sxb96#li_pjr#li0.dat
Ionisation Per Photon Coefficients
- Ion
- Li0+
- Temperature Range
- 0.043 eV → 259 eV
- Density Range
- 10.00 cm-3 → 1.000 x 1015 cm-3
| Wavelength | Transition | Driving Population |
|---|---|---|
| 2742Å | 1s2 4p1 2P2.5 → 1s2 2s1 2S0.5 | 1s2 2s1 2S0.5 |
| 3233.6Å | 1s2 3p1 2P2.5 → 1s2 2s1 2S0.5 | 1s2 2s1 2S0.5 |
| 4604.2Å | 1s2 4d1 2D4.5 → 1s2 2p1 2P2.5 | 1s2 2s1 2S0.5 |
| 4973.1Å | 1s2 4s1 2S0.5 → 1s2 2p1 2P2.5 | 1s2 2s1 2S0.5 |
| 6105.3Å | 1s2 3d1 2D4.5 → 1s2 2p1 2P2.5 | 1s2 2s1 2S0.5 |
| 6709.7Å | 1s2 2p1 2P2.5 → 1s2 2s1 2S0.5 | 1s2 2s1 2S0.5 |
| 8128.6Å | 1s2 3s1 2S0.5 → 1s2 2p1 2P2.5 | 1s2 2s1 2S0.5 |
----------------------------------------------------------------------- IONISATION/PHOTON LIST: INFORMATION ----------- NUCLEAR CHARGE = 3 ION CHARGE +1 = 1 SPECIFIC ION FILE : /home/adas/adas/adf04/adas#3/cpb02_ls#li0.dat EXPANSION FILE : /home/adas/adas/adf18/a17_p208/exp96#li/exp96#li_li0ls.dat META. ION. COEFF. SELECTOR: *(1,1) *(1,2) * - rate from specific ion file N - no rate available OPTIONS : LNORM=F LPSEL=F LZSEL=F LIOSEL=T LHSEL=F LRSEL=T LISEL=F LNSEL =T Configuration (2S+1)L(w-1/2) Energy (cm**-1) 1 1S2 2S1 (2)0( 0.5) 0.0 2 1S2 2P1 (2)1( 2.5) 14903.9 3 1S2 3S1 (2)0( 0.5) 27206.1 4 1S2 3P1 (2)1( 2.5) 30925.4 5 1S2 3D1 (2)2( 4.5) 31283.1 6 1S2 4S1 (2)0( 0.5) 35012.1 7 1S2 4P1 (2)1( 2.5) 36469.6 8 1S2 4D1 (2)2( 4.5) 36623.4 9 1S2 4F1 (2)3( 6.5) 36630.2 POPULATION PROCESSING CODE: ADAS208 ISEL WAVELENGTH TRANSITION TYPE METASTABLE IMET NMET ---- ---------- ------------------------ ----- ------------ ---- ---- 1. 6709.7 2(2)1( 2.5)- 1(2)0( 0.5) EXCIT 1(2)0( 0.5) 1 1 2. 3233.6 4(2)1( 2.5)- 1(2)0( 0.5) EXCIT 1(2)0( 0.5) 1 1 3. 2742.0 7(2)1( 2.5)- 1(2)0( 0.5) EXCIT 1(2)0( 0.5) 1 1 4. 8128.6 3(2)0( 0.5)- 2(2)1( 2.5) EXCIT 1(2)0( 0.5) 1 1 5. 6105.3 5(2)2( 4.5)- 2(2)1( 2.5) EXCIT 1(2)0( 0.5) 1 1 6. 4973.1 6(2)0( 0.5)- 2(2)1( 2.5) EXCIT 1(2)0( 0.5) 1 1 7. 4604.2 8(2)2( 4.5)- 2(2)1( 2.5) EXCIT 1(2)0( 0.5) 1 1 CODE : ADAS208 PRODUCER : Martin O'Mullane DATE : 30/10/02 ------------------------------------------------------------------------------- --------------------------------------------------------------------------------- ---------------------------------------------------------------------------------