> = 2.9, 1600 centred ignition spots</td></tr><tr><td rowspan="12">3D</td><td>N1</td><td>6</td><td>3D delayed-detonation ρ<sub>9</sub> = 2.9, 1 ignition spot</td></tr><tr><td>N3</td><td>6</td><td>3D delayed-detonation ρ<sub>9</sub> = 2.9, 3 ignition spots</td></tr><tr><td>N5</td><td>6</td><td>3D delayed-detonation ρ<sub>9</sub> = 2.9, 5 ignition spots</td></tr><tr><td>N10</td><td>6</td><td>3D delayed-detonation ρ<sub>9</sub> = 2.9, 10 ignition spots</td></tr><tr><td>N20</td><td>6</td><td>3D delayed-detonation ρ<sub>9</sub> = 2.9, 20 ignition spots</td></tr><tr><td>N40</td><td>6</td><td>3D delayed-detonation ρ<sub>9</sub> = 2.9, 40 ignition spots</td></tr><tr><td>N100H</td><td>6</td><td>3D delayed-detonation ρ<sub>9</sub> = 1.0, 100 ignition spots</td></tr><tr><td>N100</td><td>6</td><td>3D delayed-detonation ρ<sub>9</sub> = 2.9, 100 ignition spots</td></tr><tr><td>N100L</td><td>6</td><td>3D delayed-detonation ρ<sub>9</sub> = 5.5, 100 ignition spots</td></tr><tr><td>N150</td><td>6</td><td>3D delayed-detonation ρ<sub>9</sub> = 2.9, 150 ignition spots</td></tr><tr><td>N200</td><td>6</td><td>3D delayed-detonation ρ<sub>9</sub> = 2.9, 200 ignition spots</td></tr><tr><td>N300C</td><td>6</td><td>3D delayed-detonation ρ<sub>9</sub> = 2.9, 300 centred ignition spots</td></tr></tbody></table>

**Notes.** The model used in our input cosmological simulations is given in bold.

**References.** SN<sub>Ia</sub>: (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). SN<sub>cc</sub>: (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).
<table><caption>**Table A.3.** continued.</caption><thead><tr><th>Category</th><th>Name</th><th>Ref.</th><th>Remarks</th></tr></thead><tbody><tr><td rowspan="12">3D</td><td>N1600</td><td>6</td><td>3D delayed-detonation ρ<sub>9</sub> = 2.9, 1600 ignition spots</td></tr><tr><td>N1600C</td><td>6</td><td>3D delayed-detonation ρ<sub>9</sub> = 2.9, 1600 centred ignition spots</td></tr><tr><td>N100_Z0.5</td><td>6</td><td>3D delayed-detonation ρ<sub>9</sub> = 2.9, 100 ignition spots, Z<sub>init</sub> = 0.5 Z<sub>☉</sub></td></tr><tr><td>N100_Z0.1</td><td>6</td><td>3D delayed-detonation ρ<sub>9</sub> = 2.9, 100 ignition spots, Z<sub>init</sub> = 0.1 Z<sub>☉</sub></td></tr><tr><td>N100_Z0.01</td><td>6</td><td>3D delayed-detonation ρ<sub>9</sub> = 2.9, 100 ignition spots, Z<sub>init</sub> = 0.01 Z<sub>☉</sub></td></tr><tr><td>N100_c50</td><td>7</td><td>N100 with WD homogeneous core with 50% C (mass)</td></tr><tr><td>N100_rpc20</td><td>7</td><td>N100 with WD C-depleted core with 20% C (mass)</td></tr><tr><td>N100_rpc32</td><td>7</td><td>N100 with WD C-depleted core with 32% C (mass)</td></tr><tr><td>N100_rpc40</td><td>7</td><td>N100 with WD C-depleted core with 40% C (mass)</td></tr><tr><td rowspan="23">LN18</td><td>050-1-c3-1P</td><td>12</td><td>2D deflagr., ρ<sub>9</sub> = 0.5, centred ignition, Z<sub>init</sub> = 1 Z<sub>☉</sub></td></tr><tr><td>100-1-c3-1P</td><td>12</td><td>2D deflagr., ρ<sub>9</sub> = 1.0, centred ignition, Z<sub>init</sub> = 