Chemical composition and enrichment of the Centaurus cluster core seen by XRISM/Resolve

Open Access

Table E.1.

SNIa and SNcc yield models, taken from literature and used in this work.

Category	Name	Reference	Description
SNIa, near-M_Ch
Iw99	W7	1	1D deflagration, ρ₉ = 2.12
Iw99	W70	1	1D deflagration, ρ₉ = 2.12, Z_init = 0
Ma10	C-DEF	2	2D deflagration, ρ₉ = 2.9
Fi14	N1def	3	3D deflagration, ρ₉ = 2.9, 1 ignition spot
Fi14	N3def	3	3D deflagration, ρ₉ = 2.9, 3 ignition spots
Fi14	N5def	3	3D deflagration, ρ₉ = 2.9, 5 ignition spots
Fi14	N10def	3	3D deflagration, ρ₉ = 2.9, 10 ignition spots
Fi14	N20def	3	3D deflagration, ρ₉ = 2.9, 20 ignition spots
Fi14	N40def	3	3D deflagration, ρ₉ = 2.9, 40 ignition spots
Fi14	N100Ldef	3	3D deflagration, ρ₉ = 1.0, 100 ignition spots
Fi14	N100def	3	3D deflagration, ρ₉ = 2.9, 100 ignition spots
Fi14	N100Hdef	3	3D deflagration, ρ₉ = 5.5, 100 ignition spots
Fi14	N150def	3	3D deflagration, ρ₉ = 2.9, 150 ignition spots
Fi14	N200def	3	3D deflagration, ρ₉ = 2.9, 200 ignition spots
Fi14	N300Cdef	3	3D deflagration, ρ₉ = 2.9, 300 centred ignition spots
Fi14	N1600def	3	3D deflagration, ρ₉ = 2.9, 1600 ignition spots
Fi14	N1600Cdef	3	3D deflagration, ρ₉ = 2.9, 1600 centred ignition spots
Le18	050-1-c3-P	4	2D deflagration, ρ₉ = 0.5, Z_init = 0.02
Le18	100-1-c3-P	4	2D deflagration, ρ₉ = 1.0, Z_init = 0.02
Le18	300-1-c3-P	4	2D deflagration, ρ₉ = 3.0, Z_init = 0.02
Le18	500-1-c3-P	4	2D deflagration, ρ₉ = 5.0, Z_init = 0.02
Le18	W7new	4	1D deflagration, W7 model (1) with updated electron capture and rates

Iw99	WDD1	1	1D delayed-detonation, ρ₉ = 2.12, ρ_T,7 = 1.7
Iw99	WDD2	1	1D delayed-detonation, ρ₉ = 2.12, ρ_T,7 = 2.2
Iw99	WDD3	1	1D delayed-detonation, ρ₉ = 2.12, ρ_T,7 = 3.0
Iw99	CDD1	1	1D delayed-detonation, ρ₉ = 1.37, ρ_T,7 = 1.7
Iw99	CDD2	1	1D delayed-detonation, ρ₉ = 1.37, ρ_T,7 = 2.2
Ba06	DDTa	5,6	1D delayed-detonation, fits the Tycho SNR, ρ_T,7 = 3.9
Ba06	DDTc	5,6	1D delayed-detonation, fits the Tycho SNR, ρ_T,7 = 2.2
Ba06	DDTe	5,6	1D delayed-detonation, fits the Tycho SNR, ρ_T,7 = 1.3
Ma10	C-DDT	2	2D delayed-detonation, ρ₉ = 2.9, ρ_T,7 = 1.0
