qef97#li_kvi#b5.dat
Charge Exchange Effective Emission Coefficients
- Ion
- B5+
- Temperature Range
- 100 eV → 3000 eV
- Density Range
- 1.000 x 1011 cm-3 → 1.000 x 1014 cm-3
- Energy Range
- 1000 eV → 1.000 x 104 eV
- Mag Field Range
- 3 T → 3 T
- Zeff Range
- 1 → 6
ADF12
- Filename
- qef97#li_kvi#b5.dat
- Full Path
- adf12/qef97#li/qef97#li_kvi#b5.dat
Download data
| Wavelength | Transition |
|---|
| 50Å | 3 → 1 |
| 194.3Å | 4 → 2 |
| 262.3Å | 3 → 2 |
| 512.5Å | 5 → 3 |
| 749.7Å | 4 → 3 |
| 1049.7Å | 6 → 4 |
| 1619.9Å | 5 → 4 |
| 1860.4Å | 7 → 5 |
| 2981.4Å | 6 → 5 |
| 2998.6Å | 8 → 6 |
| 4519.9Å | 9 → 7 |
| 4944.7Å | 7 → 6 |
| 7618.6Å | 8 → 7 |
| 11112.5Å | 9 → 8 |
Predecessors
Contributors
- Kernfysisch Versneller Instituut
- Hugh Summers
- Martin O'Mullane
----------------------------------------------------------------------- EFFECTIVE COEFFICIENT LIST: ISEL TYPE ION INFORMATION ---- ---- --- ----------- 1. CX.EMIS. B + 4 N = 3 - 2 262.3 20/6/97 2. CX.EMIS. B + 4 N = 4 - 3 749.7 20/6/97 3. CX.EMIS. B + 4 N = 5 - 4 1619.9 20/6/97 4. CX.EMIS. B + 4 N = 6 - 5 2981.4 20/6/97 5. CX.EMIS. B + 4 N = 7 - 6 4944.7 20/6/97 6. CX.EMIS. B + 4 N = 8 - 7 7618.6 20/6/97 7. CX.EMIS. B + 4 N = 9 - 8 11112.5 20/6/97 8. CX.EMIS. B + 4 N = 3 - 1 50.0 20/6/97 9. CX.EMIS. B + 4 N = 4 - 2 194.3 20/6/97 10. CX.EMIS. B + 4 N = 5 - 3 512.5 20/6/97 11. CX.EMIS. B + 4 N = 6 - 4 1049.7 20/6/97 12. CX.EMIS. B + 4 N = 7 - 5 1860.4 20/6/97 13. CX.EMIS. B + 4 N = 8 - 6 2998.6 20/6/97 14. CX.EMIS. B + 4 N = 9 - 7 4519.9 20/6/97 ----------------------------------------------------------------------- Donor: li0(2s) Production code: ADAS309 Source data set: /packages/adas/adf01/qcx#li0/qcx#li0_kvi#be4.dat Producer: H. P. Summers Date: 20 June 1997 Update: ----------------------------------------------------------------------- Replace QZEFF data. The previous version only changed on integral Z which leads to problems in interpolation as the file contains fractional Zeff. AUTHOR : Martin O'Mullane DATE : 10/10/05 --------------------------------------------------------------------------------- ---------------------------------------------------------------------------------