Table A.1
Energy levels experimentally established and semi-empirically calculated for Nd III (extract).
Par. | Label | J | E | ΔE | τ | Eigenvector Composition | |||
---|---|---|---|---|---|---|---|---|---|
(cm−1) | (cm−1) | (s) | (%) | ||||||
(1) | (2) | (3) | (4) | (5) | (6) | (7) | (8) | ||
e | 4f4 5I | 4 | 0.000(*) | 4.2 | 0.604 | 97 4f4 5I | |||
⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ |
e | 4f3(4I°)5f 5L | 6 | 114016.4(6) | −4.8 | 5.2 × 10−10 | 0.760 | 79 4f3(4I°)5f 5L | 13 4f3(4I°)5f 5K | 2 4f3(2H2°)5f 3K |
e | 4f3(4I°)5f 5M | 7 | 114015.1(5) | −6.5 | 5.1 × 10−10 | 0.768 | 88 4f3(4I°)5f 5M | 7 4f3(4I°)5f 5L | 3 4f3(2H2°)5f 3L |
e | 4f3(4I°)5f 5K | 5 | 114021.3(4) | −18.0 | 5.1 × 10−10 | 0.702 | 81 4f3(4I°)5f 5K | 14 4f3(4I°)5f 3I | 2 4f3(2H2°)5f 3I |
⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ |
e | 8 | 130935.4(*) | 5.2 × 10−10 | 1.020 | 51 4f3(2H2°)5f 1L | 19 4f3(2H2°)5f 3L | 10 4f3(2H1°)5f 1L | ||
o | 4f3(4I°)5d 5L° | 6 | 15158.154(7) | −53.0 | 3.2 × 10−3 | 0.724 | 93 4f3(4I°)5d 5L° | 3 4f3(2H2°)5d 3K° | 3 4f3(4I°)5d 3K° |
⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ |
o | 3 | 47 499.8(*) | 1.5 × 10−6 | 0.926 | 53 4f3(4G°)6s 5G° | 17 4f3(2G1°)6s 3G° | 13 4f3(2G2°)6s 3G° | ||
o | ![]() |
4 | 103085.765(10) | −5.7 | 1.4 × 10−9 | 0.605 | 97 4f3(4I°)7s 5I° | 3 4f3(2H2°)7s 3H° | |
o | ![]() |
5 | 103335.469(8) | −2.7 | 1.4 × 10−9 | 0.866 | 56 4f3(4I°)7s 3I° | 40 4f3(4I°)7s 5I° | 2 4f3(2H2°)7s 3H° |
o | 1 | 103 359.1(*) | 1.8 × 10−7 | 1.000 | 59 4f3(2F1°)5d 1P° | 40 4f3(2F2°)5d 1P° | |||
o | 4f3(4I°)6d 5K° | 5 | 103 652.472(9) | 2.6 | 1.1 × 10−9 | 0.695 | 84 4f3(4I°)6d 5K° | 11 4f3(4I°)6d 3I° | 3 4f3(2H2°)6d 3I° |
⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ | ⋮ |
o | 4f3(4I°)6d 3G° | 5 | 111 138.018(18) | −26.2 | 1.3 × 10−9 | 1.196 | 79 4f3(4I°)6d 3G° | 12 4f3(4I°)6d 5G° | 4 4f3(4I°)6d 3H° |
Notes. The full version of this table is available at Zenodo with up to five leading eigenvector components for each energy level. The columns are: (1) parity, where ‘e’ is for even and ‘o’ is for odd, (2) assigned configuration and term label for levels experimentally found, (3) total angular momentum J, (4) experimentally determined or semi-empirically calculated level energy in this work, uncertainties are in parentheses in units of the final decimal place for experimental energies, an uncertainty ‘*’ indicates an experimentally unknown level, where only the calculated energy is shown, (5) difference between observed and calculated level energies, (6)-(8) lifetime due to electric dipole (E1) transitions, Landé ɡ-factor, and three leading eigenvector percentages calculated using the Cowan code in this work.
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