1 Z<sub>☉</sub></td></tr><tr><td>100-0-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 1.0, centred ignition, Z<sub>init</sub> = 0 Z<sub>☉</sub></td></tr><tr><td>100-0.1-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 1.0, centred ignition, Z<sub>init</sub> = 0.1 Z<sub>☉</sub></td></tr><tr><td>100-0.5-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 1.0, centred ignition, Z<sub>init</sub> = 0.5 Z<sub>☉</sub></td></tr><tr><td>100-1-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 1.0, centred ignition, Z<sub>init</sub> = 1 Z<sub>☉</sub></td></tr><tr><td>100-2-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 1.0, centred ignition, Z<sub>init</sub> = 2 Z<sub>☉</sub></td></tr><tr><td>100-3-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 1.0, centred ignition, Z<sub>init</sub> = 3 Z<sub>☉</sub></td></tr><tr><td>100-5-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 1.0, centred ignition, Z<sub>init</sub> = 5 Z<sub>☉</sub></td></tr><tr><td>300-1-c3-1P</td><td>12</td><td>2D deflagr., ρ<sub>9</sub> = 3.0, centred ignition, Z<sub>init</sub> = 1 Z<sub>☉</sub></td></tr><tr><td>300-0-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 3.0, centred ignition, Z<sub>init</sub> = 0 Z<sub>☉</sub></td></tr><tr><td>300-0.1-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 3.0, centred ignition, Z<sub>init</sub> = 0.1 Z<sub>☉</sub></td></tr><tr><td>300-0.5-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 3.0, centred ignition, Z<sub>init</sub> = 0.5 Z<sub>☉</sub></td></tr><tr><td>300-1-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 3.0, centred ignition, Z<sub>init</sub> = 1 Z<sub>☉</sub></td></tr><tr><td>300-2-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 3.0, centred ignition, Z<sub>init</sub> = 2 Z<sub>☉</sub></td></tr><tr><td>300-3-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 3.0, centred ignition, Z<sub>init</sub> = 3 Z<sub>☉</sub></td></tr><tr><td>300-5-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 3.0, centred ignition, Z<sub>init</sub> = 5 Z<sub>☉</sub></td></tr><tr><td>500-1-c3-1P</td><td>12</td><td>2D deflagr., ρ<sub>9</sub> = 5.0, centred ignition, Z<sub>init</sub> = 1 Z<sub>☉</sub></td></tr><tr><td>500-0-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 5.0, centred ignition, Z<sub>init</sub> = 0 Z<sub>☉</sub></td></tr><tr><td>500-0.1-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 5.0, centred ignition, Z<sub>init</sub> = 0.1 Z<sub>☉</sub></td></tr><tr><td>500-0.5-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 5.0, centred ignition, Z<sub>init</sub> = 0.5 Z<sub>☉</sub></td></tr><tr><td>500-1-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 5.0, centred ignition, Z<sub>init</sub> = 1 Z<sub>☉</sub></td></tr><tr><td>500-2-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 5.0, centred ignition, Z<sub>init</sub> = 2 Z<sub>☉</sub></td></tr><tr><td>500-3-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 5.0, centred ignition, Z<sub>init</sub> = 3 