lilike_lgy10#se31.dat
Resolved Specific Ion Data Collections
- Ion
- Se31+
- Temperature Range
- 17.66 eV → 1.766 x 105 eV
ADF04
- Filename
- lilike_lgy10#se31.dat
- Full Path
- adf04/copaw#li/lilike_lgy10#se31.dat
Download data
- Spontaneous Emission: Se+31(i) → Se+31(j) + hv
- Electron Impact Excitation: Se+31(i) + e → Se+31(j) + e
| 2s1 2S0.5 | 0.0 cm-1 |
| 2p1 2P0.5 | 536279.0 cm-1 |
| 2p1 2P1.5 | 937115.0 cm-1 |
| 3s1 2S0.5 | 16472900.0 cm-1 |
| 3p1 2P0.5 | 16621100.0 cm-1 |
| 3p1 2P1.5 | 16735700.0 cm-1 |
| 3d1 2D1.5 | 16796100.0 cm-1 |
| 3d1 2D2.5 | 16834100.0 cm-1 |
| 4s1 2S0.5 | 22154500.0 cm-1 |
| 4p1 2P0.5 | 22215400.0 cm-1 |
| 4p1 2P1.5 | 22262000.0 cm-1 |
| 4d1 2D1.5 | 22286900.0 cm-1 |
| 4d1 2D2.5 | 22302800.0 cm-1 |
| 4f1 2F2.5 | 22304200.0 cm-1 |
| 4f1 2F3.5 | 22312200.0 cm-1 |
| 5s1 2S0.5 | 24762800.0 cm-1 |
| 5p1 2P0.5 | 24793500.0 cm-1 |
| 5p1 2P1.5 | 24816200.0 cm-1 |
| 5d1 2D1.5 | 24828900.0 cm-1 |
| 5d1 2D2.5 | 24836800.0 cm-1 |
| 5f1 2F2.5 | 24837600.0 cm-1 |
| 5f1 2F3.5 | 24841600.0 cm-1 |
| 5g1 2G3.5 | 24841600.0 cm-1 |
| 5g1 2G4.5 | 24844100.0 cm-1 |
| 1s1 2s2 2S0.5 | 92889900.0 cm-1 |
| 1s1 2s1 2p1 4P0.5 | 93014300.0 cm-1 |
| 1s1 2s1 2p1 4P1.5 | 93102500.0 cm-1 |
| 1s1 2s1 2p1 4P2.5 | 93396800.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 93476000.0 cm-1 |
| 1s1 2p2 4P0.5 | 93714100.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 93740400.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 93887300.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 93942700.0 cm-1 |
| 1s1 2p2 4P1.5 | 93953000.0 cm-1 |
| 1s1 2p2 4P2.5 | 94067300.0 cm-1 |
| 1s1 2p2 2P0.5 | 94212700.0 cm-1 |
| 1s1 2p2 2D1.5 | 94227000.0 cm-1 |
| 1s1 2p2 2D2.5 | 94471900.0 cm-1 |
| 1s1 2p2 2P1.5 | 94642100.0 cm-1 |
| 1s1 2p2 2S0.5 | 94813600.0 cm-1 |
| 1s1 2s1 3s1 4S1.5 | 109555000.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 109710000.0 cm-1 |
| 1s1 2s1 3p1 4P0.5 | 109747000.0 cm-1 |
| 1s1 2s1 3p1 4P1.5 | 109755000.0 cm-1 |
| 1s1 2s1 3p1 4P2.5 | 109852000.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 109858000.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 109861000.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 109939000.0 cm-1 |
| 1s1 2s1 3d1 4D0.5 | 109946000.0 cm-1 |
| 1s1 2s1 3d1 4D1.5 | 109959000.0 cm-1 |
| 1s1 2s1 3d1 4D2.5 | 109977000.0 cm-1 |
| 1s1 2p1 3s1 4P0.5 | 109979000.0 cm-1 |
| 1s1 2s1 3d1 4D3.5 | 110002000.0 cm-1 |
| 1s1 2p1 3s1 4P1.5 | 110037000.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 110055000.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 110057000.0 cm-1 |
| 1s1 2p1 3p1 4D0.5 | 110062000.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 110077000.0 cm-1 |
| 1s1 2p1 3p1 4D1.5 | 110103000.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 110143000.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 110196000.0 cm-1 |
| 1s1 2p1 3p1 4S1.5 | 110222000.0 cm-1 |
| 1s1 2p1 3p1 4P0.5 | 110246000.0 cm-1 |
| 1s1 2p1 3p1 4D2.5 | 110248000.0 cm-1 |
| 1s1 2p1 3d1 4F1.5 | 110277000.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 110295000.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 110312000.0 cm-1 |
| 1s1 2p1 3d1 4F2.5 | 110318000.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 110327000.0 cm-1 |
| 1s1 2p1 3s1 4P2.5 | 110338000.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 110367000.0 cm-1 |
| 1s1 2p1 3d1 4D2.5 | 110381000.0 cm-1 |
| 1s1 2p1 3d1 4F3.5 | 110410000.0 cm-1 |
| 1s1 2p1 3d1 4D1.5 | 110415000.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 110421000.0 cm-1 |
| 1s1 2p1 3d1 4D0.5 | 110425000.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 110442000.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 110463000.0 cm-1 |
| 1s1 2p1 3p1 4P1.5 | 110506000.0 cm-1 |
| 1s1 2p1 3p1 4P2.5 | 110534000.0 cm-1 |
| 1s1 2p1 3p1 4D3.5 | 110546000.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 110567000.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 110573000.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 110589000.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 110654000.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 110674000.0 cm-1 |
