Rb2+ energy levels in Rydbergs (Ry) from the large-scale grasp calculations compared with the available tabulations from the NIST data base (Kramida et al. 2018). A sample of the lowest 13 levels for the residual Rb2+ ion from the 456-level grasp calculations are shown compared to experiment. The percentage difference Δ(per cent) compared to experiment individual energy levels is given for completeness.
Level . | STATE . | TERM . | NIST (Ry) . | GRASP (Ry) . | Δ(per cent)a . |
---|---|---|---|---|---|
1 | 4s24p5 | |$\rm ^2P^o_{3/2}$| | 0.000 00 | 0.000 00 | 0.0 |
2 | 4s24p5 | |$\rm ^2P^o_{1/2}$| | 0.067 20 | 0.066 78 | 0.6 |
3 | 4s4p6 | |$\rm ^2S_{1/2}$| | 1.184 94 | 1.222 87 | 3.2 |
4 | 4s24p4(3P)4d | |$\rm ^4D_{7/2}$| | 1.409 92 | 1.444 46 | 2.5 |
5 | 4s24p4(3P)4d | |$\rm ^4D_{5/2}$| | 1.411 35 | 1.446 80 | 2.5 |
6 | 4s24p4(3P)4d | |$\rm ^4D_{3/2}$| | 1.417 61 | 1.453 68 | 2.5 |
7 | 4s24p4(3P)4d | |$\rm ^4D_{1/2}$| | 1.425 16 | 1.461 40 | 2.5 |
8 | 4s24p4(3P)4d | |$\rm ^4F_{9/2}$| | 1.484 62 | 1.536 50 | 3.5 |
9 | 4s24p4(3P)4d | |$\rm ^4F_{7/2}$| | 1.508 53 | 1.563 35 | 3.6 |
10 | 4s24p4(3P)4d | |$\rm ^4F_{5/2}$| | 1.529 29 | 1.581 92 | 3.4 |
11 | 4s24p4(3P)4d | |$\rm ^4F_{3/2}$| | 1.537 77 | 1.590 50 | 3.4 |
12 | 4s24p4(1P)4d | |$\rm ^2P_{1/2}$| | 1.513 51 | 1.592 18 | 5.2 |
13 | 4s24p4(1P)4d | |$\rm ^2D_{3/2}$| | 1.567 76 | 1.620 83 | 3.4 |
Level . | STATE . | TERM . | NIST (Ry) . | GRASP (Ry) . | Δ(per cent)a . |
---|---|---|---|---|---|
1 | 4s24p5 | |$\rm ^2P^o_{3/2}$| | 0.000 00 | 0.000 00 | 0.0 |
2 | 4s24p5 | |$\rm ^2P^o_{1/2}$| | 0.067 20 | 0.066 78 | 0.6 |
3 | 4s4p6 | |$\rm ^2S_{1/2}$| | 1.184 94 | 1.222 87 | 3.2 |
4 | 4s24p4(3P)4d | |$\rm ^4D_{7/2}$| | 1.409 92 | 1.444 46 | 2.5 |
5 | 4s24p4(3P)4d | |$\rm ^4D_{5/2}$| | 1.411 35 | 1.446 80 | 2.5 |
6 | 4s24p4(3P)4d | |$\rm ^4D_{3/2}$| | 1.417 61 | 1.453 68 | 2.5 |
7 | 4s24p4(3P)4d | |$\rm ^4D_{1/2}$| | 1.425 16 | 1.461 40 | 2.5 |
8 | 4s24p4(3P)4d | |$\rm ^4F_{9/2}$| | 1.484 62 | 1.536 50 | 3.5 |
9 | 4s24p4(3P)4d | |$\rm ^4F_{7/2}$| | 1.508 53 | 1.563 35 | 3.6 |
10 | 4s24p4(3P)4d | |$\rm ^4F_{5/2}$| | 1.529 29 | 1.581 92 | 3.4 |
11 | 4s24p4(3P)4d | |$\rm ^4F_{3/2}$| | 1.537 77 | 1.590 50 | 3.4 |
12 | 4s24p4(1P)4d | |$\rm ^2P_{1/2}$| | 1.513 51 | 1.592 18 | 5.2 |
13 | 4s24p4(1P)4d | |$\rm ^2D_{3/2}$| | 1.567 76 | 1.620 83 | 3.4 |
aAbsolute percentage difference, Δ(per cent), between theoretical and experimental energy levels for the Rb iii ion. The average Δ(per cent) of the energy levels with experiment is ≈3 per cent.
