nelike_lgy09#ga21.dat
Resolved Specific Ion Data Collections
- Ion
- Ga21+
- Temperature Range
- 8.341 eV → 8.341 x 104 eV
ADF04
- Filename
- nelike_lgy09#ga21.dat
- Full Path
- adf04/copaw#ne/nelike_lgy09#ga21.dat
Download data
- Spontaneous Emission: Ga+21(i) → Ga+21(j) + hv
- Electron Impact Excitation: Ga+21(i) + e → Ga+21(j) + e
| 2s2 2p6 1S0.0 | 0.0 cm-1 |
| 2s2 2p5 3s1 3P2.0 | 9215070.0 cm-1 |
| 2s2 2p5 3s1 1P1.0 | 9234470.0 cm-1 |
| 2s2 2p5 3s1 3P0.0 | 9442480.0 cm-1 |
| 2s2 2p5 3s1 3P1.0 | 9453460.0 cm-1 |
| 2s2 2p5 3p1 3S1.0 | 9547390.0 cm-1 |
| 2s2 2p5 3p1 3D2.0 | 9575140.0 cm-1 |
| 2s2 2p5 3p1 3D3.0 | 9615280.0 cm-1 |
| 2s2 2p5 3p1 1P1.0 | 9621500.0 cm-1 |
| 2s2 2p5 3p1 3P2.0 | 9645320.0 cm-1 |
| 2s2 2p5 3p1 3P0.0 | 9731560.0 cm-1 |
| 2s2 2p5 3p1 3D1.0 | 9796230.0 cm-1 |
| 2s2 2p5 3p1 3P1.0 | 9850440.0 cm-1 |
| 2s2 2p5 3p1 1D2.0 | 9857540.0 cm-1 |
| 2s2 2p5 3p1 1S0.0 | 9960590.0 cm-1 |
| 2s2 2p5 3d1 3P0.0 | 10038500.0 cm-1 |
| 2s2 2p5 3d1 3P1.0 | 10052800.0 cm-1 |
| 2s2 2p5 3d1 3P2.0 | 10078400.0 cm-1 |
| 2s2 2p5 3d1 3F4.0 | 10078800.0 cm-1 |
| 2s2 2p5 3d1 3F3.0 | 10079500.0 cm-1 |
| 2s2 2p5 3d1 1D2.0 | 10099900.0 cm-1 |
| 2s2 2p5 3d1 3D3.0 | 10117400.0 cm-1 |
| 2s2 2p5 3d1 3D1.0 | 10180100.0 cm-1 |
| 2s2 2p5 3d1 3F2.0 | 10304200.0 cm-1 |
| 2s2 2p5 3d1 3D2.0 | 10319200.0 cm-1 |
| 2s2 2p5 3d1 1F3.0 | 10327800.0 cm-1 |
| 2s2 2p5 3d1 1P1.0 | 10392000.0 cm-1 |
| 2s1 2p6 3s1 3S1.0 | 10693900.0 cm-1 |
| 2s1 2p6 3s1 1S0.0 | 10766800.0 cm-1 |
| 2s1 2p6 3p1 3P0.0 | 11042500.0 cm-1 |
| 2s1 2p6 3p1 3P1.0 | 11048800.0 cm-1 |
| 2s1 2p6 3p1 3P2.0 | 11096000.0 cm-1 |
| 2s1 2p6 3p1 1P1.0 | 11114200.0 cm-1 |
| 2s1 2p6 3d1 3D1.0 | 11534400.0 cm-1 |
| 2s1 2p6 3d1 3D2.0 | 11539200.0 cm-1 |
| 2s1 2p6 3d1 3D3.0 | 11548500.0 cm-1 |
| 2s1 2p6 3d1 1D2.0 | 11598300.0 cm-1 |
| 2s2 2p5 4s1 3P2.0 | 12464400.0 cm-1 |
| 2s2 2p5 4s1 1P1.0 | 12470000.0 cm-1 |
| 2s2 2p5 4p1 3S1.0 | 12599600.0 cm-1 |
| 2s2 2p5 4p1 3D2.0 | 12606300.0 cm-1 |
| 2s2 2p5 4p1 3D3.0 | 12621600.0 cm-1 |
