clike_bmf#fe20.dat
Resolved Specific Ion Data Collections
- Ion
- Fe20+
- Temperature Range
- 18.96 eV → 3.800 x 104 eV
ADF04
- Filename
- clike_bmf#fe20.dat
- Full Path
- adf04/clike/clike_bmf#fe20.dat
Download data
- Spontaneous Emission: Fe+20(i) → Fe+20(j) + hv
- Electron Impact Excitation: Fe+20(i) + e → Fe+20(j) + e
| 2s22p2 3P0.0 | 0.0 cm-1 |
| 2s22p2 3P1.0 | 73850.2 cm-1 |
| 2s22p2 3P2.0 | 117353.0 cm-1 |
| 2s22p2 1D2.0 | 244561.0 cm-1 |
| 2s22p2 1S0.0 | 371901.0 cm-1 |
| 2s2p3 5S2.0 | 486951.0 cm-1 |
| 2s2p3 3D1.0 | 776782.0 cm-1 |
| 2s2p3 3D2.0 | 777352.0 cm-1 |
| 2s2p3 3D3.0 | 803932.0 cm-1 |
| 2s2p3 3P0.0 | 916383.0 cm-1 |
| 2s2p3 3P1.0 | 924883.0 cm-1 |
| 2s2p3 3P2.0 | 942323.0 cm-1 |
| 2s2p3 3S1.0 | 1095600.0 cm-1 |
| 2s2p3 1D2.0 | 1126800.0 cm-1 |
| 2s2p3 1P1.0 | 1261000.0 cm-1 |
| 2s22p3s 3P0.0 | 7726190.0 cm-1 |
| 2s22p3s 3P1.0 | 7734910.0 cm-1 |
| 2s22p3s 3P2.0 | 7839940.0 cm-1 |
| 2s22p3s 1P1.0 | 7863120.0 cm-1 |
| 2s22p3d 3F2.0 | 8061600.0 cm-1 |
| 2s22p3d 3F3.0 | 8101420.0 cm-1 |
| 2s22p3d 1D2.0 | 8098020.0 cm-1 |
| 2s22p3d 3D1.0 | 8121800.0 cm-1 |
| 2s22p3d 3F4.0 | 8189600.0 cm-1 |
| 2s22p3d 3D2.0 | 8187420.0 cm-1 |
| 2s22p3d 3D3.0 | 8195020.0 cm-1 |
| 2s22p3d 3P2.0 | 8230920.0 cm-1 |
| 2s22p3d 3P1.0 | 8232300.0 cm-1 |
| 2s22p3d 3P0.0 | 8234400.0 cm-1 |
| 2s22p3d 1F3.0 | 8313620.0 cm-1 |
| 2s22p3d 1P1.0 | 8293920.0 cm-1 |
| 1s22p4 3P2.0 | 1646300.0 cm-1 |
| 1s22p4 3P1.0 | 1740510.0 cm-1 |
| 1s22p4 3P0.0 | 1735710.0 cm-1 |
| 1s22p4 1D2.0 | 1817300.0 cm-1 |
| 1s22p4 1S0.0 | 2048210.0 cm-1 |
----------------------------------------------------------------------------- Description of the above data set: Ionization potential from: NIST Database for Atomic Spectroscopy Version 1.0 Observed energy levels, collision strengths and radiative probabilities up to 2s22p3d from: Mason H E, Doschek G A, Feldman U, Bhatia A K, 1979, A&A, 73, 74 Observed energies and collision strengths for transition with 1s22p4 from: Aggarwal K M, 1991, ApJ SS, 77, 677 Data set produced :- Mon Oct 23 13:32:57 BST ----------------------------------------------------------------------------- --------------------------------------------------------------------------------- ---------------------------------------------------------------------------------