ls#ni15.dat
Resolved Specific Ion Data Collections
- Ion
- Ni15+
- Temperature Range
- 22.06 eV → 4412 eV
ADF04
- Filename
- ls#ni15.dat
- Full Path
- adf04/copmm#28/ls#ni15.dat
Download data
- Spontaneous Emission: Ni+15(i) → Ni+15(j) + hv
- Electron Impact Excitation: Ni+15(i) + e → Ni+15(j) + e
| 24515 2P2.5 | 0.0 cm-1 |
| 14525 4P5.5 | 256778.0 cm-1 |
| 14525 2D4.5 | 339911.0 cm-1 |
| 14525 2S0.5 | 387897.0 cm-1 |
| 14525 2P2.5 | 438937.0 cm-1 |
| 24516 2D4.5 | 521160.0 cm-1 |
| 35 4S1.5 | 663312.0 cm-1 |
| 35 2D4.5 | 677135.0 cm-1 |
| 14515516 4F13.5 | 730324.0 cm-1 |
| 35 2P2.5 | 737775.0 cm-1 |
| 14515516 4P5.5 | 775365.0 cm-1 |
| 14515516 4D9.5 | 780716.0 cm-1 |
| 14515516 2D4.5 | 796438.0 cm-1 |
| 14515516 2F6.5 | 839510.0 cm-1 |
| 14515516 2P2.5 | 881981.0 cm-1 |
| 14515516 2F6.5 | 914539.0 cm-1 |
| 14515516 2D4.5 | 928489.0 cm-1 |
| 14515516 2P2.5 | 936073.0 cm-1 |
| 14526 4F13.5 | 1269270.0 cm-1 |
| 14526 4P5.5 | 1298280.0 cm-1 |
| 14526 2D4.5 | 1318460.0 cm-1 |
| 14526 2G8.5 | 1329470.0 cm-1 |
| 14526 2F6.5 | 1339610.0 cm-1 |
| 14526 2P2.5 | 1366790.0 cm-1 |
| 14526 2S0.5 | 1391950.0 cm-1 |
| 36 4F13.5 | 2097890.0 cm-1 |
| 36 4P5.5 | 2125480.0 cm-1 |
| 36 2G8.5 | 2127250.0 cm-1 |
| 36 2H10.5 | 2137160.0 cm-1 |
| 36 2D4.5 | 2140010.0 cm-1 |
| 36 2P2.5 | 2141950.0 cm-1 |
| 36 2F6.5 | 2165150.0 cm-1 |
| 36 2D4.5 | 2203740.0 cm-1 |
--------------------------------------------------------------------------------- Generated from Cowan Atomic Structure Program M O'Mullane 18:22 19/05/1994 SCF method used : HR Scale factors for Slater Parameters : 80 99 85 85 60 Optically allowed transitions : yes Optically forbidden transitions M1 : parity 1 Optically forbidden transitions E2 : parity 1 Born Collision-Strength - print : 9 - forbidden : 0 -> 2 - allowed : 1 -> 1 - included : 3,all Parity 1 Parity 2 Allowed 394 0 841 initially 79 0 237 reduced --------------------------------------------------------------------------------- Correct the orbital energy line to insert 0.0 for orbitals not present in the set of configurations. Martin O'Mullane 29-11-2011 -------------------------------------------------------------------------------