Z<sub>☉</sub></td></tr><tr><td>500-5-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 5.0, centred ignition, Z<sub>init</sub> = 5 Z<sub>☉</sub></td></tr><tr><td>HWD</td><td>N5_hy</td><td>8</td><td>Hybrid WD (CO and ONe layers)</td></tr><tr><td>GCD</td><td>GCD200</td><td>9</td><td>Gravity-confined detonation</td></tr><tr><td rowspan="7">DbleDet</td><td>CSDD-L</td><td>10</td><td>2D converging-shock double-deton., M<sub>CO</sub> = 0.45 M<sub>☉</sub></td></tr><tr><td>CSDD-S</td><td>10</td><td>2D converging-shock double-deton., M<sub>CO</sub> = 0.58 M<sub>☉</sub></td></tr><tr><td>ELDD-L</td><td>10</td><td>2D edge-lit double-detonation, M<sub>CO</sub> = 0.45 M<sub>☉</sub></td></tr><tr><td>ELDD-S</td><td>10</td><td>2D edge-lit double-detonation, M<sub>CO</sub> = 0.58 M<sub>☉</sub></td></tr><tr><td>HeD-L</td><td>10</td><td>2D He detonation only, M<sub>CO</sub> = 0.45 M<sub>☉</sub></td></tr><tr><td>HeD-S</td><td>10</td><td>2D He detonation only, M<sub>CO</sub> = 0.58 M<sub>☉</sub></td></tr></tbody></table>
<table><caption>**Table A.3.** continued.</caption><thead><tr><th>Category</th><th>Name</th><th>Ref.</th><th>Remarks</th></tr></thead><tbody><tr><td rowspan="10">3D</td><td>N1600</td><td>6</td><td>3D delayed-detonation ρ<sub>9</sub> = 2.9, 1600 ignition spots</td></tr><tr><td>N1600C</td><td>6</td><td>3D delayed-detonation ρ<sub>9</sub> = 2.9, 1600 centred ignition spots</td></tr><tr><td>N100_Z0.5</td><td>6</td><td>3D delayed-detonation ρ<sub>9</sub> = 2.9, 100 ignition spots, Z<sub>init</sub> = 0.5 Z<sub>☉</sub></td></tr><tr><td>N100_Z0.1</td><td>6</td><td>3D delayed-detonation ρ<sub>9</sub> = 2.9, 100 ignition spots, Z<sub>init</sub> = 0.1 Z<sub>☉</sub></td></tr><tr><td>N100_Z0.01</td><td>6</td><td>3D delayed-detonation ρ<sub>9</sub> = 2.9, 100 ignition spots, Z<sub>init</sub> = 0.01 Z<sub>☉</sub></td></tr><tr><td>N100_c50</td><td>7</td><td>N100 with WD homogeneous core with 50% C (mass)</td></tr><tr><td>N100_rpc20</td><td>7</td><td>N100 with WD C-depleted core with 20% C (mass)</td></tr><tr><td>N100_rpc32</td><td>7</td><td>N100 with WD C-depleted core with 32% C (mass)</td></tr><tr><td>N100_rpc40</td><td>7</td><td>N100 with WD C-depleted core with 40% C (mass)</td></tr><tr><td rowspan="20">LN18</td><td>050-1-c3-1P</td><td>12</td><td>2D deflagr., ρ<sub>9</sub> = 0.5, centred ignition, Z<sub>init</sub> = 1 Z<sub>☉</sub></td></tr><tr><td>100-1-c3-1P</td><td>12</td><td>2D deflagr., ρ<sub>9</sub> = 1.0, centred ignition, Z<sub>init</sub> = 1 Z<sub>☉</sub></td></tr><tr><td>100-0-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 1.0, centred ignition, Z<sub>init</sub> = 0 Z<sub>☉</sub></td></tr><tr><td>100-0.1-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 1.0, centred ignition, Z<sub>init</sub> = 0.1 Z<sub>☉</sub></td></tr><tr><td>100-0.5-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 1.0, centred ignition, Z<sub>init</sub> = 0.5 Z<sub>☉</sub></td></tr><tr><td>100-1-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 1.0, centred ignition, Z<sub>init</sub> = 