Table A.1
Sources and parameters of opacities used in this work
Source | Line list | Cutting Length (cm−1) | |
---|---|---|---|
Al | This worka | Kurucz1 | - |
AlO | DACEb & This work | ATP2 | 100 |
Ca | This work | Kurucz | - |
CaO | DACE & This work | VBATHY3 | 100 |
Fe | This Work | Kurucz | - |
K | This Work | Kurucz | - |
Mg | This Work | Kurucz | - |
MgO | DACE & This work | LiTY4 | 100 |
Na | This Workc | VALD35 | Varied (300 max) |
O | This Work | Kurucz | - |
O2 | This Work | HITRAN6 | 100 |
Si | This Work | Kurucz | - |
SiO | This Work | Kurucz (shortwave) & EBJT7 | Varied (300 max) |
SiO2 | DACE | OYT38 | 100 |
Ti | This Work | Kurucz | - |
TiO | DACE & This Work | Toto9 | 100 |
Al+ | This Work | Kurucz | - |
Ca+ | This Work | Kurucz | - |
Fe+ | This Work | Kurucz | - |
Mg+ | This Work | Kurucz | - |
Na+ | This Work | Kurucz | - |
O+ | This Work | Kurucz | - |
Si+ | This Work | Kurucz | - |
Ti+ | This Work | Kurucz | - |
a Opacities are computed with HELIOS-K https://github.com/exoclime/HELIOS-K (Grimm & Heng 2015; Grimm et al. 2021) ; b DACE database https://dace.unige.ch/; c Na doublet wings computed using the unified line-shape theory of Rossi & Pascale (1985); Allard et al. (2007a,b);1 Kurucz (Kurucz 1992);2 ATP (Patrascu et al. 2015);3 VBATHY (Yurchenko et al. 2016);4 LiTY (Li et al. 2019);5 VALD3 (Ryabchikova et al. 2015);6 HITRAN (Gordon et al. 2017; Chubb et al. 2021);7 EBJT (Gordon et al. 2017; Chubb et al. 2021);8 OYT3 (Owens et al. 2020);8 Toto (McKemmish et al. 2019). We note that we only use opacities of main isotopes. In this work we make use of the DACE (Grimm & Heng 2015; Grimm et al. 2021), ExoMol (Chubb et al. 2021), HITRAN (Gordon et al. 2017), Kurucz (Kurucz 1992) and VALD3 (Ryabchikova et al. 2015) opacity databases.
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