coppm#li_pm#c3j.dat
Resolved Specific Ion Data Collections
- Ion
- C3+
- Temperature Range
- 0.689 eV → 1379 eV
ADF04
- Filename
- coppm#li_pm#c3j.dat
- Full Path
- adf04/coppm#li/coppm#li_pm#c3j.dat
Download data
- Spontaneous Emission: C+3(i) → C+3(j) + hv
- Electron Impact Excitation: C+3(i) + e → C+3(j) + e
| 2s1 2S0.5 | 0.0 cm-1 |
| 2p1 2P0.5 | 64484.0 cm-1 |
| 2p1 2P1.5 | 64591.1 cm-1 |
| 3s1 2S0.5 | 302849.0 cm-1 |
| 3p1 2P0.5 | 320050.0 cm-1 |
| 3p1 2P1.5 | 320082.0 cm-1 |
| 3d1 2D1.5 | 324880.0 cm-1 |
| 3d1 2D2.5 | 324890.0 cm-1 |
| 4s1 2S0.5 | 401348.0 cm-1 |
| 4p1 2P0.5 | 408311.0 cm-1 |
| 4p1 2P1.5 | 408324.0 cm-1 |
| 4d1 2D1.5 | 410336.0 cm-1 |
| 4d1 2D2.5 | 410340.0 cm-1 |
| 4f1 2F2.5 | 410434.0 cm-1 |
| 4f1 2F3.5 | 410434.0 cm-1 |
Dependents
Contributors
- Hong Zhang
- Martin O'Mullane
+ 3 6 4 520178.4 ----------------------------------------------------------------------------- The values of Upsilon for the n=2 to n=2, n=2 to n=3 and n=2 to n=4 transitions come from Burke's 1992 paper. The published values of Upsilon were processed through the OMEUPS procedure of Burgess and Tully using values of excitation potentials from Kelly's wavelength tables (1987) and, for allowed transitions, the f-values of Wiese et al.(1966). The Upsilon values are divided among the fine structure components of the multiplets in the same proportion as the corresponding values for O VI (Zhang et al.1990) at the same values of the reduced temperature Z*Z*T where Z=4 for C IV and 6 for O VI. The values of the transition probabilities are from Wiese et al.(1966) and were divided among the multiplet components using the formulae given in White's Introduction to Atomic Spectra p205. Transitions between higher levels were calculated on the impact parameter approximation. ---------------------------------------------------------------------- IMPACT PARAMETER DATA FOR C+3 GENERATED FROM SUPERSTRUCTURE OUTPUT 'JETXLE.UCL89OUT.CDATA(SS#C3J)' WJD/PM 14TH JANUARY 1994 ---------------------------------------------------------------------- The excitation and ionization potentials were taken from Kelly (1987). ------------------------------------------------------------------------------ Make comments conform to adf04 specification. Martin O'Mullane, 04-11-2010 ------------------------------------------------------------------------------ --------------------------------------------------------------------------------- ---------------------------------------------------------------------------------