1 Z<sub>☉</sub></td></tr><tr><td>100-2-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 1.0, centred ignition, Z<sub>init</sub> = 2 Z<sub>☉</sub></td></tr><tr><td>100-3-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 1.0, centred ignition, Z<sub>init</sub> = 3 Z<sub>☉</sub></td></tr><tr><td>100-5-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 1.0, centred ignition, Z<sub>init</sub> = 5 Z<sub>☉</sub></td></tr><tr><td>300-1-c3-1P</td><td>12</td><td>2D deflagr., ρ<sub>9</sub> = 3.0, centred ignition, Z<sub>init</sub> = 1 Z<sub>☉</sub></td></tr><tr><td>300-0-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 3.0, centred ignition, Z<sub>init</sub> = 0 Z<sub>☉</sub></td></tr><tr><td>300-0.1-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 3.0, centred ignition, Z<sub>init</sub> = 0.1 Z<sub>☉</sub></td></tr><tr><td>300-0.5-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 3.0, centred ignition, Z<sub>init</sub> = 0.5 Z<sub>☉</sub></td></tr><tr><td>300-1-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 3.0, centred ignition, Z<sub>init</sub> = 1 Z<sub>☉</sub></td></tr><tr><td>300-2-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 3.0, centred ignition, Z<sub>init</sub> = 2 Z<sub>☉</sub></td></tr><tr><td>300-3-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 3.0, centred ignition, Z<sub>init</sub> = 3 Z<sub>☉</sub></td></tr><tr><td>300-5-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 3.0, centred ignition, Z<sub>init</sub> = 5 Z<sub>☉</sub></td></tr><tr><td>500-1-c3-1P</td><td>12</td><td>2D deflagr., ρ<sub>9</sub> = 5.0, centred ignition, Z<sub>init</sub> = 1 Z<sub>☉</sub></td></tr><tr><td>500-0-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 5.0, centred ignition, Z<sub>init</sub> = 0 Z<sub>☉</sub></td></tr><tr><td>500-0.1-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 5.0, centred ignition, Z<sub>init</sub> = 0.1 Z<sub>☉</sub></td></tr><tr><td>500-0.5-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 5.0, centred ignition, Z<sub>init</sub> = 0.5 Z<sub>☉</sub></td></tr><tr><td>500-1-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 5.0, centred ignition, Z<sub>init</sub> = 1 Z<sub>☉</sub></td></tr><tr><td>500-2-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 5.0, centred ignition, Z<sub>init</sub> = 2 Z<sub>☉</sub></td></tr><tr><td>500-3-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 5.0, centred ignition, Z<sub>init</sub> = 3 Z<sub>☉</sub></td></tr><tr><td>500-5-c3</td><td>12</td><td>2D del.-det., ρ<sub>9</sub> = 5.0, centred ignition, Z<sub>init</sub> = 5 Z<sub>☉</sub></td></tr><tr><td>HWD</td><td>N5_hy</td><td>8</td><td>Hybrid WD (CO and ONe layers)</td></tr><tr><td>GCD</td><td>GCD200</td><td>9</td><td>Gravity-confined detonation</td></tr><tr><td rowspan="7">DbleDet</td><td>CSDD-L</td><td>10</td><td>2D converging-shock double-deton., M<sub>CO</sub> = 0.45 M<sub>☉</sub></td></tr><tr><td>CSDD-S</td><td>10</td><td>2D converging-shock double-deton., M<sub>CO</sub> = 0.58 