| 1s1 2p1 3d1 4F4.5 | 110692000.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 110701000.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 110705000.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 110721000.0 cm-1 |
| 1s1 2p1 3d1 4D3.5 | 110723000.0 cm-1 |
| 1s1 2p1 3d1 4P1.5 | 110739000.0 cm-1 |
| 1s1 2p1 3d1 4P0.5 | 110750000.0 cm-1 |
| 1s1 2p1 3d1 4P2.5 | 110762000.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 110776000.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 110783000.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 110792000.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 110833000.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 110857000.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 110877000.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 110901000.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 110910000.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 110933000.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 110950000.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 110978000.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 111009000.0 cm-1 |
| 1s1 2s1 4s1 4S1.5 | 115368000.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 115418000.0 cm-1 |
| 1s1 2s1 4p1 4P0.5 | 115439000.0 cm-1 |
| 1s1 2s1 4p1 4P1.5 | 115444000.0 cm-1 |
| 1s1 2s1 4p1 4P2.5 | 115479000.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 115493000.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 115498000.0 cm-1 |
| 1s1 2s1 4d1 4D0.5 | 115523000.0 cm-1 |
| 1s1 2s1 4d1 4D1.5 | 115525000.0 cm-1 |
| 1s1 2s1 4d1 4D2.5 | 115530000.0 cm-1 |
| 1s1 2s1 4d1 4D3.5 | 115540000.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 115556000.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 115559000.0 cm-1 |
| 1s1 2s1 4f1 4F1.5 | 115572000.0 cm-1 |
| 1s1 2s1 4f1 4F2.5 | 115573000.0 cm-1 |
| 1s1 2s1 4f1 4F3.5 | 115575000.0 cm-1 |
| 1s1 2s1 4f1 4F4.5 | 115581000.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 115585000.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 115586000.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 115715000.0 cm-1 |
| 1s1 2p1 4s1 4P0.5 | 115715000.0 cm-1 |
| 1s1 2p1 4p1 4D0.5 | 115757000.0 cm-1 |
| 1s1 2p1 4s1 4P1.5 | 115761000.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 115775000.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 115792000.0 cm-1 |
| 1s1 2p1 4p1 4D1.5 | 115800000.0 cm-1 |
| 1s1 2p1 4p1 4S1.5 | 115819000.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 115821000.0 cm-1 |
| 1s1 2p1 4p1 4P0.5 | 115843000.0 cm-1 |
| 1s1 2p1 4d1 4F1.5 | 115844000.0 cm-1 |
| 1s1 2p1 4p1 4D2.5 | 115856000.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 115864000.0 cm-1 |
| 1s1 2p1 4d1 4F2.5 | 115873000.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 115876000.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 115879000.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 115884000.0 cm-1 |
| 1s1 2p1 4d1 4D2.5 | 115888000.0 cm-1 |
| 1s1 2p1 4f1 4G2.5 | 115890000.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 115899000.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 115907000.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 115914000.0 cm-1 |
| 1s1 2p1 4d1 4P1.5 | 115916000.0 cm-1 |
| 1s1 2p1 4d1 4D0.5 | 115922000.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 115924000.0 cm-1 |
| 1s1 2p1 4d1 4F3.5 | 115925000.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 115932000.0 cm-1 |
| 1s1 2p1 4f1 4G3.5 | 115940000.0 cm-1 |
| 1s1 2p1 4f1 4F1.5 | 115943000.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 115946000.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 115950000.0 cm-1 |
| 1s1 2p1 4f1 4F4.5 | 115951000.0 cm-1 |
| 1s1 2p1 4f1 4D3.5 | 115955000.0 cm-1 |
| 1s1 2p1 4s1 4P2.5 | 116101000.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 116131000.0 cm-1 |
| 1s1 2p1 4p1 4P1.5 | 116162000.0 cm-1 |
| 1s1 2p1 4p1 4P2.5 | 116167000.0 cm-1 |