Ma10	O-DDT	2	2D delayed-detonation, ρ₉ = 2.9, ρ_T,7 = 1.0, off-centre ignition
Se13	N1	7	3D delayed-detonation, ρ₉ = 2.9, 1 ignition spot
Se13	N3	7	3D delayed-detonation, ρ₉ = 2.9, 3 ignition spots
Se13	N5	7	3D delayed-detonation, ρ₉ = 2.9, 5 ignition spots
Se13	N10	7	3D delayed-detonation, ρ₉ = 2.9, 10 ignition spots
Se13	N20	7	3D delayed-detonation, ρ₉ = 2.9, 20 ignition spots
Se13	N40	7	3D delayed-detonation, ρ₉ = 2.9, 40 ignition spots
Se13	N100L	7	3D delayed-detonation, ρ₉ = 1.0, 100 ignition spots
Se13	N100	7	3D delayed-detonation, ρ₉ = 2.9, 100 ignition spots
Se13	N100H	7	3D delayed-detonation, ρ₉ = 5.5, 100 ignition spots
Se13	N150	7	3D delayed-detonation, ρ₉ = 2.9, 150 ignition spots
Se13	N200	7	3D delayed-detonation, ρ₉ = 2.9, 200 ignition spots
Se13	N300C	7	3D delayed-detonation, ρ₉ = 2.9, 300 centred ignition spots
Se13	N1600	7	3D delayed-detonation, ρ₉ = 2.9, 1600 ignition spots
Se13	N1600C	7	3D delayed-detonation, ρ₉ = 2.9, 1600 centred ignition spots
Oh14	N100_c50	8	3D delayed-detonation, N100 model (7), homogeneous with 50% C
Oh14	N100_rpc20	8	3D delayed-detonation, N100 model (7), depleted core with 20% C
Oh14	N100_rpc32	8	3D delayed-detonation, N100 model (7), depleted core with 32% C
Oh14	N100_rpc40	8	3D delayed-detonation, N100 model (7), depleted core with 40% C
Le18	100-0-c3	4	2D delayed-detonation, ρ₉ = 1.0, Z_init = 0
Le18	100-0.1-c3	4	2D delayed-detonation, ρ₉ = 1.0, Z_init = 0.002
Le18	100-0.5-c3	4	2D delayed-detonation, ρ₉ = 1.0, Z_init = 0.01
Le18	100-1-c3	4	2D delayed-detonation, ρ₉ = 1.0, Z_init = 0.02
Le18	100-2-c3	4	2D delayed-detonation, ρ₉ = 1.0, Z_init = 0.04
Le18	100-3-c3	4	2D delayed-detonation, ρ₉ = 1.0, Z_init = 0.06
Le18	100-5-c3	4	2D delayed-detonation, ρ₉ = 1.0, Z_init = 0.1
Le18	100-1-c3	4	2D delayed-detonation, ρ₉ = 1.0, Z_init = 0.02
Le18	300-0-c3	4	2D delayed-detonation, ρ₉ = 3.0, Z_init = 0
Le18	300-0.1-c3	4	2D delayed-detonation, ρ₉ = 3.0, Z_init = 0.002
Le18	300-0.5-c3	4	2D delayed-detonation, ρ₉ = 3.0, Z_init = 0.01
Le18	300-1-c3	4	2D delayed-detonation, ρ₉ = 3.0, Z_init = 0.02
Le18	300-2-c3	4	2D delayed-detonation, ρ₉ = 3.0, Z_init = 0.04
