lilike_dcg00#c3ls.dat
Resolved Specific Ion Data Collections
- Ion
- C3+
- Temperature Range
- 1.379 eV → 276 eV
ADF04
- Filename
- lilike_dcg00#c3ls.dat
- Full Path
- adf04/lilike/lilike_dcg00#c3ls.dat
Download data
- Spontaneous Emission: C+3(i) → C+3(j) + hv
- Electron Impact Excitation: C+3(i) + e → C+3(j) + e
| 1s22s(2s) 2S0.5 | 0.0 cm-1 |
| 1s22p(2p) 2P2.5 | 65034.0 cm-1 |
| 1s23s(2s) 2S0.5 | 302024.0 cm-1 |
| 1s23p(2p) 2P2.5 | 319365.0 cm-1 |
| 1s23d(2d) 2D4.5 | 323873.0 cm-1 |
| 1s24s(2s) 2S0.5 | 400346.0 cm-1 |
| 1s24p(2p) 2P2.5 | 407367.0 cm-1 |
| 1s24d(2d) 2D4.5 | 409265.0 cm-1 |
| 1s24f(2f) 2F6.5 | 409321.0 cm-1 |
+ 3 6 4 520159.(1S) ------------------------------------------------------------------------------- See: Griffin D C, Badnell N R, and Pindzola M S 2000 J. Phys. B 33, 1013 for a more complete description. From a 41-state RMPS calculation that included the 9 spectroscopic terms of the configurations 1s22s, 1s22p, 1s23s, 1s23p, 1s23d, 1s24s, 1s24p, 1s24d, 1s24f; and the 32 pseudo states 1s2nl for n = 5 to 12 and l = 0 to 3 in the close-coupling expansion. The 1s and 2s orbitals were generated from a single-configuration Hartree-Fock (SCHF) calculation on 1s22s, while the 2p through 4f orbitals were generated from a SCHF calculation on the terms 1s2nl with the 1s orbital frozen. The pseudo states were generated from an non-orthogonal Laguerre basis; these states were then orthogonalized with respect to the Hartree-Fock orbitals and each other. For the L = 0 to 12 even and odd parity LSPI partial waves, we performed an R-Matrix calculation with exchange. For the higher partial waves we performed a no-exchange R-Matrix calculation for L = 13 to 60 with the long-range perturbations turned on and with topup. However, because of numerical problems for high partial waves that affected only the 2-4, 2-7, and 2-9 transitions, the NX run for these three transitions was from L = 13 to L = 30, again with long- range perturbations turned on and with topup. The continuum basis for these calculations was set to 40 and the radius of the R-matrix box was 20.76 a.u. Donald C. Griffin May 18, 2000 ------------------------------------------------------------------------------- --------------------------------------------------------------------------------- ---------------------------------------------------------------------------------