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 1P° | −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 1P° | −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 1P° | −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 1P° | −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 2F° | 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 5−8 give collisional broadening data (see text and notes). Columns 9−12 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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