Le18	300-3-c3	4	2D delayed-detonation, ρ₉ = 3.0, Z_init = 0.06
Le18	300-5-c3	4	2D delayed-detonation, ρ₉ = 3.0, Z_init = 0.1
Le18	300-1-c3	4	2D delayed-detonation, ρ₉ = 3.0, Z_init = 0.02
Le18	500-0-c3	4	2D delayed-detonation, ρ₉ = 5.0, Z_init = 0
Le18	500-0.1-c3	4	2D delayed-detonation, ρ₉ = 5.0, Z_init = 0.002
Le18	500-0.5-c3	4	2D delayed-detonation, ρ₉ = 5.0, Z_init = 0.01
Le18	500-1-c3	4	2D delayed-detonation, ρ₉ = 5.0, Z_init = 0.02
Le18	500-2-c3	4	2D delayed-detonation, ρ₉ = 5.0, Z_init = 0.04
Le18	500-3-c3	4	2D delayed-detonation, ρ₉ = 5.0, Z_init = 0.06
Le18	500-5-c3	4	2D delayed-detonation, ρ₉ = 5.0, Z_init = 0.1
Le18	500-1-c3	4	2D delayed-detonation, ρ₉ = 5.0, Z_init = 0.02
Kr15	hyCONe	9	3D deflagration, hybrid CONe based on N5def (3)
Se16	GCD200	10	3D gravitationally confined detonation, ρ₉ = 2.9, ignition at R = 200 km
SNIa, sub-M_Ch
Pa10	0.9_0.9	11	WD-WD violent merger, M_WD ≃ 0.9 + 0.9, ρ₉ = 1.4 × 10⁻²
Kr13	0.9_0.76	12	WD-WD violent merger, M_WD = 0.9 + 0.76, ρ₉ = 1.91 × 10⁻³
Si10	det_0.81	13	1D pure detonation, ρ₉ = 1 × 10⁻², M_WD = 0.81 M_⊙
Si10	det_0.88	13	1D pure detonation, ρ₉ = 1.45 × 10⁻², M_WD = 0.88 M_⊙
Si10	det_0.97	13	1D pure detonation, ρ₉ = 2.4 × 10⁻², M_WD = 0.97 M_⊙
Si10	det_1.06	13	1D pure detonation, ρ₉ = 4.15 × 10⁻², M_WD = 1.06 M_⊙
Si10	det_1.15	13	1D pure detonation, ρ₉ = 7.9 × 10⁻², M_WD = 1.15 M_⊙
Si12	CSDD-S	14	2D double-detonation, ρ₉ = 0.85, M_WD = 0.79 M_⊙, converging shocks
Si12	CSDD-L	14	2D double-detonation, ρ₉ = 0.381, M_WD = 0.66 M_⊙, converging shocks
Si12	ELDD-S	14	2D double-detonation, ρ₉ = 0.85, M_WD = 0.79 M_⊙, edge-lit
Si12	ELDD-L	14	2D double-detonation, ρ₉ = 0.381, M_WD = 0.66 M_⊙, edge-lit
Si12	HeD-S	14	2D double-detonation, ρ₉ = 0.85, M_WD = 0.79 M_⊙, He detonation only
Si12	HeD-L	14	2D double-detonation, ρ₉ = 0.381, M_WD = 0.66 M_⊙, He detonation only
Ma15	CO15e7	15	2D pure detonation, ρ₉ = 15 × 10⁻², M_WD = 1.23 M_⊙
Ma15	ONe10e7	15	2D pure detonation, ONe WD, ρ₉ = 10 × 10⁻², M_WD = 1.18 M_⊙
Ma15	ONe13e7	15	2D pure detonation, ONe WD, ρ₉ = 13 × 10⁻², M_WD = 1.21 M_⊙
Ma15	ONe15e7	15	2D pure detonation, ONe WD, ρ₉ = 15 × 10⁻², M_WD = 1.23 M_⊙