| 2s2 2p5 4p1 1P1.0 | 12623900.0 cm-1 |
| 2s2 2p5 4p1 3P2.0 | 12631500.0 cm-1 |
| 2s2 2p5 4p1 3P0.0 | 12674700.0 cm-1 |
| 2s2 2p5 4s1 3P0.0 | 12692100.0 cm-1 |
| 2s2 2p5 4s1 3P1.0 | 12694800.0 cm-1 |
| 2s2 2p5 4d1 3P0.0 | 12780400.0 cm-1 |
| 2s2 2p5 4d1 3P1.0 | 12786000.0 cm-1 |
| 2s2 2p5 4d1 3F3.0 | 12793900.0 cm-1 |
| 2s2 2p5 4d1 3F4.0 | 12794300.0 cm-1 |
| 2s2 2p5 4d1 3P2.0 | 12795200.0 cm-1 |
| 2s2 2p5 4d1 1D2.0 | 12801200.0 cm-1 |
| 2s2 2p5 4d1 3D3.0 | 12807700.0 cm-1 |
| 2s2 2p5 4p1 3D1.0 | 12831500.0 cm-1 |
| 2s2 2p5 4d1 1P1.0 | 12836400.0 cm-1 |
| 2s2 2p5 4p1 3P1.0 | 12851400.0 cm-1 |
| 2s2 2p5 4p1 1D2.0 | 12854000.0 cm-1 |
| 2s2 2p5 4p1 1S0.0 | 12869000.0 cm-1 |
| 2s2 2p5 4f1 3D1.0 | 12879300.0 cm-1 |
| 2s2 2p5 4f1 1G4.0 | 12881000.0 cm-1 |
| 2s2 2p5 4f1 3D2.0 | 12882000.0 cm-1 |
| 2s2 2p5 4f1 3G5.0 | 12883100.0 cm-1 |
| 2s2 2p5 4f1 1D2.0 | 12886500.0 cm-1 |
| 2s2 2p5 4f1 3F3.0 | 12886500.0 cm-1 |
| 2s2 2p5 4f1 1F3.0 | 12887300.0 cm-1 |
| 2s2 2p5 4f1 3F4.0 | 12889500.0 cm-1 |
| 2s2 2p5 4d1 3F2.0 | 13019900.0 cm-1 |
| 2s2 2p5 4d1 3D2.0 | 13025700.0 cm-1 |
| 2s2 2p5 4d1 1F3.0 | 13029300.0 cm-1 |
| 2s2 2p5 4d1 3D1.0 | 13046600.0 cm-1 |
| 2s2 2p5 4f1 3G3.0 | 13110500.0 cm-1 |
| 2s2 2p5 4f1 3F2.0 | 13112700.0 cm-1 |
| 2s2 2p5 4f1 3G4.0 | 13113400.0 cm-1 |
| 2s2 2p5 4f1 3D3.0 | 13114000.0 cm-1 |
| 2s2 2p5 5s1 3P2.0 | 13874600.0 cm-1 |
| 2s2 2p5 5s1 1P1.0 | 13877400.0 cm-1 |
| 2s1 2p6 4s1 3S1.0 | 13916500.0 cm-1 |
| 2s2 2p5 5p1 3D2.0 | 13945600.0 cm-1 |
| 2s1 2p6 4s1 1S0.0 | 13946600.0 cm-1 |
| 2s2 2p5 5p1 3S1.0 | 13949200.0 cm-1 |
| 2s2 2p5 5p1 3D3.0 | 13953100.0 cm-1 |
| 2s2 2p5 5p1 1P1.0 | 13957800.0 cm-1 |
| 2s2 2p5 5p1 3P2.0 | 13957900.0 cm-1 |
| 2s2 2p5 5p1 1S0.0 | 13980800.0 cm-1 |
| 2s2 2p5 5d1 3P0.0 | 14029900.0 cm-1 |
| 2s2 2p5 5d1 3P1.0 | 14032900.0 cm-1 |
| 2s2 2p5 5d1 3F3.0 | 14037100.0 cm-1 |
| 2s2 2p5 5d1 3F4.0 | 14037600.0 cm-1 |
| 2s2 2p5 5d1 3P2.0 | 14037700.0 cm-1 |
| 2s2 2p5 5d1 1D2.0 | 14040500.0 cm-1 |