M<sub>☉</sub></td></tr><tr><td>ELDD-L</td><td>10</td><td>2D edge-lit double-detonation, M<sub>CO</sub> = 0.45 M<sub>☉</sub></td></tr><tr><td>ELDD-S</td><td>10</td><td>2D edge-lit double-detonation, M<sub>CO</sub> = 0.58 M<sub>☉</sub></td></tr><tr><td>HeD-L</td><td>10</td><td>2D He detonation only, M<sub>CO</sub> = 0.45 M<sub>☉</sub></td></tr><tr><td>HeD-S</td><td>10</td><td>2D He detonation only, M<sub>CO</sub> = 0.58 M<sub>☉</sub></td></tr></tbody></table>
<table><caption>**Table A.3.** continued.</caption><thead><tr><th>Category</th><th>Name</th><th>Ref.</th><th>Remarks</th></tr></thead><tbody><tr><td rowspan="7">ONe</td><td>CO15e7</td><td>11</td><td>2D (sub-M<sub>Ch</sub>) detonation carbon-oxygen WD, ρ<sub>9</sub> = 0.15</td></tr><tr><td>ONe10e7</td><td>11</td><td>2D (sub-M<sub>Ch</sub>) detonation oxygen-neon WD, ρ<sub>9</sub> = 0.10</td></tr><tr><td>ONe13e7</td><td>11</td><td>2D (sub-M<sub>Ch</sub>) detonation oxygen-neon WD, ρ<sub>9</sub> = 0.13</td></tr><tr><td>ONe15e7</td><td>11</td><td>2D (sub-M<sub>Ch</sub>) detonation oxygen-neon WD, ρ<sub>9</sub> = 0.15</td></tr><tr><td>ONe17e7</td><td>11</td><td>2D (sub-M<sub>Ch</sub>) detonation oxygen-neon WD, ρ<sub>9</sub> = 0.17</td></tr><tr><td>ONe20e7</td><td>11</td><td>2D (sub-M<sub>Ch</sub>) detonation oxygen-neon WD, ρ<sub>9</sub> = 0.20</td></tr><tr><td rowspan="6">Det</td><td>det_0.81</td><td>13</td><td>1D (sub-M<sub>Ch</sub>) pure detonation, M<sub>CO</sub> = 0.81 M<sub>☉</sub>, ρ<sub>7</sub> = 1.0</td></tr><tr><td>det_0.88</td><td>13</td><td>1D (sub-M<sub>Ch</sub>) pure detonation, M<sub>CO</sub> = 0.88 M<sub>☉</sub>, ρ<sub>7</sub> = 1.45</td></tr><tr><td>det_0.97</td><td>13</td><td>1D (sub-M<sub>Ch</sub>) pure detonation, M<sub>CO</sub> = 0.97 M<sub>☉</sub>, ρ<sub>7</sub> = 2.4</td></tr><tr><td>det_1.06</td><td>13</td><td>1D (sub-M<sub>Ch</sub>) pure detonation, M<sub>CO</sub> = 1.06 M<sub>☉</sub>, ρ<sub>7</sub> = 4.15</td></tr><tr><td>det_1.15</td><td>13</td><td>1D (sub-M<sub>Ch</sub>) pure detonation, M<sub>CO</sub> = 1.15 M<sub>☉</sub>, ρ<sub>7</sub> = 7.9</td></tr><tr><td>det_1.06_0.075Ne</td><td>13</td><td>1D (sub-M<sub>Ch</sub>) pure detonation, M<sub>CO</sub> = 1.06 M<sub>☉</sub>, ρ<sub>7</sub> = 4.15, C/O/Ne mass fraction = 0.425/0.5/0.075</td></tr><tr><td>6D</td><td>Sh18_Ma_b_Zc_d</td><td>14</td><td>3D (sub-M<sub>Ch</sub>) 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<sub>☉</sub>), C/O compositions (b ∈ {30/70, 50/50}), metallicity Z<sub>init</sub> (Zc ∈ {0, 0.005, 0.01, 0.02}), and normalizations of the <sup>12</sup>C+<sup>16</sup>O reaction rate (d ∈ {0.1, 1.0})</td></tr><tr><td rowspan="2">Merger</td><td>09_09</td><td>15</td><td>3D (sub-M<sub>Ch</sub>) violent WD merger (double-degen.), 0.9+0.9 M<sub>☉</sub></td></tr><tr><td>11_09</td><td>16</td><td>3D (sub-M<sub>Ch</sub>) violent WD merger (double-degen.), 1.1+0.9 M<sub>☉</sub></td></tr><tr><td rowspan="2">Merger2</td><td>09_076</td><td>17</td><td>3D (sub-M<sub>Ch</sub>) violent WD merger (double-degen.), 0.9+0.76 M<sub>☉</sub>, Z<sub>init</sub> = 1 Z<sub>☉</sub></td></tr><tr><td>09_076_Z0.01</td><td>17</td><td>3D (sub-M<sub>Ch</sub>) violent WD merger (double-degen.), 0.9+0.76 M<sub>☉</sub>, Z<sub>init</sub> = 0.01 Z<sub>☉</sub></td></tr></tbody></table>