Ma15	ONe17e7	15	2D pure detonation, ONe WD, ρ₉ = 17 × 10⁻², M_WD = 1.24 M_⊙
Ma15	ONe20e7	15	2D pure detonation, ONe WD, ρ₉ = 20 × 10⁻², M_WD = 1.25 M_⊙
Sh18	M08_3070_Z0_1	16	3D D⁶, M_WD = 0.8, C/O = 30/70, Z_init = 0, ¹²C+¹⁶O rate = 1
Sh18	M08_3070_Z0_01	16	3D D⁶, M_WD = 0.8, C/O = 30/70, Z_init = 0, ¹²C+¹⁶O rate = 0.1
Sh18	M08_3070_Z0005_1	16	3D D⁶, M_WD = 0.8, C/O = 30/70, Z_init = 0.005, ¹²C+¹⁶O rate = 1
Sh18	M08_3070_Z0005_01	16	3D D⁶, M_WD = 0.8, C/O = 30/70, Z_init = 0.005, ¹²C+¹⁶O rate = 0.1
Sh18	M08_3070_Z001_1	16	3D D⁶, M_WD = 0.8, C/O = 30/70, Z_init = 0.01, ¹²C+¹⁶O rate = 1
Sh18	M08_3070_Z001_01	16	3D D⁶, M_WD = 0.8, C/O = 30/70, Z_init = 0.01, ¹²C+¹⁶O rate = 0.1
Sh18	M08_3070_Z002_1	16	3D D⁶, M_WD = 0.8, C/O = 30/70, Z_init = 0.02, ¹²C+¹⁶O rate = 1
Sh18	M08_3070_Z002_01	16	3D D⁶, M_WD = 0.8, C/O = 30/70, Z_init = 0.02, ¹²C+¹⁶O rate = 0.1
Sh18	M08_5050_Z0_1	16	3D D⁶, M_WD = 0.8, C/O = 50/50, Z_init = 0, ¹²C+¹⁶O rate = 1
Sh18	M08_5050_Z0_01	16	3D D⁶, M_WD = 0.8, C/O = 50/50, Z_init = 0, ¹²C+¹⁶O rate = 0.1
Sh18	M08_5050_Z0005_1	16	3D D⁶, M_WD = 0.8, C/O = 50/50, Z_init = 0.005, ¹²C+¹⁶O rate = 1
Sh18	M08_5050_Z0005_01	16	3D D⁶, M_WD = 0.8, C/O = 50/50, Z_init = 0.005, ¹²C+¹⁶O rate = 0.1
Sh18	M08_5050_Z001_1	16	3D D⁶, M_WD = 0.8, C/O = 50/50, Z_init = 0.01, ¹²C+¹⁶O rate = 1
Sh18	M08_5050_Z001_01	16	3D D⁶, M_WD = 0.8, C/O = 50/50, Z_init = 0.01, ¹²C+¹⁶O rate = 0.1
Sh18	M08_5050_Z002_1	16	3D D⁶, M_WD = 0.8, C/O = 50/50, Z_init = 0.02, ¹²C+¹⁶O rate = 1
Sh18	M08_5050_Z002_01	16	3D D⁶, M_WD = 0.8, C/O = 50/50, Z_init = 0.02, ¹²C+¹⁶O rate = 0.1
Sh18	M085_3070_Z0_1	16	3D D⁶, M_WD = 0.85, C/O = 30/70, Z_init = 0, ¹²C+¹⁶O rate = 1
Sh18	M085_3070_Z0_01	16	3D D⁶, M_WD = 0.85, C/O = 30/70, Z_init = 0, ¹²C+¹⁶O rate = 0.1
Sh18	M085_3070_Z0005_1	16	3D D⁶, M_WD = 0.85, C/O = 30/70, Z_init = 0.005, ¹²C+¹⁶O rate = 1
Sh18	M085_3070_Z0005_01	16	3D D⁶, M_WD = 0.85, C/O = 30/70, Z_init = 0.005, ¹²C+¹⁶O rate = 0.1
Sh18	M085_3070_Z001_1	16	3D D⁶, M_WD = 0.85, C/O = 30/70, Z_init = 0.01, ¹²C+¹⁶O rate = 1
Sh18	M085_3070_Z001_01	16	3D D⁶, M_WD = 0.85, C/O = 30/70, Z_init = 0.01, ¹²C+¹⁶O rate = 0.1