| 2s2 2p5 5d1 3D3.0 | 14043700.0 cm-1 |
| 2s2 2p5 5d1 1P1.0 | 14057200.0 cm-1 |
| 2s1 2p6 4p1 3P0.0 | 14064100.0 cm-1 |
| 2s1 2p6 4p1 3P1.0 | 14068300.0 cm-1 |
| 2s2 2p5 5f1 3D1.0 | 14078200.0 cm-1 |
| 2s2 2p5 5f1 3D2.0 | 14079900.0 cm-1 |
| 2s2 2p5 5f1 1G4.0 | 14080600.0 cm-1 |
| 2s2 2p5 5f1 3G5.0 | 14081700.0 cm-1 |
| 2s2 2p5 5f1 3F3.0 | 14082600.0 cm-1 |
| 2s2 2p5 5f1 1D2.0 | 14083200.0 cm-1 |
| 2s2 2p5 5f1 1F3.0 | 14083200.0 cm-1 |
| 2s2 2p5 5g1 3F2.0 | 14084500.0 cm-1 |
| 2s2 2p5 5f1 3F4.0 | 14084700.0 cm-1 |
| 2s2 2p5 5g1 3F3.0 | 14084900.0 cm-1 |
| 2s2 2p5 5g1 1H5.0 | 14086600.0 cm-1 |
| 2s1 2p6 4p1 3P2.0 | 14086900.0 cm-1 |
| 2s2 2p5 5g1 3G3.0 | 14086900.0 cm-1 |
| 2s2 2p5 5g1 1G4.0 | 14087500.0 cm-1 |
| 2s2 2p5 5g1 3H6.0 | 14087700.0 cm-1 |
| 2s2 2p5 5g1 3G4.0 | 14088000.0 cm-1 |
| 2s2 2p5 5g1 3G5.0 | 14088900.0 cm-1 |
| 2s1 2p6 4p1 1P1.0 | 14089300.0 cm-1 |
| 2s2 2p5 5s1 3P0.0 | 14107100.0 cm-1 |
| 2s2 2p5 5s1 3P1.0 | 14109700.0 cm-1 |
| 2s2 2p5 5p1 3D1.0 | 14172000.0 cm-1 |
| 2s2 2p5 5p1 3P1.0 | 14182600.0 cm-1 |
| 2s2 2p5 5p1 1D2.0 | 14182600.0 cm-1 |
| 2s2 2p5 5p1 3P0.0 | 14188000.0 cm-1 |
| 2s1 2p6 4d1 3D1.0 | 14253000.0 cm-1 |
| 2s1 2p6 4d1 3D2.0 | 14253600.0 cm-1 |
| 2s1 2p6 4d1 3D3.0 | 14255800.0 cm-1 |
| 2s2 2p5 5d1 3F2.0 | 14264200.0 cm-1 |
| 2s2 2p5 5d1 3D2.0 | 14267200.0 cm-1 |
| 2s2 2p5 5d1 1F3.0 | 14268700.0 cm-1 |
| 2s1 2p6 4d1 1D2.0 | 14274400.0 cm-1 |
| 2s2 2p5 5d1 3D1.0 | 14276100.0 cm-1 |
| 2s2 2p5 5g1 1F3.0 | 14308700.0 cm-1 |
| 2s2 2p5 5f1 3G3.0 | 14309200.0 cm-1 |
| 2s2 2p5 5g1 3F4.0 | 14309400.0 cm-1 |
| 2s2 2p5 5f1 3G4.0 | 14310700.0 cm-1 |
| 2s2 2p5 5f1 3F2.0 | 14311100.0 cm-1 |
| 2s2 2p5 5f1 3D3.0 | 14312200.0 cm-1 |
| 2s2 2p5 5g1 3H4.0 | 14315100.0 cm-1 |
| 2s2 2p5 5g1 3H5.0 | 14315900.0 cm-1 |
| 2s1 2p6 4f1 3F2.0 | 14341500.0 cm-1 |
| 2s1 2p6 4f1 3F3.0 | 14344400.0 cm-1 |
| 2s1 2p6 4f1 1F3.0 | 14348600.0 cm-1 |
| 2s1 2p6 4f1 3F4.0 | 14349500.0 cm-1 |
| 2s2 2p5 6s1 3P2.0 | 14620100.0 cm-1 |
| 2s2 2p5 6s1 1P1.0 | 14621400.0 cm-1 |