| 1s1 2p1 4p1 4D3.5 | 116186000.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 116203000.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 116224000.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 116238000.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 116242000.0 cm-1 |
| 1s1 2p1 4d1 4F4.5 | 116243000.0 cm-1 |
| 1s1 2p1 4d1 4D3.5 | 116247000.0 cm-1 |
| 1s1 2p1 4d1 4D1.5 | 116253000.0 cm-1 |
| 1s1 2p1 4d1 4P0.5 | 116256000.0 cm-1 |
| 1s1 2p1 4d1 4P2.5 | 116264000.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 116271000.0 cm-1 |
| 1s1 2p1 4f1 4F3.5 | 116278000.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 116281000.0 cm-1 |
| 1s1 2p1 4f1 4F2.5 | 116282000.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 116283000.0 cm-1 |
| 1s1 2p1 4f1 4G4.5 | 116284000.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 116289000.0 cm-1 |
| 1s1 2p1 4f1 4D1.5 | 116289000.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 116292000.0 cm-1 |
| 1s1 2p1 4f1 4G5.5 | 116293000.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 116294000.0 cm-1 |
| 1s1 2p1 4f1 4D0.5 | 116295000.0 cm-1 |
| 1s1 2p1 4f1 4D2.5 | 116296000.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 116301000.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 116306000.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 116343000.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 116343000.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 116376000.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 116389000.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 116398000.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 116421000.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 116427000.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 116430000.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 116438000.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 116447000.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 116452000.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 116458000.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 116460000.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 116466000.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 116469000.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 116470000.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 116479000.0 cm-1 |
Contributors
- Guiyun Liang
- Nigel Badnell
------------------------------------------------------------------------ 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 = 1.28326 2S = 1.04975 2P = 0.95371 3S = 1.03602 3P = 0.94485 3D = 0.88782 4S = 1.03521 4P = 0.94452 4D = 0.88938 4F = 1.04314 5S = 1.03689 5P = 0.94650 5D = 0.89285 5F = 0.89000 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. 60 continuum basis orbitals were used, giving a smallest maximum basis-orbital energy of 3509.2142 Rydbergs (47746.368405 eV) A fine energy mesh of 0.000004 Z**2 Rydbergs (0.052301464 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (130.75366 eV) was used from the last threshold up to 2.721912 Z**2 Rydbergs (35590 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (130.75366 eV) was used from first threshold up to 2.721912 Z**2 Rydbergs (35590 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: 12/10/10 ------------------------------------------------------------------------ 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 = 1.28866 2S = 1.05137 2P = 0.95554 3S = 1.03804 3P = 0.94675 3D = 0.89024 4S = 1.03870 4P = 0.94774 4D = 0.89386 4F = 1.05322 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. 40 continuum basis orbitals were used, giving a smallest maximum basis-orbital energy of 0 Rydbergs (0.000000 eV) A fine energy mesh of 0.000004 Z**2 Rydbergs (0.052301464 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (130.75366 eV) was used from the last threshold up to 2.721912 Z**2 Rydbergs (35590 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (130.75366 eV) was used from first threshold up to 2.721912 Z**2 Rydbergs (35590 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 4.89587 3 8.62897 Produced by: Guiyun Liang Date: 13/08/10 ------------------------------------------------------------------------