Sh18	M085_3070_Z002_1	16	3D D⁶, M_WD = 0.85, C/O = 30/70, Z_init = 0.02, ¹²C+¹⁶O rate = 1
Sh18	M085_3070_Z002_01	16	3D D⁶, M_WD = 0.85, C/O = 30/70, Z_init = 0.02, ¹²C+¹⁶O rate = 0.1
Sh18	M085_5050_Z0_1	16	3D D⁶, M_WD = 0.85, C/O = 50/50, Z_init = 0, ¹²C+¹⁶O rate = 1
Sh18	M085_5050_Z0_01	16	3D D⁶, M_WD = 0.85, C/O = 50/50, Z_init = 0, ¹²C+¹⁶O rate = 0.1
Sh18	M085_5050_Z0005_1	16	3D D⁶, M_WD = 0.85, C/O = 50/50, Z_init = 0.005, ¹²C+¹⁶O rate = 1
Sh18	M085_5050_Z0005_01	16	3D D⁶, M_WD = 0.85, C/O = 50/50, Z_init = 0.005, ¹²C+¹⁶O rate = 0.1
Sh18	M085_5050_Z001_1	16	3D D⁶, M_WD = 0.85, C/O = 50/50, Z_init = 0.01, ¹²C+¹⁶O rate = 1
Sh18	M085_5050_Z001_01	16	3D D⁶, M_WD = 0.85, C/O = 50/50, Z_init = 0.01, ¹²C+¹⁶O rate = 0.1
Sh18	M085_5050_Z002_1	16	3D D⁶, M_WD = 0.85, C/O = 50/50, Z_init = 0.02, ¹²C+¹⁶O rate = 1
Sh18	M085_5050_Z002_01	16	3D D⁶, M_WD = 0.85, C/O = 50/50, Z_init = 0.02, ¹²C+¹⁶O rate = 0.1
Sh18	M09_3070_Z0_1	16	3D D⁶, M_WD = 0.9, C/O = 30/70, Z_init = 0, ¹²C+¹⁶O rate = 1
Sh18	M09_3070_Z0_01	16	3D D⁶, M_WD = 0.9, C/O = 30/70, Z_init = 0, ¹²C+¹⁶O rate = 0.1
Sh18	M09_3070_Z0005_1	16	3D D⁶, M_WD = 0.9, C/O = 30/70, Z_init = 0.005, ¹²C+¹⁶O rate = 1
Sh18	M09_3070_Z0005_01	16	3D D⁶, M_WD = 0.9, C/O = 30/70, Z_init = 0.005, ¹²C+¹⁶O rate = 0.1
Sh18	M09_3070_Z001_1	16	3D D⁶, M_WD = 0.9, C/O = 30/70, Z_init = 0.01, ¹²C+¹⁶O rate = 1
Sh18	M09_3070_Z001_01	16	3D D⁶, M_WD = 0.9, C/O = 30/70, Z_init = 0.01, ¹²C+¹⁶O rate = 0.1
Sh18	M09_3070_Z002_1	16	3D D⁶, M_WD = 0.9, C/O = 30/70, Z_init = 0.02, ¹²C+¹⁶O rate = 1
Sh18	M09_3070_Z002_01	16	3D D⁶, M_WD = 0.9, C/O = 30/70, Z_init = 0.02, ¹²C+¹⁶O rate = 0.1
Sh18	M09_5050_Z0_1	16	3D D⁶, M_WD = 0.9, C/O = 50/50, Z_init = 0, ¹²C+¹⁶O rate = 1
Sh18	M09_5050_Z0_01	16	3D D⁶, M_WD = 0.9, C/O = 50/50, Z_init = 0, ¹²C+¹⁶O rate = 0.1
Sh18	M09_5050_Z0005_1	16	3D D⁶, M_WD = 0.9, C/O = 50/50, Z_init = 0.005, ¹²C+¹⁶O rate = 1
Sh18	M09_5050_Z0005_01	16	3D D⁶, M_WD = 0.9, C/O = 50/50, Z_init = 0.005, ¹²C+¹⁶O rate = 0.1
Sh18	M09_5050_Z001_1	16	3D D⁶, M_WD = 0.9, C/O = 50/50, Z_init = 0.01, ¹²C+¹⁶O rate = 1