| 2s2 2p5 6p1 3S1.0 | 14658700.0 cm-1 |
| 2s2 2p5 6p1 3D2.0 | 14660200.0 cm-1 |
| 2s2 2p5 6p1 3D3.0 | 14664200.0 cm-1 |
| 2s2 2p5 6p1 1P1.0 | 14664900.0 cm-1 |
| 2s2 2p5 6p1 3P2.0 | 14666700.0 cm-1 |
| 2s2 2p5 6p1 1S0.0 | 14678700.0 cm-1 |
| 2s2 2p5 6d1 3P0.0 | 14707900.0 cm-1 |
| 2s2 2p5 6d1 3P1.0 | 14709400.0 cm-1 |
| 2s2 2p5 6d1 3F3.0 | 14711300.0 cm-1 |
| 2s2 2p5 6d1 3F4.0 | 14711500.0 cm-1 |
| 2s2 2p5 6d1 3D2.0 | 14711800.0 cm-1 |
| 2s2 2p5 6d1 1D2.0 | 14713300.0 cm-1 |
| 2s2 2p5 6d1 3D3.0 | 14715000.0 cm-1 |
| 2s2 2p5 6d1 1P1.0 | 14723400.0 cm-1 |
| 2s2 2p5 6s1 3P0.0 | 14846800.0 cm-1 |
| 2s2 2p5 6s1 3P1.0 | 14847500.0 cm-1 |
| 2s2 2p5 6p1 3D1.0 | 14886200.0 cm-1 |
| 2s2 2p5 6p1 3P1.0 | 14891400.0 cm-1 |
| 2s2 2p5 6p1 1D2.0 | 14892100.0 cm-1 |
| 2s2 2p5 6p1 3P0.0 | 14894000.0 cm-1 |
| 2s2 2p5 6d1 3F2.0 | 14937500.0 cm-1 |
| 2s2 2p5 6d1 3P2.0 | 14939100.0 cm-1 |
| 2s2 2p5 6d1 1F3.0 | 14940100.0 cm-1 |
| 2s2 2p5 6d1 3D1.0 | 14943800.0 cm-1 |
| 2s2 2p5 7s1 3P2.0 | 15057300.0 cm-1 |
| 2s2 2p5 7s1 1P1.0 | 15058200.0 cm-1 |
| 2s2 2p5 7p1 3S1.0 | 15081400.0 cm-1 |
| 2s2 2p5 7p1 3D2.0 | 15082200.0 cm-1 |
| 2s2 2p5 7p1 3D3.0 | 15084600.0 cm-1 |
| 2s2 2p5 7p1 1P1.0 | 15085100.0 cm-1 |
| 2s2 2p5 7p1 3P2.0 | 15086200.0 cm-1 |
| 2s2 2p5 7p1 1S0.0 | 15093600.0 cm-1 |
| 2s2 2p5 7d1 3P0.0 | 15111800.0 cm-1 |
| 2s2 2p5 7d1 3P1.0 | 15112700.0 cm-1 |
| 2s2 2p5 7d1 3F3.0 | 15113800.0 cm-1 |
| 2s2 2p5 7d1 3F4.0 | 15113900.0 cm-1 |
| 2s2 2p5 7d1 3D2.0 | 15114100.0 cm-1 |
| 2s2 2p5 7d1 1D2.0 | 15115000.0 cm-1 |
| 2s2 2p5 7d1 3D3.0 | 15116000.0 cm-1 |
| 2s2 2p5 7d1 1P1.0 | 15121300.0 cm-1 |
| 2s2 2p5 7s1 3P0.0 | 15284000.0 cm-1 |
| 2s2 2p5 7s1 3P1.0 | 15284400.0 cm-1 |
| 2s2 2p5 7p1 3D1.0 | 15308500.0 cm-1 |
| 2s2 2p5 7p1 3P1.0 | 15311000.0 cm-1 |
| 2s2 2p5 7p1 1D2.0 | 15312100.0 cm-1 |
| 2s2 2p5 7p1 3P0.0 | 15313100.0 cm-1 |
| 2s1 2p6 5s1 3S1.0 | 15335900.0 cm-1 |
| 2s2 2p5 7d1 3F2.0 | 15340300.0 cm-1 |
| 2s2 2p5 7d1 3P2.0 | 15341200.0 cm-1 |