Rb2+ energy levels in Rydbergs (Ry) from the large-scale grasp calculations compared with the available tabulations from the NIST data base (Kramida et al. 2018). A sample of the lowest 13 levels for the residual Rb2+ ion from the 456-level grasp calculations are shown compared to experiment. The percentage difference Δ(per cent) compared to experiment individual energy levels is given for completeness.
Level . | STATE . | TERM . | NIST (Ry) . | GRASP (Ry) . | Δ(per cent)a . |
---|---|---|---|---|---|
1 | 4s24p5 | |$\rm ^2P^o_{3/2}$| | 0.000 00 | 0.000 00 | 0.0 |
2 | 4s24p5 | |$\rm ^2P^o_{1/2}$| | 0.067 20 | 0.066 78 | 0.6 |
3 | 4s4p6 | |$\rm ^2S_{1/2}$| | 1.184 94 | 1.222 87 | 3.2 |
4 | 4s24p4(3P)4d | |$\rm ^4D_{7/2}$| | 1.409 92 | 1.444 46 | 2.5 |
5 | 4s24p4(3P)4d | |$\rm ^4D_{5/2}$| | 1.411 35 | 1.446 80 | 2.5 |
6 | 4s24p4(3P)4d | |$\rm ^4D_{3/2}$| | 1.417 61 | 1.453 68 | 2.5 |
7 | 4s24p4(3P)4d | |$\rm ^4D_{1/2}$| | 1.425 16 | 1.461 40 | 2.5 |
8 | 4s24p4(3P)4d | |$\rm ^4F_{9/2}$| | 1.484 62 | 1.536 50 | 3.5 |
9 | 4s24p4(3P)4d | |$\rm ^4F_{7/2}$| | 1.508 53 | 1.563 35 | 3.6 |
10 | 4s24p4(3P)4d | |$\rm ^4F_{5/2}$| | 1.529 29 | 1.581 92 | 3.4 |
11 | 4s24p4(3P)4d | |$\rm ^4F_{3/2}$| | 1.537 77 | 1.590 50 | 3.4 |
12 | 4s24p4(1P)4d | |$\rm ^2P_{1/2}$| | 1.513 51 | 1.592 18 | 5.2 |
13 | 4s24p4(1P)4d | |$\rm ^2D_{3/2}$| | 1.567 76 | 1.620 83 | 3.4 |
Level . | STATE . | TERM . | NIST (Ry) . | GRASP (Ry) . | Δ(per cent)a . |
---|---|---|---|---|---|
1 | 4s24p5 | |$\rm ^2P^o_{3/2}$| | 0.000 00 | 0.000 00 | 0.0 |
2 | 4s24p5 | |$\rm ^2P^o_{1/2}$| | 0.067 20 | 0.066 78 | 0.6 |
3 | 4s4p6 | |$\rm ^2S_{1/2}$| | 1.184 94 | 1.222 87 | 3.2 |
4 | 4s24p4(3P)4d | |$\rm ^4D_{7/2}$| | 1.409 92 | 1.444 46 | 2.5 |
5 | 4s24p4(3P)4d | |$\rm ^4D_{5/2}$| | 1.411 35 | 1.446 80 | 2.5 |
6 | 4s24p4(3P)4d | |$\rm ^4D_{3/2}$| | 1.417 61 | 1.453 68 | 2.5 |
7 | 4s24p4(3P)4d | |$\rm ^4D_{1/2}$| | 1.425 16 | 1.461 40 | 2.5 |
8 | 4s24p4(3P)4d | |$\rm ^4F_{9/2}$| | 1.484 62 | 1.536 50 | 3.5 |
9 | 4s24p4(3P)4d | |$\rm ^4F_{7/2}$| | 1.508 53 | 1.563 35 | 3.6 |
10 | 4s24p4(3P)4d | |$\rm ^4F_{5/2}$| | 1.529 29 | 1.581 92 | 3.4 |
11 | 4s24p4(3P)4d | |$\rm ^4F_{3/2}$| | 1.537 77 | 1.590 50 | 3.4 |
12 | 4s24p4(1P)4d | |$\rm ^2P_{1/2}$| | 1.513 51 | 1.592 18 | 5.2 |
13 | 4s24p4(1P)4d | |$\rm ^2D_{3/2}$| | 1.567 76 | 1.620 83 | 3.4 |
aAbsolute percentage difference, Δ(per cent), between theoretical and experimental energy levels for the Rb iii ion. The average Δ(per cent) of the energy levels with experiment is ≈3 per cent.
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