Sh18	M09_5050_Z001_01	16	3D D⁶, M_WD = 0.9, C/O = 50/50, Z_init = 0.01, ¹²C+¹⁶O rate = 0.1
Sh18	M09_5050_Z002_1	16	3D D⁶, M_WD = 0.9, C/O = 50/50, Z_init = 0.02, ¹²C+¹⁶O rate = 1
Sh18	M09_5050_Z002_01	16	3D D⁶, M_WD = 0.9, C/O = 50/50, Z_init = 0.02, ¹²C+¹⁶O rate = 0.1
Sh18	M10_3070_Z0_1	16	3D D⁶, M_WD = 1.0, C/O = 30/70, Z_init = 0, ¹²C+¹⁶O rate = 1
Sh18	M10_3070_Z0_01	16	3D D⁶, M_WD = 1.0, C/O = 30/70, Z_init = 0, ¹²C+¹⁶O rate = 0.1
Sh18	M10_3070_Z0005_1	16	3D D⁶, M_WD = 1.0, C/O = 30/70, Z_init = 0.005, ¹²C+¹⁶O rate = 1
Sh18	M10_3070_Z0005_01	16	3D D⁶, M_WD = 1.0, C/O = 30/70, Z_init = 0.005, ¹²C+¹⁶O rate = 0.1
Sh18	M10_3070_Z001_1	16	3D D⁶, M_WD = 1.0, C/O = 30/70, Z_init = 0.01, ¹²C+¹⁶O rate = 1
Sh18	M10_3070_Z001_01	16	3D D⁶, M_WD = 1.0, C/O = 30/70, Z_init = 0.01, ¹²C+¹⁶O rate = 0.1
Sh18	M10_3070_Z002_1	16	3D D⁶, M_WD = 1.0, C/O = 30/70, Z_init = 0.02, ¹²C+¹⁶O rate = 1
Sh18	M10_3070_Z002_01	16	3D D⁶, M_WD = 1.0, C/O = 30/70, Z_init = 0.02, ¹²C+¹⁶O rate = 0.1
Sh18	M10_5050_Z0_1	16	3D D⁶, M_WD = 1.0, C/O = 50/50, Z_init = 0, ¹²C+¹⁶O rate = 1
Sh18	M10_5050_Z0_01	16	3D D⁶, M_WD = 1.0, C/O = 50/50, Z_init = 0, ¹²C+¹⁶O rate = 0.1
Sh18	M10_5050_Z0005_1	16	3D D⁶, M_WD = 1.0, C/O = 50/50, Z_init = 0.005, ¹²C+¹⁶O rate = 1
Sh18	M10_5050_Z0005_01	16	3D D⁶, M_WD = 1.0, C/O = 50/50, Z_init = 0.005, ¹²C+¹⁶O rate = 0.1
Sh18	M10_5050_Z001_1	16	3D D⁶, M_WD = 1.0, C/O = 50/50, Z_init = 0.01, ¹²C+¹⁶O rate = 1
Sh18	M10_5050_Z001_01	16	3D D⁶, M_WD = 1.0, C/O = 50/50, Z_init = 0.01, ¹²C+¹⁶O rate = 0.1
Sh18	M10_5050_Z002_1	16	3D D⁶, M_WD = 1.0, C/O = 50/50, Z_init = 0.02, ¹²C+¹⁶O rate = 1
Sh18	M10_5050_Z002_01	16	3D D⁶, M_WD = 1.0, C/O = 50/50, Z_init = 0.02, ¹²C+¹⁶O rate = 0.1
Sh18	M11_3070_Z0_1	16	3D D⁶, M_WD = 1.1, C/O = 30/70, Z_init = 0, ¹²C+¹⁶O rate = 1
Sh18	M11_3070_Z0_01	16	3D D⁶, M_WD = 1.1, C/O = 30/70, Z_init = 0, ¹²C+¹⁶O rate = 0.1
Sh18	M11_3070_Z0005_1	16	3D D⁶, M_WD = 1.1, C/O = 30/70, Z_init = 0.005, ¹²C+¹⁶O rate = 1
Sh18	M11_3070_Z0005_01	16	3D D⁶, M_WD = 1.1, C/O = 30/70, Z_init = 0.005, ¹²C+¹⁶O rate = 0.1
Sh18	M11_3070_Z001_1	16	3D D⁶, M_WD = 1.1, C/O = 30/70, Z_init = 0.01, ¹²C+¹⁶O rate = 1
