lilike_lgy10#ge29.dat
Resolved Specific Ion Data Collections
- Ion
- Ge29+
- Temperature Range
- 15.51 eV → 1.551 x 105 eV
ADF04
- Filename
- lilike_lgy10#ge29.dat
- Full Path
- adf04/copaw#li/lilike_lgy10#ge29.dat
Download data
- Spontaneous Emission: Ge+29(i) → Ge+29(j) + hv
- Electron Impact Excitation: Ge+29(i) + e → Ge+29(j) + e
| 2s1 2S0.5 | 0.0 cm-1 |
| 2p1 2P0.5 | 499159.0 cm-1 |
| 2p1 2P1.5 | 808708.0 cm-1 |
| 3s1 2S0.5 | 14470300.0 cm-1 |
| 3p1 2P0.5 | 14608400.0 cm-1 |
| 3p1 2P1.5 | 14697400.0 cm-1 |
| 3d1 2D1.5 | 14753400.0 cm-1 |
| 3d1 2D2.5 | 14782700.0 cm-1 |
| 4s1 2S0.5 | 19460200.0 cm-1 |
| 4p1 2P0.5 | 19517000.0 cm-1 |
| 4p1 2P1.5 | 19553300.0 cm-1 |
| 4d1 2D1.5 | 19576400.0 cm-1 |
| 4d1 2D2.5 | 19588700.0 cm-1 |
| 4f1 2F2.5 | 19590000.0 cm-1 |
| 4f1 2F3.5 | 19596200.0 cm-1 |
| 5s1 2S0.5 | 21751000.0 cm-1 |
| 5p1 2P0.5 | 21779600.0 cm-1 |
| 5p1 2P1.5 | 21797400.0 cm-1 |
| 5d1 2D1.5 | 21809200.0 cm-1 |
| 5d1 2D2.5 | 21815300.0 cm-1 |
| 5f1 2F2.5 | 21816000.0 cm-1 |
| 5f1 2F3.5 | 21819200.0 cm-1 |
| 5g1 2G3.5 | 21819200.0 cm-1 |
| 5g1 2G4.5 | 21821100.0 cm-1 |
| 1s1 2s2 2S0.5 | 81944700.0 cm-1 |
| 1s1 2s1 2p1 4P0.5 | 82062100.0 cm-1 |
| 1s1 2s1 2p1 4P1.5 | 82135600.0 cm-1 |
| 1s1 2s1 2p1 4P2.5 | 82356200.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 82487500.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 82684800.0 cm-1 |
| 1s1 2p2 4P0.5 | 82700700.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 82821600.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 82866400.0 cm-1 |
| 1s1 2p2 4P1.5 | 82873100.0 cm-1 |
| 1s1 2p2 4P2.5 | 82973200.0 cm-1 |
| 1s1 2p2 2P0.5 | 83125700.0 cm-1 |
| 1s1 2p2 2D1.5 | 83130100.0 cm-1 |
| 1s1 2p2 2D2.5 | 83302500.0 cm-1 |
| 1s1 2p2 2P1.5 | 83455500.0 cm-1 |
| 1s1 2p2 2S0.5 | 83626000.0 cm-1 |
| 1s1 2s1 3s1 4S1.5 | 96599500.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 96740100.0 cm-1 |
| 1s1 2s1 3p1 4P0.5 | 96776800.0 cm-1 |
| 1s1 2s1 3p1 4P1.5 | 96784300.0 cm-1 |
| 1s1 2s1 3p1 4P2.5 | 96857200.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 96866100.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 96867400.0 cm-1 |
| 1s1 2s1 3d1 4D0.5 | 96947200.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 96952600.0 cm-1 |
| 1s1 2s1 3d1 4D1.5 | 96957800.0 cm-1 |
| 1s1 2s1 3d1 4D2.5 | 96972100.0 cm-1 |
| 1s1 2p1 3s1 4P0.5 | 96989900.0 cm-1 |
| 1s1 2s1 3d1 4D3.5 | 96991800.0 cm-1 |
| 1s1 2p1 3s1 4P1.5 | 97040200.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 97042800.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 97044900.0 cm-1 |
| 1s1 2p1 3p1 4D0.5 | 97069100.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 97079500.0 cm-1 |
| 1s1 2p1 3p1 4D1.5 | 97105500.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 97142100.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 97171600.0 cm-1 |
| 1s1 2p1 3p1 4S1.5 | 97201800.0 cm-1 |
| 1s1 2p1 3p1 4D2.5 | 97220600.0 cm-1 |
| 1s1 2p1 3p1 4P0.5 | 97232300.0 cm-1 |
| 1s1 2p1 3d1 4F1.5 | 97253000.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 97264500.0 cm-1 |
| 1s1 2p1 3s1 4P2.5 | 97269200.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 97284100.0 cm-1 |
| 1s1 2p1 3d1 4F2.5 | 97289200.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 97296500.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 97325700.0 cm-1 |
| 1s1 2p1 3d1 4D2.5 | 97340800.0 cm-1 |
| 1s1 2p1 3d1 4F3.5 | 97364300.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 97371400.0 cm-1 |
| 1s1 2p1 3d1 4D1.5 | 97377100.0 cm-1 |
| 1s1 2p1 3d1 4D0.5 | 97385800.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 97393300.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 97397500.0 cm-1 |
