Open Access

Table 1

Parameters of the least-squares fit of energy levels of the 4f4, 4f35d, 4f36s, and 4f36p configurations of Nd III in Cowan’s codes (extract).

Conf. Param. LSF(a) (cm−1) G(b) HFR(a) (cm−1) Ratio(a, c)
4f4 Eav 32 348(22) 35 503 −3156
F2(4f,4f) 71 335(105) 92636 0.770
F4(4f,4f) 40 755(201) 57680 0.707
F6(4f,4f) 35 267(f) 3 41 372 0.852
α (4f) 8(f) 0
β (4f) −310(f) 0
γ (4f) 1110(f) 0
ζ (4f) 782(4) 849 0.921

4f35d Eav 44999(43) 36 770 8229
F2(4f,4f) 78 070(397) 1 101 378 0.770
F4(4f,4f) 49 616(383) 2 63 552 0.781
F6(4f,4f) 38 949(554) 3 45 705 0.852
α(4f) 22(f) 0
β(4f) −600(f) 0
γ(4f) 1450(f) 0
ζ(4f) 882(2) 4 947 0.932
ζ(5d) 785(7) 831 0.945
F1(4f,5d) 953(81) 0
F2(4f,5d) 19310(119) 26408 0.731
F3(4f,5d) 0(f) 0
F4(4f,5d) 13 958(275) 13 022 1.072
G1(4f,5d) 9138(39) 12824 0.713
G2(4f,5d) 1689(198) 0
G3(4f,5d) 9205(142) 10202 0.902
G4(4f,5d) 0(f) 0
G5(4f,5d) 5148(126) 7735 0.666

4f36s Eav 55 647(49) 47956 7691
F2(4f,4f) 78 723(400) 1 102226 0.770
F4(4f,4f) 50 064(387) 2 64126 0.781
F6(4f,4f) 39 310(559) 3 46129 0.852
α(4f) 22(f) 0
β(4f) −600(f) 0
γ(4f) 1450(f) 0
ζ(4f) 886(2) 4 953 0.932
G3(4f,6s) 2393(72) 2870 0.834

4f36p 88 343(29) 79811 8544
F2(4f,4f) 78 655(146) 102329 0.769
F4(4f,4f) 49 923(164) 64196 0.778
F6(4f,4f) 39 344(f) 3 46180 0.852
α(4f) 22(f) 0
β(4f) −600(f) 0
γ(4f) 1450(f) 0
ζ(4f) 888(2) 954 0.930
ζ(6p) 2467(10) 1989 1.240
F1(4f,6p) 739(45) 0
F2(4f,6p) 6396(359) 7861 0.814
G2(4f,6p) 2082(55) 1981 1.051
G3(4f,6p) 0(f) 0
G4(4f,6p) 1490(93) 1791 0.832

Notes. The full version of this table is available at the CDS. (a)Parameter values determined in the ab initio pseudo-relativistic Hartree-Fock (HFR) and least-squares-fitted (LSF) calculations and their ratio. Standard deviations of the fitted LSF parameters are in parentheses, where ‘f’ means the parameter was fixed. (b) Parameters in each numbered group (G) were linked together by sharing the same ratios to their corresponding HFR values. (c)Differences between LSF and HFR parameters are given for Eav.

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