lilike_dcg01#li0.dat
Resolved Specific Ion Data Collections
- Ion
- Li0+
- Temperature Range
- 0.086 eV → 8.617 eV
ADF04
- Filename
- lilike_dcg01#li0.dat
- Full Path
- adf04/lilike/lilike_dcg01#li0.dat
Download data
- Spontaneous Emission: Li+0(i) → Li+0(j) + hv
- Electron Impact Excitation: Li+0(i) + e → Li+0(j) + e
| 2s(2s) 2S0.5 | 0.0 cm-1 |
| 2p(2p) 2P2.5 | 14850.0 cm-1 |
| 3s(2s) 2S0.5 | 26890.0 cm-1 |
| 3p(2p) 2P2.5 | 30626.0 cm-1 |
| 3d(2d) 2D4.5 | 30893.0 cm-1 |
| 4s(2s) 2S0.5 | 34643.0 cm-1 |
| 4p(2p) 2P2.5 | 36112.0 cm-1 |
| 4d(2d) 2D4.5 | 36228.0 cm-1 |
| 4f(2f) 2F6.5 | 36229.0 cm-1 |
Dependents
Contributors
- Don Griffin
- James Colgan
- Allan Whiteford
------------------------------------------------------------------------------- For more information see: D. C. Griffin, D. M. Mitnik, J. Colgan, and M. S. Pindzola, Phys. Rev. A 64 032718 (2001) From a 55-state R-matrix with pseudo-state (RMPS) calculation The 1s and 2s orbitals were determined from a Hartree-Fock (HF) calculation on 1s22s. The 2p, 3s, 3p, 3d, 4s, 4p, 4d, and 4f orbitals were determined from a frozen-core HF calculation on 1s2nl. In addition, we generated 1s2nl pseudo states for: ns with n=6 to 15, np with n=6 to 14, nd with n=6 to 13, nf with n=6 to 12, and ng with n=6 to 12 using Laguerre orbitals. These were used to represent the target continuum as well as the highly excited Rydberg states. For the RMPS calculation with exchange, all partial LSPI partial waves from L = 0 to L = 9 were included. This was then extended to higher L values by adding to it the results of a no-exchange 9-state R-matrix calculation from L=10 to L=60 with top up. The size of the continuum basis for these calculations was 36 and the size of the R-matrix box was 77.3 au. Donald C. Griffin December, 2 2001 Update: Changed format of first line from "Li 0" to "Li+ 0" Allan Whiteford, August 17 2006 ------------------------------------------------------------------------------- --------------------------------------------------------------------------------- ---------------------------------------------------------------------------------