hlike_cpb03#be3.dat
Resolved Specific Ion Data Collections
- Ion
- Be3+
- Temperature Range
- 1.723 eV → 431 eV
ADF04
- Filename
- hlike_cpb03#be3.dat
- Full Path
- adf04/hlike/hlike_cpb03#be3.dat
Download data
- Spontaneous Emission: Be+3(i) → Be+3(j) + hv
- Electron Impact Excitation: Be+3(i) + e → Be+3(j) + e
| 1s1 2S0.5 | 0.0 cm-1 |
| 2s1 2S0.5 | 1316850.0 cm-1 |
| 2p1 2P2.5 | 1316850.0 cm-1 |
| 3s1 2S0.5 | 1560710.0 cm-1 |
| 3p1 2P2.5 | 1560710.0 cm-1 |
| 3d1 2D4.5 | 1560710.0 cm-1 |
| 4s1 2S0.5 | 1646060.0 cm-1 |
| 4p1 2P2.5 | 1646060.0 cm-1 |
| 4d1 2D4.5 | 1646060.0 cm-1 |
| 4f1 2F6.5 | 1646060.0 cm-1 |
Dependents
Contributors
- Connor Ballance
- Don Griffin
------------------------------------------------------------------------------- From a 57 term R-matrix with pseudo states (RMPS) calculation. The close-coupling expansion included the 9 spectroscopic terms arising from the configurations 1s, 2l, 3l, and 4l. In addition it, included the 48 pseudo-state terms arising from the configurations 5l with l = 0 to 4 and nl with n = 6 to 12 and l = 0 to 5. The pseudo orbitals were generated from a set of non-orthogonal Laguerre orbitals that were then orthogonalized to the spectroscopic orbitals and to each other. The screening parameters for the Laguerre orbitals were adjusted to obtain a good distribution of pseudo states above and below the ionization limit. In STG3 of the R-Matrix calculation, the term energies were adjusted to the experimental values. For all LSPI partial waves from L=0 to 11, we performed an RMPS calculation with exchange. For the LSPI partial waves from L=12 to 50, we performed a no-exchange RMPS calculation. These partial waves were then topped up. The size of the continuum basis was 51 and the size of the R-matrix "box" was 21.4 au. In the resonance region of the calculation, we used an energy mesh spacing of 5.0e-04 Ryd; above all thresholds of the 5l configurations, we employed an energy-mesh spacing of 1.4e-02 Ryd up to a total energy of 30 Ryd. Note we do not include data for transitions between degenerate levels for hydrogenic systems The numbers in the last column of the above table are the theoretical values for the reduced effective collision strengths in the infinite temperature limit as defined in Burgess and Tully Astron. Astrophys. 254 436 (1992). NAME: C Ballance and D Griffin DATE: July 22, 2003 -------------------------------------------------------------------------------