lilike_lgy10#as30.dat
Resolved Specific Ion Data Collections
- Ion
- As30+
- Temperature Range
- 16.54 eV → 1.654 x 105 eV
ADF04
- Filename
- lilike_lgy10#as30.dat
- Full Path
- adf04/copaw#li/lilike_lgy10#as30.dat
Download data
- Spontaneous Emission: As+30(i) → As+30(j) + hv
- Electron Impact Excitation: As+30(i) + e → As+30(j) + e
| 2s1 2S0.5 | 0.0 cm-1 |
| 2p1 2P0.5 | 517618.0 cm-1 |
| 2p1 2P1.5 | 870586.0 cm-1 |
| 3s1 2S0.5 | 15454400.0 cm-1 |
| 3p1 2P0.5 | 15597500.0 cm-1 |
| 3p1 2P1.5 | 15698700.0 cm-1 |
| 3d1 2D1.5 | 15756900.0 cm-1 |
| 3d1 2D2.5 | 15790400.0 cm-1 |
| 4s1 2S0.5 | 20784300.0 cm-1 |
| 4p1 2P0.5 | 20843100.0 cm-1 |
| 4p1 2P1.5 | 20884300.0 cm-1 |
| 4d1 2D1.5 | 20908400.0 cm-1 |
| 4d1 2D2.5 | 20922300.0 cm-1 |
| 4f1 2F2.5 | 20923700.0 cm-1 |
| 4f1 2F3.5 | 20930700.0 cm-1 |
| 5s1 2S0.5 | 23231200.0 cm-1 |
| 5p1 2P0.5 | 23260900.0 cm-1 |
| 5p1 2P1.5 | 23281000.0 cm-1 |
| 5d1 2D1.5 | 23293200.0 cm-1 |
| 5d1 2D2.5 | 23300200.0 cm-1 |
| 5f1 2F2.5 | 23300900.0 cm-1 |
| 5f1 2F3.5 | 23304500.0 cm-1 |
| 5g1 2G3.5 | 23304500.0 cm-1 |
| 5g1 2G4.5 | 23306700.0 cm-1 |
| 1s1 2s2 2S0.5 | 87328200.0 cm-1 |
| 1s1 2s1 2p1 4P0.5 | 87449100.0 cm-1 |
| 1s1 2s1 2p1 4P1.5 | 87529900.0 cm-1 |
| 1s1 2s1 2p1 4P2.5 | 87785200.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 87892500.0 cm-1 |
| 1s1 2p2 4P0.5 | 88118200.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 88121400.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 88263200.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 88313000.0 cm-1 |
| 1s1 2p2 4P1.5 | 88321600.0 cm-1 |
| 1s1 2p2 4P2.5 | 88429000.0 cm-1 |
| 1s1 2p2 2P0.5 | 88577800.0 cm-1 |
| 1s1 2p2 2D1.5 | 88587200.0 cm-1 |
| 1s1 2p2 2D2.5 | 88793500.0 cm-1 |
| 1s1 2p2 2P1.5 | 88955200.0 cm-1 |
| 1s1 2p2 2S0.5 | 89126200.0 cm-1 |
| 1s1 2s1 3s1 4S1.5 | 102971000.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 103119000.0 cm-1 |
| 1s1 2s1 3p1 4P0.5 | 103156000.0 cm-1 |
| 1s1 2s1 3p1 4P1.5 | 103163000.0 cm-1 |
| 1s1 2s1 3p1 4P2.5 | 103248000.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 103256000.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 103258000.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 103338000.0 cm-1 |
| 1s1 2s1 3d1 4D0.5 | 103341000.0 cm-1 |
| 1s1 2s1 3d1 4D1.5 | 103351000.0 cm-1 |
| 1s1 2s1 3d1 4D2.5 | 103367000.0 cm-1 |
| 1s1 2p1 3s1 4P0.5 | 103378000.0 cm-1 |
| 1s1 2s1 3d1 4D3.5 | 103390000.0 cm-1 |
| 1s1 2p1 3s1 4P1.5 | 103432000.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 103442000.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 103444000.0 cm-1 |
| 1s1 2p1 3p1 4D0.5 | 103459000.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 103472000.0 cm-1 |
| 1s1 2p1 3p1 4D1.5 | 103498000.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 103536000.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 103577000.0 cm-1 |
| 1s1 2p1 3p1 4S1.5 | 103605000.0 cm-1 |
| 1s1 2p1 3p1 4D2.5 | 103627000.0 cm-1 |
| 1s1 2p1 3p1 4P0.5 | 103633000.0 cm-1 |
| 1s1 2p1 3d1 4F1.5 | 103658000.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 103673000.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 103691000.0 cm-1 |
| 1s1 2p1 3s1 4P2.5 | 103694000.0 cm-1 |
| 1s1 2p1 3d1 4F2.5 | 103699000.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 103705000.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 103739000.0 cm-1 |
| 1s1 2p1 3d1 4D2.5 | 103753000.0 cm-1 |
| 1s1 2p1 3d1 4F3.5 | 103780000.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 103786000.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 103794000.0 cm-1 |
| 1s1 2p1 3d1 4D0.5 | 103798000.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 103812000.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 103818000.0 cm-1 |
| 1s1 2p1 3p1 4P1.5 | 103856000.0 cm-1 |
| 1s1 2p1 3p1 4P2.5 | 103884000.0 cm-1 |
