ic#cu1.dat
Resolved Specific Ion Data Collections
- Ion
- Cu1+
- Temperature Range
- 0.069 eV → 758 eV
ADF04
- Filename
- ic#cu1.dat
- Full Path
- adf04/copmm#29/ic#cu1.dat
Download data
- Spontaneous Emission: Cu+1(i) → Cu+1(j) + hv
- Electron Impact Excitation: Cu+1(i) + e → Cu+1(j) + e
| 65606 1S0.0 | 0.0 cm-1 |
| 65596517 3D3.0 | 9658.5 cm-1 |
| 65596517 3D2.0 | 10507.9 cm-1 |
| 65596517 3D1.0 | 11592.9 cm-1 |
| 65596517 1D2.0 | 13704.2 cm-1 |
| 65596518 3P2.0 | 52631.0 cm-1 |
| 65596518 3P1.0 | 53928.4 cm-1 |
| 65596518 3F3.0 | 54250.0 cm-1 |
| 65596518 3F4.0 | 54292.6 cm-1 |
| 65596518 3P0.0 | 54779.6 cm-1 |
| 65596518 3F2.0 | 55469.1 cm-1 |
| 65596518 1F3.0 | 56425.5 cm-1 |
| 65596518 1D2.0 | 56908.0 cm-1 |
| 65596518 3D3.0 | 57306.4 cm-1 |
| 65596518 3D1.0 | 58359.7 cm-1 |
| 65596518 3D2.0 | 58612.2 cm-1 |
| 65596518 1P1.0 | 58767.7 cm-1 |
| 65596519 3S1.0 | 99014.3 cm-1 |
| 65596519 3G5.0 | 99630.6 cm-1 |
| 65596519 3G4.0 | 99705.2 cm-1 |
| 65596519 1P1.0 | 99717.2 cm-1 |
| 65596519 3P2.0 | 99738.0 cm-1 |
| 65596519 3D3.0 | 100039.0 cm-1 |
| 65596519 1F3.0 | 100234.0 cm-1 |
| 65596519 3F4.0 | 100276.0 cm-1 |
| 65596519 1D2.0 | 100279.0 cm-1 |
| 65596519 3P0.0 | 100713.0 cm-1 |
| 65596519 3P1.0 | 101317.0 cm-1 |
| 65596519 3G3.0 | 101662.0 cm-1 |
| 65596519 1G4.0 | 101764.0 cm-1 |
| 65596519 3D1.0 | 101818.0 cm-1 |
| 65596519 3D2.0 | 101991.0 cm-1 |
| 65596519 3F3.0 | 102247.0 cm-1 |
| 65596519 3F2.0 | 102299.0 cm-1 |
| 65596519 1S0.0 | 111647.0 cm-1 |
U+ 1 29 2 171402.5 -------------------------------------------------------------------------------- Configuration Eissner == Standard R % Parentage 1 65606 == 3P6 3DA 98 1 1S 1S/ 2 65596517 == 3P6 3D9 4S1 100 1 2D 2D/ 1 2S 3D/ 3 65596517 == 3P6 3D9 4S1 90 1 2D 2D/ 1 2S 3D/ 4 65596517 == 3P6 3D9 4S1 100 1 2D 2D/ 1 2S 3D/ 5 65596517 == 3P6 3D9 4S1 90 1 2D 2D/ 1 2S 1D/ 6 65596518 == 3P6 3D9 4P1 98 1 2D 2D/ 1 2P 3P/ 7 65596518 == 3P6 3D9 4P1 96 1 2D 2D/ 1 2P 3P/ 8 65596518 == 3P6 3D9 4P1 70 1 2D 2D/ 1 2P 3F/ 9 65596518 == 3P6 3D9 4P1 100 1 2D 2D/ 1 2P 3F/ 10 65596518 == 3P6 3D9 4P1 100 1 2D 2D/ 1 2P 3P/ 11 65596518 == 3P6 3D9 4P1 90 1 2D 2D/ 1 2P 3F/ 12 65596518 == 3P6 3D9 4P1 51 1 2D 2D/ 1 2P 1F/ 13 65596518 == 3P6 3D9 4P1 59 1 2D 2D/ 1 2P 1D/ 14 65596518 == 3P6 3D9 4P1 60 1 2D 2D/ 1 2P 3D/ 15 65596518 == 3P6 3D9 4P1 83 1 2D 2D/ 1 2P 3D/ 16 65596518 == 3P6 3D9 4P1 61 1 2D 2D/ 1 2P 3D/ 17 65596518 == 3P6 3D9 4P1 84 1 2D 2D/ 1 2P 1P/ 18 65596519 == 3P6 3D9 4D1 78 1 2D 2D/ 1 2D 3S/ 19 65596519 == 3P6 3D9 4D1 100 1 2D 2D/ 1 2D 3G/ 20 65596519 == 3P6 3D9 4D1 52 1 2D 2D/ 1 2D 3G/ 21 65596519 == 3P6 3D9 4D1 52 1 2D 2D/ 1 2D 1P/ 22 65596519 == 3P6 3D9 4D1 74 1 2D 2D/ 1 2D 3P/ 23 65596519 == 3P6 3D9 4D1 85 1 2D 2D/ 1 2D 3D/ 24 65596519 == 3P6 3D9 4D1 47 1 2D 2D/ 1 2D 1F/ 25 65596519 == 3P6 3D9 4D1 81 1 2D 2D/ 1 2D 3F/ 26 65596519 == 3P6 3D9 4D1 46 1 2D 2D/ 1 2D 1D/ 27 65596519 == 3P6 3D9 4D1 99 1 2D 2D/ 1 2D 3P/ 28 65596519 == 3P6 3D9 4D1 51 1 2D 2D/ 1 2D 3P/ 29 65596519 == 3P6 3D9 4D1 79 1 2D 2D/ 1 2D 3G/ 30 65596519 == 3P6 3D9 4D1 * 40 1 2D 2D/ 1 2D 1G/ 31 65596519 == 3P6 3D9 4D1 77 1 2D 2D/ 1 2D 3D/ 32 65596519 == 3P6 3D9 4D1 45 1 2D 2D/ 1 2D 3D/ 33 65596519 == 3P6 3D9 4D1 49 1 2D 2D/ 1 2D 3F/ 34 65596519 == 3P6 3D9 4D1 73 1 2D 2D/ 1 2D 3F/ 35 65596519 == 3P6 3D9 4D1 98 1 2D 2D/ 1 2D 1S/ (R) - Levels (or levels within a term) have been reassigned from their principal component. -------------------------------------------------------------------------------- Generated from Cowan Atomic Structure Program From IFG file : ./ifg#cu29-01_adf34.dat Options in effect Coupling Avalue numtemps Lweight Isonuclear Comment Level IC YES 14 NO YES 2 Cowan code options ------------------ Cowan plane wave Born method Scale factors 75 95 75 75 75 Parity 1 Parity 2 Allowed 180 55 162 initially 180 55 162 reduced Note: The Born method does NOT calculate spin changing transitions correctly. You should supplement for important transitions of this type. -------------------------------------------------------------------------------- Code : ADAS801 Producer : Martin O'Mullane Date : 16/12/04 --------------------------------------------------------------------------------