<table><caption>**Table A.3.** continued.</caption><thead><tr><th>Category</th><th>Name</th><th>Ref.</th><th>Remarks</th></tr></thead><tbody><tr><td rowspan="6">ONe</td><td>CO15e7</td><td>11</td><td>2D (sub-M<sub>Ch</sub>) detonation carbon-oxygen WD, ρ<sub>9</sub> = 0.15</td></tr><tr><td>ONe10e7</td><td>11</td><td>2D (sub-M<sub>Ch</sub>) detonation oxygen-neon WD, ρ<sub>9</sub> = 0.10</td></tr><tr><td>ONe13e7</td><td>11</td><td>2D (sub-M<sub>Ch</sub>) detonation oxygen-neon WD, ρ<sub>9</sub> = 0.13</td></tr><tr><td>ONe15e7</td><td>11</td><td>2D (sub-M<sub>Ch</sub>) detonation oxygen-neon WD, ρ<sub>9</sub> = 0.15</td></tr><tr><td>ONe17e7</td><td>11</td><td>2D (sub-M<sub>Ch</sub>) detonation oxygen-neon WD, ρ<sub>9</sub> = 0.17</td></tr><tr><td>ONe20e7</td><td>11</td><td>2D (sub-M<sub>Ch</sub>) detonation oxygen-neon WD, ρ<sub>9</sub> = 0.20</td></tr><tr><td rowspan="6">Det</td><td>det_0.81</td><td>13</td><td>1D (sub-M<sub>Ch</sub>) pure detonation, M<sub>CO</sub> = 0.81 M<sub>☉</sub>, ρ<sub>7</sub> = 1.0</td></tr><tr><td>det_0.88</td><td>13</td><td>1D (sub-M<sub>Ch</sub>) pure detonation, M<sub>CO</sub> = 0.88 M<sub>☉</sub>, ρ<sub>7</sub> = 1.45</td></tr><tr><td>det_0.97</td><td>13</td><td>1D (sub-M<sub>Ch</sub>) pure detonation, M<sub>CO</sub> = 0.97 M<sub>☉</sub>, ρ<sub>7</sub> = 2.4</td></tr><tr><td>det_1.06</td><td>13</td><td>1D (sub-M<sub>Ch</sub>) pure detonation, M<sub>CO</sub> = 1.06 M<sub>☉</sub>, ρ<sub>7</sub> = 4.15</td></tr><tr><td>det_1.15</td><td>13</td><td>1D (sub-M<sub>Ch</sub>) pure detonation, M<sub>CO</sub> = 1.15 M<sub>☉</sub>, ρ<sub>7</sub> = 7.9</td></tr><tr><td>det_1.06_0.075Ne</td><td>13</td><td>1D (sub-M<sub>Ch</sub>) pure detonation, M<sub>CO</sub> = 1.06 M<sub>☉</sub>, ρ<sub>7</sub> = 4.15, C/O/Ne mass fraction = 0.425/0.5/0.075</td></tr><tr><td>6D</td><td>Sh18_Ma_b_Zc_d</td><td>14</td><td>3D (sub-M<sub>Ch</sub>) 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<sub>☉</sub>), C/O compositions (b ∈ {30/70, 50/50}), metallicity Z<sub>init</sub> (Zc ∈ {0, 0.005, 0.01, 0.02}), and normalizations of the <sup>12</sup>C+<sup>16</sup>O reaction rate (d ∈ {0.1, 1.0})</td></tr><tr><td rowspan="2">Merger</td><td>09_09</td><td>15</td><td>3D (sub-M<sub>Ch</sub>) violent WD merger (double-degen.), 0.9+0.9 M<sub>☉</sub></td></tr><tr><td>11_09</td><td>16</td><td>3D (sub-M<sub>Ch</sub>) violent WD merger (double-degen.), 1.1+0.9 M<sub>☉</sub></td></tr><tr><td rowspan="2">Merger2</td><td>09_076</td><td>17</td><td>3D (sub-M<sub>Ch</sub>) violent WD merger (double-degen.), 0.9+0.76 M<sub>☉</sub>, Z<sub>init</sub> = 1 Z<sub>☉</sub></td></tr><tr><td>09_076_Z0.01</td><td>17</td><td>3D (sub-M<sub>Ch</sub>) violent WD merger (double-degen.), 0.9+0.76 M<sub>☉</sub>, Z<sub>init</sub> = 0.01 Z<sub>☉</sub></td></tr></tbody></table>