lilike_lgy10#c3.dat
Resolved Specific Ion Data Collections
- Ion
- C3+
- Temperature Range
- 0.276 eV → 2757 eV
ADF04
- Filename
- lilike_lgy10#c3.dat
- Full Path
- adf04/copaw#li/lilike_lgy10#c3.dat
Download data
- Spontaneous Emission: C+3(i) → C+3(j) + hv
- Electron Impact Excitation: C+3(i) + e → C+3(j) + e
| 2s1 2S0.5 | 0.0 cm-1 |
| 2p1 2P0.5 | 65100.0 cm-1 |
| 2p1 2P1.5 | 65203.0 cm-1 |
| 3s1 2S0.5 | 302235.0 cm-1 |
| 3p1 2P0.5 | 319564.0 cm-1 |
| 3p1 2P1.5 | 319594.0 cm-1 |
| 3d1 2D1.5 | 324121.0 cm-1 |
| 3d1 2D2.5 | 324130.0 cm-1 |
| 4s1 2S0.5 | 400575.0 cm-1 |
| 4p1 2P0.5 | 407602.0 cm-1 |
| 4p1 2P1.5 | 407615.0 cm-1 |
| 4d1 2D1.5 | 409521.0 cm-1 |
| 4d1 2D2.5 | 409525.0 cm-1 |
| 4f1 2F2.5 | 409580.0 cm-1 |
| 4f1 2F3.5 | 409582.0 cm-1 |
| 5s1 2S0.5 | 444553.0 cm-1 |
| 5p1 2P0.5 | 448073.0 cm-1 |
| 5p1 2P1.5 | 448079.0 cm-1 |
| 5d1 2D1.5 | 449053.0 cm-1 |
| 5d1 2D2.5 | 449055.0 cm-1 |
| 5f1 2F2.5 | 449087.0 cm-1 |
| 5f1 2F3.5 | 449088.0 cm-1 |
| 5g1 2G3.5 | 449088.0 cm-1 |
| 5g1 2G4.5 | 449089.0 cm-1 |
| 1s1 2s2 2S0.5 | 2363520.0 cm-1 |
| 1s1 2s1 2p1 4P0.5 | 2386850.0 cm-1 |
| 1s1 2s1 2p1 4P1.5 | 2386890.0 cm-1 |
| 1s1 2s1 2p1 4P2.5 | 2386950.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 2430850.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 2430900.0 cm-1 |
| 1s1 2p2 4P0.5 | 2462940.0 cm-1 |
| 1s1 2p2 4P1.5 | 2462980.0 cm-1 |
| 1s1 2p2 4P2.5 | 2463040.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 2467420.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 2467450.0 cm-1 |
| 1s1 2p2 2D1.5 | 2491650.0 cm-1 |
| 1s1 2p2 2D2.5 | 2491660.0 cm-1 |
| 1s1 2p2 2P0.5 | 2496070.0 cm-1 |
| 1s1 2p2 2P1.5 | 2496150.0 cm-1 |
| 1s1 2p2 2S0.5 | 2546020.0 cm-1 |
| 1s1 2s1 3s1 4S1.5 | 2707700.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 2726020.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 2732140.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 2732150.0 cm-1 |
| 1s1 2s1 3p1 4P0.5 | 2733840.0 cm-1 |
| 1s1 2s1 3p1 4P1.5 | 2733850.0 cm-1 |
| 1s1 2s1 3p1 4P2.5 | 2733860.0 cm-1 |
| 1s1 2s1 3d1 4D0.5 | 2744260.0 cm-1 |
| 1s1 2s1 3d1 4D1.5 | 2744270.0 cm-1 |
| 1s1 2s1 3d1 4D2.5 | 2744270.0 cm-1 |
| 1s1 2s1 3d1 4D3.5 | 2744280.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 2750180.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 2753000.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 2753000.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 2766800.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 2766820.0 cm-1 |
| 1s1 2p1 3s1 4P0.5 | 2771710.0 cm-1 |
| 1s1 2p1 3s1 4P1.5 | 2771740.0 cm-1 |
| 1s1 2p1 3s1 4P2.5 | 2771800.0 cm-1 |
| 1s1 2p1 3p1 4D0.5 | 2779700.0 cm-1 |
| 1s1 2p1 3p1 4D1.5 | 2779720.0 cm-1 |
| 1s1 2p1 3p1 4D2.5 | 2779760.0 cm-1 |
| 1s1 2p1 3p1 4D3.5 | 2779810.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 2780020.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 2780030.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 2782020.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 2782040.0 cm-1 |
| 1s1 2p1 3p1 4S1.5 | 2786680.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 2787720.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 2787810.0 cm-1 |
| 1s1 2p1 3d1 4F1.5 | 2791760.0 cm-1 |
| 1s1 2p1 3d1 4F2.5 | 2791780.0 cm-1 |
| 1s1 2p1 3d1 4F3.5 | 2791810.0 cm-1 |
| 1s1 2p1 3d1 4F4.5 | 2791850.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 2794650.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 2794660.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 2796870.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 2796960.0 cm-1 |
| 1s1 2p1 3p1 4P0.5 | 2797520.0 cm-1 |
| 1s1 2p1 3p1 4P1.5 | 2797540.0 cm-1 |
| 1s1 2p1 3p1 4P2.5 | 2797570.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 2797870.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 2797890.0 cm-1 |
| 1s1 2p1 3d1 4D0.5 | 2802610.0 cm-1 |
| 1s1 2p1 3d1 4D1.5 | 2802620.0 cm-1 |
| 1s1 2p1 3d1 4D2.5 | 2802630.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 2802630.0 cm-1 |
| 1s1 2p1 3d1 4D3.5 | 2802640.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 2802710.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 2804640.0 cm-1 |
| 1s1 2p1 3d1 4P2.5 | 2806150.0 cm-1 |
| 1s1 2p1 3d1 4P1.5 | 2806180.0 cm-1 |