| 1s1 2p1 3p1 4D3.5 | 103885000.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 103916000.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 103923000.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 103927000.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 103997000.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 104010000.0 cm-1 |
| 1s1 2p1 3d1 4F4.5 | 104022000.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 104035000.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 104050000.0 cm-1 |
| 1s1 2p1 3d1 4D3.5 | 104056000.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 104062000.0 cm-1 |
| 1s1 2p1 3d1 4D1.5 | 104072000.0 cm-1 |
| 1s1 2p1 3d1 4P0.5 | 104082000.0 cm-1 |
| 1s1 2p1 3d1 4P2.5 | 104091000.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 104110000.0 cm-1 |
| 1s1 2p1 3d1 4P1.5 | 104112000.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 104120000.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 104163000.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 104184000.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 104208000.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 104229000.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 104238000.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 104259000.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 104279000.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 104301000.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 104332000.0 cm-1 |
| 1s1 2s1 4s1 4S1.5 | 108428000.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 108476000.0 cm-1 |
| 1s1 2s1 4p1 4P0.5 | 108496000.0 cm-1 |
| 1s1 2s1 4p1 4P1.5 | 108501000.0 cm-1 |
| 1s1 2s1 4p1 4P2.5 | 108531000.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 108545000.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 108549000.0 cm-1 |
| 1s1 2s1 4d1 4D0.5 | 108574000.0 cm-1 |
| 1s1 2s1 4d1 4D1.5 | 108576000.0 cm-1 |
| 1s1 2s1 4d1 4D2.5 | 108580000.0 cm-1 |
| 1s1 2s1 4d1 4D3.5 | 108588000.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 108604000.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 108607000.0 cm-1 |
| 1s1 2s1 4f1 4F1.5 | 108620000.0 cm-1 |
| 1s1 2s1 4f1 4F2.5 | 108621000.0 cm-1 |
| 1s1 2s1 4f1 4F3.5 | 108623000.0 cm-1 |
| 1s1 2s1 4f1 4F4.5 | 108628000.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 108632000.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 108633000.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 108760000.0 cm-1 |
| 1s1 2p1 4s1 4P0.5 | 108762000.0 cm-1 |
| 1s1 2p1 4p1 4D0.5 | 108803000.0 cm-1 |
| 1s1 2p1 4s1 4P1.5 | 108805000.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 108818000.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 108835000.0 cm-1 |
| 1s1 2p1 4p1 4D1.5 | 108843000.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 108859000.0 cm-1 |
| 1s1 2p1 4p1 4S1.5 | 108860000.0 cm-1 |
| 1s1 2p1 4d1 4F1.5 | 108884000.0 cm-1 |
| 1s1 2p1 4p1 4P0.5 | 108884000.0 cm-1 |
| 1s1 2p1 4p1 4D2.5 | 108893000.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 108901000.0 cm-1 |
| 1s1 2p1 4d1 4F2.5 | 108910000.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 108913000.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 108916000.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 108919000.0 cm-1 |
| 1s1 2p1 4d1 4D2.5 | 108924000.0 cm-1 |
| 1s1 2p1 4f1 4G2.5 | 108927000.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 108935000.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 108942000.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 108947000.0 cm-1 |
| 1s1 2p1 4d1 4P1.5 | 108952000.0 cm-1 |
| 1s1 2p1 4d1 4D0.5 | 108957000.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 108958000.0 cm-1 |
| 1s1 2p1 4d1 4F3.5 | 108958000.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 108966000.0 cm-1 |
| 1s1 2p1 4f1 4G3.5 | 108973000.0 cm-1 |
| 1s1 2p1 4f1 4F1.5 | 108976000.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 108979000.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 108983000.0 cm-1 |
| 1s1 2p1 4f1 4F4.5 | 108983000.0 cm-1 |
