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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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