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Table 1

New and remeasured laboratory oscillator strengths for Mn i.

Upper Lower Wavenumberb λ air BF BF   Unc. TP c This Work Previous Worke Calc.f
level levela (cm-1) (Å) (%) (7   s-1) log (gf) Unc. (dex)d log (gf) Unc. (dex) log (gf)

3d5(6S)4s4p a   6S5/2 24 802.25 4030.75 0.965 4 16.01 (0.80) −0.51 0.02 −0.47 0.08 −0.52
E = 24   802.25   cm-1 a   6D9/2 7749.96 12 899.76 0.026 13 0.43 (0.05) −1.07 0.05 −1.06
τ = 60.3 ± 1.3   nsg a   6D7/2 7520.25 13 293.80 0.007 13 0.12 (0.02) −1.58 0.05 −1.61
a   6D5/2 7350.73 13 600.37 0.001 13 0.02 (0.003) −2.33 0.05 −2.40
Residual 0.000
3d5(6S)4s4p a   6S5/2 24 788.05 4033.06 0.967 4 15.16 (0.76) −0.65 0.02 −0.62 0.08 −0.62
E = 24   788.05   cm-1 a   6D7/2 7506.05 13 318.94 0.017 13 0.27 (0.03) −1.37 0.05 −1.36
τ = 63.8 ± 1.4   nsf a   6D5/2 7336.53 13 626.96 0.012 13 0.19 (0.02) −1.51 0.05 −1.52
a   6D3/2 7219.57 13 847.46 0.004 13 0.06 (0.01) −1.98 0.05 −2.00
Residual 0.000
3d5(6S)4s4p a   6S5/2 24 779.32 4034.48 0.969 4 14.66 (0.73) −0.84 0.02 −0.81 0.08 −0.81
E = 24   779.32   cm-1 a   6D5/2 7327.80 13 642.93 0.009 13 0.14 (0.02) −1.82 0.05 −1.81
τ = 66.1 ± 1.4   nsf a   6D3/2 7210.84 13 864.22 0.013 13 0.20 (0.03) −1.65 0.05 −1.64
a   6D1/2 7142.11 13 997.52 0.009 13 0.14 (0.02) −1.78 0.05 −1.79
Residual 0.000
3d5(6S)4s4p a   6S5/2 31 001.15 3224.76 0.348 8 0.36 (0.04) −2.47 0.04 −2.45 0.08 −2.48
E = 31   001.15   cm-1 a   4D7/2 7704.48 12 975.91 0.524 6 0.54 (0.04) −1.09 0.03 −0.94
τ = 970 ± 50   nsf a   4D5/2 7451.95 13 415.64 0.113 9 0.12 (0.01) −1.73 0.04 −1.60
a   4D3/2 7281.63 13 729.44 0.013 10 0.01 (0.001) −2.65 0.04 −2.57
Residual 0.002
3d5(6S)4s4p a   6S5/2 31 076.42 3216.95 0.261 8 0.23 (0.02) −2.84 0.04 −2.82 0.08 −2.82
E = 31   076.42   cm-1 a   4D5/2 7527.22 13 281.49 0.473 6 0.42 (0.03) −1.35 0.03 −1.23
τ = 1120 ± 50   nsf a   4D3/2 7356.90 13 588.97 0.229 8 0.21 (0.02) −1.64 0.04 −1.53
a   4D1/2 7257.55 13 774.99 0.035 9 0.03 (0.003) −2.45 0.04 −2.35
Residual 0.002

Notes. 

(a)

Full term designations for the lower levels are 3d6(5D)4s a4,6DJ and 3d5(6S)4s2 a6S5/2.

(b)

Ritz wavenumber.

(c)

Transition probability, the uncertainty is given in brackets (± ).

(d)

The uncertainty in the log (gf) is expressed in dex, where  ± 0.01 dex corresponds to approximately  ± 2.5 per cent.

(e)

The previous laboratory log (gf)s from Booth et al. (1984), the uncertainties in the log (gf)s of Booth et al. (1984) are those assigned by NIST, Fuhr & Wiese (2003).

(f)

Semi-empirical log (gf) calculations of Kurucz & Bell (1995).

(g)

Radiative lifetime values, τ, for are from Schnabel et al. (1995) and for are from Kronfeldt et al. (1985).

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