| 1s1 2p1 3d1 4P0.5 | 2806190.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 2814990.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 2815040.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 2815350.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 2815380.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 2815430.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 2815450.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 2820770.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 2820780.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 2823630.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 2823640.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 2824020.0 cm-1 |
| 1s1 2s1 4s1 4S1.5 | 2826320.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 2832570.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 2832580.0 cm-1 |
| 1s1 2s1 4p1 4P0.5 | 2834550.0 cm-1 |
| 1s1 2s1 4p1 4P1.5 | 2834550.0 cm-1 |
| 1s1 2s1 4p1 4P2.5 | 2834560.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 2835340.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 2838190.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 2838190.0 cm-1 |
| 1s1 2s1 4d1 4D0.5 | 2838280.0 cm-1 |
| 1s1 2s1 4d1 4D1.5 | 2838280.0 cm-1 |
| 1s1 2s1 4d1 4D2.5 | 2838280.0 cm-1 |
| 1s1 2s1 4d1 4D3.5 | 2838280.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 2841150.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 2841150.0 cm-1 |
| 1s1 2s1 4f1 4F1.5 | 2842500.0 cm-1 |
| 1s1 2s1 4f1 4F2.5 | 2842510.0 cm-1 |
| 1s1 2s1 4f1 4F3.5 | 2842510.0 cm-1 |
| 1s1 2s1 4f1 4F4.5 | 2842510.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 2845530.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 2845530.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 2863070.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 2869730.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 2869740.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 2874290.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 2874290.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 2877930.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 2877940.0 cm-1 |
| 1s1 2p1 4s1 4P0.5 | 2879840.0 cm-1 |
| 1s1 2p1 4s1 4P1.5 | 2879870.0 cm-1 |
| 1s1 2p1 4s1 4P2.5 | 2879930.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 2884240.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 2884300.0 cm-1 |
| 1s1 2p1 4p1 4D0.5 | 2885080.0 cm-1 |
| 1s1 2p1 4p1 4D1.5 | 2885100.0 cm-1 |
| 1s1 2p1 4p1 4D2.5 | 2885130.0 cm-1 |
| 1s1 2p1 4p1 4D3.5 | 2885170.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 2885800.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 2885830.0 cm-1 |
| 1s1 2p1 4p1 4S1.5 | 2887140.0 cm-1 |
| 1s1 2p1 4p1 4P0.5 | 2888130.0 cm-1 |
| 1s1 2p1 4p1 4P1.5 | 2888150.0 cm-1 |
| 1s1 2p1 4p1 4P2.5 | 2888180.0 cm-1 |
| 1s1 2p1 4d1 4F1.5 | 2889100.0 cm-1 |
| 1s1 2p1 4d1 4F2.5 | 2889130.0 cm-1 |
| 1s1 2p1 4d1 4F3.5 | 2889150.0 cm-1 |
| 1s1 2p1 4d1 4F4.5 | 2889190.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 2889290.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 2889310.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 2890340.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 2890400.0 cm-1 |
| 1s1 2p1 4d1 4D0.5 | 2891100.0 cm-1 |
| 1s1 2p1 4d1 4D1.5 | 2891100.0 cm-1 |
| 1s1 2p1 4d1 4D2.5 | 2891110.0 cm-1 |
| 1s1 2p1 4d1 4D3.5 | 2891130.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 2891740.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 2891760.0 cm-1 |
| 1s1 2p1 4f1 4F1.5 | 2891930.0 cm-1 |
| 1s1 2p1 4f1 4F2.5 | 2891930.0 cm-1 |
| 1s1 2p1 4f1 4F3.5 | 2891940.0 cm-1 |
| 1s1 2p1 4f1 4F4.5 | 2891950.0 cm-1 |
| 1s1 2p1 4d1 4P2.5 | 2892440.0 cm-1 |
| 1s1 2p1 4d1 4P1.5 | 2892470.0 cm-1 |
| 1s1 2p1 4d1 4P0.5 | 2892480.0 cm-1 |
| 1s1 2p1 4f1 4G2.5 | 2893330.0 cm-1 |
| 1s1 2p1 4f1 4G3.5 | 2893350.0 cm-1 |
| 1s1 2p1 4f1 4G4.5 | 2893380.0 cm-1 |
| 1s1 2p1 4f1 4G5.5 | 2893410.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 2894230.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 2894280.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 2894570.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 2894640.0 cm-1 |
| 1s1 2p1 4f1 4D3.5 | 2895100.0 cm-1 |
| 1s1 2p1 4f1 4D2.5 | 2895120.0 cm-1 |
| 1s1 2p1 4f1 4D1.5 | 2895140.0 cm-1 |