Sh18	M11_3070_Z001_01	16	3D D⁶, M_WD = 1.1, C/O = 30/70, Z_init = 0.01, ¹²C+¹⁶O rate = 0.1
Sh18	M11_3070_Z002_1	16	3D D⁶, M_WD = 1.1, C/O = 30/70, Z_init = 0.02, ¹²C+¹⁶O rate = 1
Sh18	M11_3070_Z002_01	16	3D D⁶, M_WD = 1.1, C/O = 30/70, Z_init = 0.02, ¹²C+¹⁶O rate = 0.1
Sh18	M11_5050_Z0_1	16	3D D⁶, M_WD = 1.1, C/O = 50/50, Z_init = 0, ¹²C+¹⁶O rate = 1
Sh18	M11_5050_Z0_01	16	3D D⁶, M_WD = 1.1, C/O = 50/50, Z_init = 0, ¹²C+¹⁶O rate = 0.1
Sh18	M11_5050_Z0005_1	16	3D D⁶, M_WD = 1.1, C/O = 50/50, Z_init = 0.005, ¹²C+¹⁶O rate = 1
Sh18	M11_5050_Z0005_01	16	3D D⁶, M_WD = 1.1, C/O = 50/50, Z_init = 0.005, ¹²C+¹⁶O rate = 0.1
Sh18	M11_5050_Z001_1	16	3D D⁶, M_WD = 1.1, C/O = 50/50, Z_init = 0.01, ¹²C+¹⁶O rate = 1
Sh18	M11_5050_Z001_01	16	3D D⁶, M_WD = 1.1, C/O = 50/50, Z_init = 0.01, ¹²C+¹⁶O rate = 0.1
Sh18	M11_5050_Z002_1	16	3D D⁶, M_WD = 1.1, C/O = 50/50, Z_init = 0.02, ¹²C+¹⁶O rate = 1
Sh18	M11_5050_Z002_01	16	3D D⁶, M_WD = 1.1, C/O = 50/50, Z_init = 0.02, ¹²C+¹⁶O rate = 0.1
Le25	100-050-2-S50	17,18	2D detonation, M_WD = 1.0, M_He = 0.05, Z_init = 0.02, spherical det.
Le25	110-050-2-B50	17,18	2D detonation, M_WD = 1.1, M_He = 0.05, Z_init = 0.02, ring-shaped det.

Notes. The inner core densities ρ₉ are given in units of 10⁹ g/cm³. The transitional deflagration-to-detonation densities ρ_T, 7 are given in units of 10⁷ g/cm³. The mass of the WD (M_WD) and, if relevant, of the He layer (M_He) are given in units of M_⊙. The Sh18 models are based on dynamically driven double-degenerate double-detonation models (DDDDDD or, more simply, D⁶).

References. (1) Iwamoto et al. (1999); (2) Maeda et al. (2010); (3) Fink et al. (2014); (4) Leung & Nomoto (2018); (5) Badenes et al. (2003); (6) Badenes et al. (2006); (7) Seitenzahl et al. (2013) (8) Ohlmann et al. (2014); (9) Kromer et al. (2015); (10) Seitenzahl et al. (2016); (11) Pakmor et al. (2010); (12) Kromer et al. (2013); (13) Sim et al. (2010); (14) Sim et al. (2012); (15) Marquardt et al. (2015); (16) Shen et al. (2018); (17) Leung & Nomoto (2020); (18) Leung et al. (2025).

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