Table 5
Populations of a few key levels arising from the 3s2 3p3 3d configuration.
| i | Lev. | POP(%) | RD(%) | EXC(%) | POP(%) | RD(%) | EXC(%) | POP(%) | RD(%) | EXC(%) | |
| D10 | D10 | D10 | RM4 | RM4 | RM4 | RM4 + DW6 | RM4 + DW6 | RM4 + DW6 | |||
|
|
|||||||||||
| 14 | 3s2 3p3 3d 5D4 | 0.13 | 63 | 37 | 0.167 | 72 | 28 | 0.176 | 73 | 27 | |
| 15.3(21) | 36(1) | 15.5(21) | 27(1) | 15.3(21) | 25(1) | ||||||
| 12.0(23) | 12.4(23) | 12.2(23) | |||||||||
| 8.7(25) | 9.4(25) | 9.4(25) | |||||||||
| 21 | 3s2 3p3 3d 3F4 | 2.6 × 10-2 | 65 | 35 | 4.0 × 10-2 | 71 | 28 | 4.1 × 10-2 | 73 | 27 | |
| 30.4(24) | 33(1) | 31.5(24) | 27(1) | 31.5(24) | 26(1) | ||||||
| 9.6(79) | 7.1(23) | 7.1(23) | |||||||||
| 6.8(23) | 6.8(79) | 6.7(79) | |||||||||
| 5.3(68) | 3.4(68) | 3.5(68) | |||||||||
| 23 | 3s2 3p3 3d 3G4 | 5.0 × 10-2 | 30 | 69 | 8.4 × 10-2 | 42 | 58 | 8.8 × 10-2 | 44 | 55 | |
| 4.7(67) | 65(1) | 4.8(32) | 54(1) | 4.8(32) | 51(1) | ||||||
| 4.6(32) | 3.4(67) | 3.7(72) | |||||||||
| 2.5(24) | 3.4(72) | 3.5(67) | |||||||||
| 24 | 3s2 3p3 3d 3G5 | 0.15 | 28 | 72 | 0.24 | 45 | 55 | 0.25 | 47 | 53 | |
| 6.4(96) | 69(1) | 9.6(147) | 53(1) | 9.7(147) | 51(1) | ||||||
| 5.0(148) | 5.1(424) | 5.5(424) | |||||||||
| 3.3(32) | 5.0(91) | 5.1(91) | |||||||||
| 3.7(161) | 4.3(161) | ||||||||||
| 25 | 3s2 3p3 3d 1G4 | 1.7 × 10-2 | 26 | 74 | 2.9 × 10-2 | 40 | 60 | 3.1 × 10-2 | 43 | 57 | |
| 5.3(184) | 69(1) | 6.6(74) | 56(1) | 7.7(74) | 53(1) | ||||||
| 5.1(32) | 5.2(32) | 5.1(32) | |||||||||
| 4.0(74) | 4.4(178) | 4.4(178) | |||||||||
| 3.7(423) | 4(423) | ||||||||||
Notes. The relative populations POP are given as percentages. RD indicates how much of the population is due to radiative decay from higher levels. EXC indicates how much of the population is due to excitation from lower levels (mostly from the ground state). Following the total percentage, the largest contributions are given, followed by the index in parenthesis of the level from which they originate, using the indexing of Tables 2 and 3. Considerable percentage contributions come from a multitude of levels not displayed here. D10 indicates values calculated with the previous model, while RM4 and RM4+DW6 with the present ion models. In all cases, the values are calculated at log Ne [cm-3] = 8 and log Te [K] = 6.15.
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