| 1s1 2p1 4f1 4D0.5 | 2895150.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 2895580.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 2896130.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 2896160.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 2896600.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 2896640.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 2901100.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 2901100.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 2907260.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 2907270.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 2907380.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 2907390.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 2910420.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 2910420.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 2911060.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 2911520.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 2911530.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 2911730.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 2911730.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 2913540.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 2913540.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 2914320.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 2914330.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 2915410.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 2915410.0 cm-1 |
Contributors
- Guiyun Liang
- Nigel Badnell
+ 3 6 4 520179.( ) ------------------------------------------------------------------------ Result of ICFT R-matrix calculation for outer shell excitation +++++++++++++++++++++++++++++++++++ Calculation automated by offline ADAS code ADAS8#3 Summary Information +++++++++++++++++++ * Ionisation energy taken from ADAS adf00 files * Energy levels calculated by AUTOSTRUCTURE * Radiative rates calculated by AUTOSTRUCTURE * Effective collision strengths calculated by ICFT R-matrix calculation using target structure from AUTOSTRUCTURE. Calculation details +++++++++++++++++++ The following scaling parameters on bound orbitals were used: 1S = 1.27206 2S = 0.99491 2P = 0.86843 3S = 1.08212 3P = 0.86491 3D = 0.78754 4S = 0.98466 4P = 0.86479 4D = 0.78918 4F = 0.01715 5S = 0.98531 5P = 0.86651 5D = 0.79200 5F = 0.76894 5G = 1.00000 An exchange calculation was performed up to J=10 A non-exchange calculation was then performed up to J=40 Followed by a top-up calculation to J -> infinity. 65 continuum basis orbitals were used, giving a smallest maximum basis-orbital energy of 65.7840 Rydbergs (895.057104 eV) A fine energy mesh of 0.000010 Z**2 Rydbergs (0.00122454 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (1.22454 eV) was used from the last threshold up to 5.266794 Z**2 Rydbergs (644.94 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (1.22454 eV) was used from first threshold up to 5.266794 Z**2 Rydbergs (644.94 eV) in the non-exchange calculation. Dipole and Born limits were used from the last calculated energy points up to infinite energy to complete the effective collision strengths Produced by: Guiyun Liang Date: 15/10/10 ------------------------------------------------------------------------ Result of ICFT R-matrix calculation for core-excitation G.Y. Liang, and N.R. Badnell, A&A (2010) +++++++++++++++++++++++++++++++++++ Calculation automated by offline ADAS code ADAS8#3 Summary Information +++++++++++++++++++ * Ionisation energy taken from ADAS adf00 files * Energy levels calculated by AUTOSTRUCTURE * Radiative rates calculated by AUTOSTRUCTURE * Effective collision strengths calculated by ICFT R-matrix calculation using target structure from AUTOSTRUCTURE. Calculation details +++++++++++++++++++ The following scaling parameters on bound orbitals were used: 1S = 1.27403 2S = 0.99759 2P = 0.87379 3S = 0.98723 3P = 0.86670 3D = 0.79331 4S = 0.98706 4P = 0.86760 4D = 0.79895 4F = 0.86160 An exchange calculation was performed up to J=10 A non-exchange calculation was then performed up to J=40 Followed by a top-up calculation to J -> infinity. 46 continuum basis orbitals were used, giving a smallest maximum basis-orbital energy of 67.8774 Rydbergs (923.539904 eV) A fine energy mesh of 0.000040 Z**2 Rydbergs (0.00489816 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (1.22454 eV) was used from the last threshold up to 5.266794 Z**2 Rydbergs (644.94 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (1.22454 eV) was used from first threshold up to 5.266794 Z**2 Rydbergs (644.94 eV) in the non-exchange calculation. Dipole and Born limits were used from the last calculated energy points up to infinite energy to complete the effective collision strengths NIST v4 energy (Ryd) 2 0.587621 3 0.588603 4 2.759763 5 2.916511 6 2.916799 7 2.960523 8 2.960618 9 3.657353 10 3.720805 11 3.720924 12 3.739258 13 3.739294 14 3.740152 15 3.740152 16 4.058496 17 4.090275 18 4.090340 19 4.099683 20 4.099698 21 4.100153 22 4.100153 23 4.100232 24 4.100232 Produced by: Guiyun Liang Date: 06/09/10 ------------------------------------------------------------------------