| 2s2 2p5 7d1 1F3.0 | 15341800.0 cm-1 |
| 2s2 2p5 7d1 3D1.0 | 15344100.0 cm-1 |
| 2s1 2p6 5s1 1S0.0 | 15344300.0 cm-1 |
| 2s1 2p6 5p1 3P0.0 | 15404800.0 cm-1 |
| 2s1 2p6 5p1 3P1.0 | 15405600.0 cm-1 |
| 2s1 2p6 5p1 3P2.0 | 15413900.0 cm-1 |
| 2s1 2p6 5p1 1P1.0 | 15416500.0 cm-1 |
| 2s1 2p6 5d1 3D1.0 | 15494400.0 cm-1 |
| 2s1 2p6 5d1 3D2.0 | 15495200.0 cm-1 |
| 2s1 2p6 5d1 3D3.0 | 15497000.0 cm-1 |
| 2s1 2p6 5d1 1D2.0 | 15504900.0 cm-1 |
| 2s1 2p6 5f1 3F2.0 | 15538100.0 cm-1 |
| 2s1 2p6 5f1 3F3.0 | 15538400.0 cm-1 |
| 2s1 2p6 5f1 3F4.0 | 15539300.0 cm-1 |
| 2s1 2p6 5f1 1F3.0 | 15540400.0 cm-1 |
| 2s1 2p6 5g1 3G3.0 | 15543800.0 cm-1 |
| 2s1 2p6 5g1 3G4.0 | 15543800.0 cm-1 |
| 2s1 2p6 5g1 3G5.0 | 15544500.0 cm-1 |
| 2s1 2p6 5g1 1G4.0 | 15544600.0 cm-1 |
------------------------------------------------------------------------ Result of ICFT R-matrix calculation +++++++++++++++++++++++++++++++++++ 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 = 1.00000 2S = 1.50306 2P = 1.12207 3S = 1.35715 3P = 1.12929 3D = 1.07705 4S = 1.000 4P = 1.000 4D = 1.000 4F = 1.000 5S = 1.000 5P = 1.000 5D = 1.000 5F = 1.000 5G = 1.000 6S = 1.000 6P = 1.000 6D = 1.000 7S = 1.000 7P = 1.000 7D = 1.000 An exchange calculation was performed up to J=11.5 A non-exchange calculation was then performed up to J=39.5 Followed by a top-up calculation to J -> infinity. 60 continuum basis orbitals were used, giving a smallest maximum basis-orbital energy of 563.9896 Rydbergs (7673.642498 eV) A fine energy mesh of 0.000005 Z**2 Rydbergs (0.03000123 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.002000 Z**2 Rydbergs (12.000492 eV) was used from the last threshold up to 0.925962 Z**2 Rydbergs (5556 eV) in the excitation calculation. A coarse energy mesh of 0.002000 Z**2 Rydbergs (12.000492 eV) was used from first threshold up to 0.925962 Z**2 Rydbergs (5556 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: 10/11/09 ------------------------------------------------------------------------