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Table 1

Data for important transitions, including diagnostic lines.

λ Transition log gf Source Γ6 log Γ4/Ne Source Dr Dp Gr Gp
σ α (5000 K)
[Å] [au] [rad s-1 cm3]

Mg i
3829 3d 3D 0.23 Fro/NIST 708 0.301 4.51 D-SB H H CH CH
3832 3d 3D 0.25 Fro/NIST 708 0.301 4.51 D-SB H H CH CH
3838 3d 3D 0.47 Fro/NIST 708 0.301 4.51 D-SB H H CH CH
4167 7d 1D 3p 1 0.75 C-T/NIST 222 0.249 3.49 D-SB H H CH H
4571 3p 3P 3s 1S 5.62 Fro/NIST 222 0.249 6.51 Mas H H CE CE
4703 5d 1D 3p 1 0.44 C-T/NIST 2806 0.269 4.11 D-SB H H CH H
5167 4s 3S 0.93 Ald 728 0.238 5.40 D-SB H CH CH CH
5173 4s 3S 0.45 Ald 728 0.238 5.40 D-SB CH CH CH CH
5184 4s 3S 0.24 Ald 728 0.238 5.40 D-SB CH CH CH CH
5528 4d 1D 3p 1 0.50 C-T/NIST 1460 0.312 4.56 D-SB H H CH CH
8710 7d 3D 1.57 But/NIST 2.72 D-SB CH0 CH0 CH H
8713 7d 3D 1.09 But/NIST 2.72 D-SB CH0 CH0 CH H
8718 7d 3D 0.87 But/NIST 2.72 D-SB CH0 CH0 CH H
8736 7f 3F° 3d 3D 0.53 But/NIST 2.95 D-SB CH0 CH0 CH H
8806 3d 1D 3p 1 0.13 Fro/NIST 529 0.277 5.39 D-SB CH CH CH CH
73 700 6h H° 5g 3G 1.34 Civ 4950 1.549 3.06 vR-HB CH CE CH CH
122 200 7h H° 6g G 1.62 Civ 5191 1.738 2.39 D-SB CH CH CH CH
123 200 7i I 6h H° 1.95 Hydro 4657 1.752 2.55 D-SB H CH0 CH CH0
188 300 8h H° 7g G 0.49 Hydro 4497 1.764 2.92 vR-HB CH0 CH0 CH CH
189 500 8i I 7h H° 1.90 Hydro 4304 1.778 2.12 vR-HB H H CH CH
Mg ii
4385 5d 2D 0.78 Sie/NIST
4391 5d 2D 0.48 Sie/NIST
4481 4f 2F° 3d 2D 0.76 Fro/NIST
5402 7g 2G 4f 2 0.06 K-P
7877 4d 2D3/2 0.39 Sie/NIST
7896 4d 2D5/2 0.64 Sie/NIST

Notes. Columns 1 and 2 give the transition wavelength and labels for the states involved. Columns 3 and 4 give the adopted oscillator strength, in the form log (gf), and the source of these data (see notes). Columns 58 give collisional broadening data (see text and notes). Columns 912 show, for each line of Mg i, the collision process most responsible for the changes between model B and model F, and thus indicates the most important contributor of the new collision data introduced in this work (see Sect. 5 for more details). Results are given for the four test atmospheric models described in Sect. 5: Dr = Dwarf, metal-rich; Dp = Dwarf, metal-poor; Gr = Giant, metal-rich; Gp = Giant, metal-poor. The collisional processes are labelled (see Sect. 5) H when the line has a sensitivity similar to charge transfer with H  and CH0; collisional excitation with H , CH, and CE indicates the line is sensitive mostly to the electron collision rates. For Mg ii lines there are non-LTE effects in some lines, but the non-LTE abundance corrections are not sensitive to any particular collisional process. Oscillator strengths (f-values) were collected mostly from the NIST database (Ralchenko et al. 2010). The original sources of the NIST data are Froese Fischer & Tachiev (2010) [Fro], Chang & Tang (1990) [C-T] Butler et al. (1993) [But], Siegel et al. (1998) [Sie]. Other sources are Aldenius et al. (2007) [Ald], Civiš, S. et al. (2013) [Civ] and Kurucz & Peytremann (1975) [K-P]. For the Mg i IR lines with no data found in the literature we calculated the f-values using the hydrogenic formula from Guseinov & Mamedov (2012) [Hydro]. To calculate the van der Waals line widths Γ6 we used data in the ABO theory format where σ is the broadening cross-section in atomic units and α is the velocity parameter. These were calculated with the ABO theory except for those marked with an asterisks, which were calculated in this work (see Table 3 for the IR lines). Stark broadening line widths, Γ4, were taken from Dimitrijevic & Sahal-Bréchot (1996) [D-SB], van Regemorter & Hoang Binh (1993) [vR-HB] and Mashonkina (2013, including only electrons) [Mas].

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