qef93#h_o8.dat
Charge Exchange Effective Emission Coefficients
- Ion
- O8+
- Temperature Range
- 1000 eV → 3.000 x 104 eV
- Density Range
- 1.000 x 1011 cm-3 → 1.000 x 1014 cm-3
- Energy Range
- 1000 eV → 3.000 x 105 eV
- Mag Field Range
- 3 T → 3 T
- Zeff Range
- 1 → 6
ADF12
- Filename
- qef93#h_o8.dat
- Full Path
- adf12/qef93#h/qef93#h_o8.dat
Download data
| Wavelength | Transition |
|---|
| 200.2Å | 5 → 3 |
| 410Å | 6 → 4 |
| 632.7Å | 5 → 4 |
| 726.7Å | 7 → 5 |
| 1164.8Å | 6 → 5 |
| 1171.6Å | 8 → 6 |
| 1766Å | 9 → 7 |
| 1931.9Å | 7 → 6 |
| 2530.6Å | 10 → 8 |
| 2975.9Å | 8 → 7 |
| 3487.9Å | 11 → 9 |
| 4340.7Å | 9 → 8 |
| 4658.7Å | 12 → 10 |
| 6068.5Å | 10 → 9 |
| 8202Å | 11 → 10 |
| 10783.9Å | 12 → 11 |
----------------------------------------------------------------------- EFFECTIVE COEFFICIENT LIST: ISEL TYPE ION INFORMATION ---- ---- --- ----------- 1. CX.EMIS. O + 7 N = 5 - 4 632.7 23/2/94 J1548 2. CX.EMIS. O + 7 N = 6 - 5 1164.8 23/2/94 J1548 3. CX.EMIS. O + 7 N = 7 - 6 1931.9 23/2/94 J1548 4. CX.EMIS. O + 7 N = 8 - 7 2975.9 23/2/94 J1548 5. CX.EMIS. O + 7 N = 9 - 8 4340.7 23/2/94 J1548 6. CX.EMIS. O + 7 N =10 - 9 6068.5 23/2/94 J1548 7. CX.EMIS. O + 7 N =11 - 10 8202.0 23/2/94 J1548 8. CX.EMIS. O + 7 N =12 - 11 10783.9 23/2/94 J1548 9. CX.EMIS. O + 7 N = 5 - 3 200.2 23/2/94 J1548 10. CX.EMIS. O + 7 N = 6 - 4 410.0 23/2/94 J1548 11. CX.EMIS. O + 7 N = 7 - 5 726.7 23/2/94 J1548 12. CX.EMIS. O + 7 N = 8 - 6 1171.6 22/2/94 J1548 13. CX.EMIS. O + 7 N = 9 - 7 1766.0 22/2/94 J1548 14. CX.EMIS. O + 7 N =10 - 8 2530.6 22/2/94 J1548 15. CX.EMIS. O + 7 N =11 - 9 3487.9 22/2/94 J1548 16. CX.EMIS. O + 7 N =12 - 10 4658.7 22/2/94 J1548 ----------------------------------------------------------------------- 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 --------------------------------------------------------------------------------- ---------------------------------------------------------------------------------