Theoretical investigation of transition data of astrophysical importance in neutral sulphur

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Table A.2

Computed transition data.

			ab initio						fine-tuned
			log(gf)		A (s⁻¹)		Acc		log(gf)		A (s⁻¹)		Acc.
Upper state	Lower state	λ (Å)	B	C	B	C	B	C	B	C	B	C	B	C
$3 p^{3} (^{4} S) 6 d 3 D_{1}^{o}$ $Mathematical equation: $\[3 \mathrm{p}^{3}({ }^{4} \mathrm{S}) 6 \mathrm{d}~^{3} \mathrm{D}_{1}^\mathrm{o}\]$$	3p⁴ ³P₂	1247.11	−4.01	−3.98	1.39E+05	1.50E+05	C	C	−4.04	−4.01	1.29E+05	1.39E+05	C	C
$3 p^{3} (^{4} S) 6 d 3 D_{2}^{o}$ $Mathematical equation: $\[3 \mathrm{p}^{3}(^{4} \mathrm{S}) 6 \mathrm{d}~^{3} \mathrm{D}_{2}^{\mathrm{o}}\]$$	3p⁴ ³P₂	1247.14	−2.86	−2.83	1.17E+06	1.26E+06	C	C	−2.90	−2.87	1.08E+06	1.17E+06	C	C
$3 p^{3} (^{4} S) 6 d 3 D_{3}^{o}$ $Mathematical equation: $\[3 \mathrm{p}^{3}({ }^{4} \mathrm{S}) 6 \mathrm{d}~^{3} \mathrm{D}_{3}^\mathrm{o}\]$$	3p⁴ ³P₂	1247.16	−2.15	−2.12	4.32E+06	4.67E+06	C	C	−2.19	−2.16	3.93E+06	4.27E+06	C	C
$3 p^{3} (^{4} S) 6 d 5 D_{3}^{o}$ $Mathematical equation: $\[3 \mathrm{p}^{3}(^{4} \mathrm{S}) 6 \mathrm{d}~^{5} \mathrm{D}_{3}^{\mathrm{o}}\]$$	3p⁴ ³P₂	1250.12	−6.43	−7.27	2.28E+02	3.25E+01	E	E	−5.82	−6.13	9.14E+02	4.54E+02	E	E
$3 p^{3} (^{4} S) 6 d 5 D_{2}^{o}$ $Mathematical equation: $\[3 \mathrm{p}^{3}(^{4} \mathrm{S}) 6 \mathrm{d}~^{5} \mathrm{D}_{2}^\mathrm{o}\]$$	3p⁴ ³P₂	1250.12	−6.13	−6.43	6.37E+02	3.20E+02	E	E	−6.14	−6.45	6.20E+02	3.04E+02	E	E
$3 p^{3} (^{4} S) 6 d 5 D_{1}^{o}$ $Mathematical equation: $\[3 \mathrm{p}^{3}(^{4} \mathrm{S}) 6 \mathrm{d}~^{5} \mathrm{D}_{1}^{\mathrm{o}}\]$$	3p⁴ ³P₂	1250.12	−6.50	−6.71	4.50E+02	2.79E+02	E	E	−6.56	−6.79	3.89E+02	2.28E+02	E	E
$3 p^{3} (^{4} S) 6 d 3 D_{1}^{o}$ $Mathematical equation: $\[3 \mathrm{p}^{3}({ }^{4} \mathrm{S}) 6 \mathrm{d}~^{3} \mathrm{D}_{1}^\mathrm{o}\]$$	3p⁴ ³P₁	1253.30	−2.85	−2.82	1.99E+06	2.14E+06	C	C	−2.89	−2.86	1.84E+06	1.97E+06	C	C
$3 p^{3} (^{4} S) 6 d 3 D_{2}^{o}$ $Mathematical equation: $\[3 \mathrm{p}^{3}(^{4} \mathrm{S}) 6 \mathrm{d}~^{3} \mathrm{D}_{2}^{\mathrm{o}}\]$$	3p⁴ ³P₁	1253.33	−2.40	−2.37	3.35E+06	3.60E+06	C	C	−2.44	−2.41	3.07E+06	3.30E+06	C	C
$3 p^{3} (^{4} S) 6 d 5 D_{2}^{o}$ $Mathematical equation: $\[3 \mathrm{p}^{3}(^{4} \mathrm{S}) 6 \mathrm{d}~^{5} \mathrm{D}_{2}^\mathrm{o}\]$$	3p⁴ ³P₁	1256.34	−8.91	−7.70	1.04E+00	1.67E+01	E	E	−8.56	−7.86	2.31E+00	1.16E+01	E	E
$3 p^{3} (^{4} S) 6 d 5 D_{1}^{o}$ $Mathematical equation: $\[3 \mathrm{p}^{3}({ }^{4} \mathrm{S}) 6 \mathrm{d}~^{5} \mathrm{D}_{1}^\mathrm{o}\]$$	3p⁴ ³P₁	1256.34	−6.48	−6.76	4.68E+02	2.44E+02	E	E	−6.66	−7.03	3.04E+02	1.31E+02	E	E
−	−	−	−	−	−	−	−	−	−	−	−	−	−	−

Notes. Only the first ten rows are shown. The wavelengths are vacuum wavelengths obtained based on the energy levels in the NIST ASD originated from Civiš et al. (2024). It should be noted that the wavelengths of the transitions associated with No. 94 and 95 (3p³(⁴S)7p ⁵P₁, 2) were calculated using the energy value of No. 96 (3p³(⁴S)7p ⁵P₃). Full table is available at the CDS.

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