lilike_dcg00#o5ls.dat
Resolved Specific Ion Data Collections
- Ion
- O5+
- Temperature Range
- 3.102 eV → 620 eV
ADF04
- Filename
- lilike_dcg00#o5ls.dat
- Full Path
- adf04/lilike/lilike_dcg00#o5ls.dat
Download data
- Spontaneous Emission: O+5(i) → O+5(j) + hv
- Electron Impact Excitation: O+5(i) + e → O+5(j) + e
| 1s22s(2s) 2S0.5 | 0.0 cm-1 |
| 1s22p(2p) 2P2.5 | 96914.0 cm-1 |
| 1s23s(2s) 2S0.5 | 638685.0 cm-1 |
| 1s23p(2p) 2P2.5 | 664879.0 cm-1 |
| 1s23d(2d) 2D4.5 | 672931.0 cm-1 |
| 1s24s(2s) 2S0.5 | 851024.0 cm-1 |
| 1s24p(2p) 2P2.5 | 861696.0 cm-1 |
| 1s24d(2d) 2D4.5 | 865067.0 cm-1 |
| 1s24f(2f) 2F6.5 | 865191.0 cm-1 |
------------------------------------------------------------------------------- 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. The continuum basis for these calculations was set to 38 and the radius of the R-matrix box was 13.96 a.u. Donald C. Griffin May 18, 2000 ------------------------------------------------------------------------------- --------------------------------------------------------------------------------- ---------------------------------------------------------------------------------