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Table D.1

Calculated transition probabilities of Nd III using configuration interaction spaces of Table 1 (extract).

Type CF ɡuA log(ɡlƒ) σRitz λRitz λRitzair$\lambda _{{\rm{Ritz}}}^{{\rm{air}}}$ Lower Level Jl Upper Level Ju El Eu gll$g_l^l$ gul$g_u^l$
(s−1) (cm−1) (Å) (Å) Term Label Term Label (cm−1) (cm−1)
(1) (2) (3) (4) (5) (6) (7) (8) (9) (10) (11) (12) (13) (14) (15)
2 0.01 2.2×106 −2.92 52 659.745(*) 1898.9837(*) 1898.3517 4f3(4D°)5d 5 4 4f2(3H)5d(2D)(4G)6s 5G 3 47 404.355 100 064.1 1.223 0.944
2 0.00 6.0×105 −3.49 52 648.771(*) 1899.3796(*) 1898.7474 4f3(4I°)6s(112,12)°$4{{\rm{f}}^3}\left( {^4{\rm{I}}^\circ } \right)6{\rm{s}}\left( {{{11} \over 2},{1 \over 2}} \right)^\circ $ 5 4f2(3F)5d2(3F) 5G 5 32 309.729 84 958.5 0.875 1.201
2 0.00 2.9×106 −2.80 52 645.550(*) 1899.4958(*) 1898.8636 4f3(2H2°)5d 1 4 4f2(3H)5d2(3P)5H 5 36517.350 89 162.9 1.067 1.173
2 0.08 8.0×107 −1.36 52 643.587(*) 1899.5666(*) 1898.9344 4f3(4F°)5d 3 4 4f3(2D1°) 6p 3F 3 32077.113 84 720.7 0.948 1.076
2 0.01 4.4×106 −2.62 52 636.914(*) 1899.8074(*) 1899.1752 4f3(2H2°)5d 3 6 4f2(3H)5d2(3F)5H 7 29 643.186 82280.1 0.990 1.133
2 0.12 l.1×106 −2.44 21 331.734(*) 4687.8514(*) 4686.5398 4f3(4I°)6d 3 5 4f3(4F°)5f 3G 5 108 852.966 130184.7 1.087 1.165
1 0.00 2.3×103 −5.12 21 328.712(*) 4688.5156(*) 4687.2038 4f3(2H2°)6s 3 5 4f3(4I°)6p 3I 5 43 022.1 64350.812 1.129 0.849
R 0.01 2.2×105 −3.14 21 325.613(800) 4689.1970(1800) 4687.8850 4f3(4I°)6d 3 6 4f3(4F°)5f 5I 6 105 866.787 127 192.4 0.966 1.052
L 0.11 4.5×106 −1.83 21 320.284(6) 4690.3690(13) 4689.0567 4f4 5I 7 4f3(4I°)5d 3 6 3714.548 25 034.832 1.177 1.241
2 0.01 1.1×104 −4.44 21 319.013(*) 4690.6487(*) 4689.3363 4f3(4I°)6d 5 4 4f2(1I)5d(2D)(2H)6s 3H 5 106265.687 127584.7 0.993 1.108
12 0.10 8.6×103 −2.55 2126.8(*) 47 019.00(*) 47 006.18 4f3(2K°)5d 1 5 4f4 1G3 4 46 408.0 48 534.8 1.014 1.005
1 0.03 1.4×103 −3.32 2089.525(*) 47 857.7667(*) 47 844.7207 4f4 3F2 3 4f3(4I°)5d 3 4 24 050.7 26 140.225 1.113 1.060
1 0.05 1.3×103 −3.34 2059.925(*) 48 545.4568(*) 48 532.2233 4f4 3M 8 4f3(4I°)5d 3 7 21 943.3 24 003.225 0.948 1.171
1 0.07 1.6×103 −3.23 2007.711 (*) 49 807.9654(*) 49 794.3880 4f4 3I1 7 4f3(4I°)5d 3 8 25 434.2 27 441.911 1.137 1.138
12 0.02 1.8×103 −3.17 2005.9(*) 49 852.93(*) 49 839.34 4f4 3H3 5 4f3(2Gl°)5d 3 5 38 143.2 40 149.1 1.028 1.120

Notes. The electronic version of this table is available at Zenodo. In Col. 1, the label ‘1’ indicates (experimentally) unknown lower level, ‘2’ indicates unknown upper level, ‘12’ indicates that both levels are unknown, ‘L’ indicates a transition observed in the laboratory, and ‘R’ indicates a transition with known levels but unobserved in the laboratory. The remaining columns are: (2) cancellation factor as defined in Cowan (1981), (3)-(4) weighted TP and log of the weighted (absorption) oscillator strength, where ɡu and ɡl refer to statistical weights of the upper and lower energy levels, respectively, (5)–(7) vacuum Ritz wavenumber, vacuum Ritz wavelength, and air Ritz wavelength converted using the three term dispersion formula from Peck & Reeder (1972), respectively, where uncertainties are given in parentheses in units of the final decimal places for lines with types ‘L’ and ‘R’, otherwise, ‘*’ indicates at least one unknown energy level for a transition, (8)–(13) level term labels, J values, and energies, where the term labels of unknown levels are from the leading eigenvectors in the LS coupling scheme, and (14)–(15) upper and lower level Landé ɡ-factors.

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