| 1s1 2p1 4f1 4D3.5 | 108988000.0 cm-1 |
| 1s1 2p1 4s1 4P2.5 | 109102000.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 109131000.0 cm-1 |
| 1s1 2p1 4p1 4P1.5 | 109161000.0 cm-1 |
| 1s1 2p1 4p1 4P2.5 | 109166000.0 cm-1 |
| 1s1 2p1 4p1 4D3.5 | 109180000.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 109197000.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 109218000.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 109231000.0 cm-1 |
| 1s1 2p1 4d1 4F4.5 | 109235000.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 109235000.0 cm-1 |
| 1s1 2p1 4d1 4D3.5 | 109239000.0 cm-1 |
| 1s1 2p1 4d1 4D1.5 | 109245000.0 cm-1 |
| 1s1 2p1 4d1 4P0.5 | 109249000.0 cm-1 |
| 1s1 2p1 4d1 4P2.5 | 109255000.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 109262000.0 cm-1 |
| 1s1 2p1 4f1 4F3.5 | 109268000.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 109271000.0 cm-1 |
| 1s1 2p1 4f1 4F2.5 | 109272000.0 cm-1 |
| 1s1 2p1 4f1 4G4.5 | 109273000.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 109278000.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 109278000.0 cm-1 |
| 1s1 2p1 4f1 4D1.5 | 109279000.0 cm-1 |
| 1s1 2p1 4f1 4G5.5 | 109282000.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 109283000.0 cm-1 |
| 1s1 2p1 4f1 4D0.5 | 109285000.0 cm-1 |
| 1s1 2p1 4f1 4D2.5 | 109285000.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 109288000.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 109292000.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 109294000.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 109338000.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 109338000.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 109367000.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 109378000.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 109387000.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 109410000.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 109415000.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 109418000.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 109426000.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 109433000.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 109438000.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 109444000.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 109446000.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 109451000.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 109454000.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 109455000.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 109464000.0 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 = 1.28319 2S = 1.04943 2P = 0.95317 3S = 1.03572 3P = 0.94543 3D = 0.88445 4S = 1.03472 4P = 0.94482 4D = 0.88609 4F = 1.07506 5S = 1.03646 5P = 0.93754 5D = 0.88944 5F = 0.86013 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 3300.4565 Rydbergs (44906.011139 eV) A fine energy mesh of 0.000005 Z**2 Rydbergs (0.061227 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (122.454 eV) was used from the last threshold up to 2.726738 Z**2 Rydbergs (33390 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (122.454 eV) was used from first threshold up to 2.726738 Z**2 Rydbergs (33390 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 = 1.28856 2S = 1.05106 2P = 0.95506 3S = 1.03768 3P = 0.94638 3D = 0.88844 4S = 1.03761 4P = 0.94735 4D = 0.89240 4F = 1.06961 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 0.000005 Z**2 Rydbergs (0.061227 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (122.454 eV) was used from the last threshold up to 2.726738 Z**2 Rydbergs (33390 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (122.454 eV) was used from first threshold up to 2.726738 Z**2 Rydbergs (33390 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 4.72374 3 8.00730 Produced by: Guiyun Liang Date: 13/08/10 ------------------------------------------------------------------------