| 1s1 2p1 3p1 4P1.5 | 97422800.0 cm-1 |
| 1s1 2p1 3p1 4D3.5 | 97442600.0 cm-1 |
| 1s1 2p1 3p1 4P2.5 | 97449900.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 97482600.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 97483500.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 97489400.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 97556600.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 97564100.0 cm-1 |
| 1s1 2p1 3d1 4F4.5 | 97571600.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 97586500.0 cm-1 |
| 1s1 2p1 3d1 4D3.5 | 97606400.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 97612500.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 97620900.0 cm-1 |
| 1s1 2p1 3d1 4P1.5 | 97623500.0 cm-1 |
| 1s1 2p1 3d1 4P0.5 | 97633200.0 cm-1 |
| 1s1 2p1 3d1 4P2.5 | 97639100.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 97660900.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 97662300.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 97667000.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 97712100.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 97728500.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 97757400.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 97775600.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 97784300.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 97803800.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 97825500.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 97843100.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 97873300.0 cm-1 |
| 1s1 2s1 4s1 4S1.5 | 101712000.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 101757000.0 cm-1 |
| 1s1 2s1 4p1 4P0.5 | 101777000.0 cm-1 |
| 1s1 2s1 4p1 4P1.5 | 101782000.0 cm-1 |
| 1s1 2s1 4p1 4P2.5 | 101808000.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 101822000.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 101826000.0 cm-1 |
| 1s1 2s1 4d1 4D0.5 | 101850000.0 cm-1 |
| 1s1 2s1 4d1 4D1.5 | 101851000.0 cm-1 |
| 1s1 2s1 4d1 4D2.5 | 101855000.0 cm-1 |
| 1s1 2s1 4d1 4D3.5 | 101862000.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 101878000.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 101881000.0 cm-1 |
| 1s1 2s1 4f1 4F1.5 | 101893000.0 cm-1 |
| 1s1 2s1 4f1 4F2.5 | 101894000.0 cm-1 |
| 1s1 2s1 4f1 4F3.5 | 101896000.0 cm-1 |
| 1s1 2s1 4f1 4F4.5 | 101900000.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 101904000.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 101905000.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 102030000.0 cm-1 |
| 1s1 2p1 4s1 4P0.5 | 102034000.0 cm-1 |
| 1s1 2p1 4p1 4D0.5 | 102073000.0 cm-1 |
| 1s1 2p1 4s1 4P1.5 | 102073000.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 102086000.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 102103000.0 cm-1 |
| 1s1 2p1 4p1 4D1.5 | 102110000.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 102123000.0 cm-1 |
| 1s1 2p1 4p1 4S1.5 | 102126000.0 cm-1 |
| 1s1 2p1 4d1 4F1.5 | 102148000.0 cm-1 |
| 1s1 2p1 4p1 4P0.5 | 102149000.0 cm-1 |
| 1s1 2p1 4p1 4D2.5 | 102155000.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 102163000.0 cm-1 |
| 1s1 2p1 4d1 4F2.5 | 102172000.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 102174000.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 102178000.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 102179000.0 cm-1 |
| 1s1 2p1 4d1 4D2.5 | 102186000.0 cm-1 |
| 1s1 2p1 4f1 4G2.5 | 102189000.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 102196000.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 102201000.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 102206000.0 cm-1 |
| 1s1 2p1 4d1 4D1.5 | 102212000.0 cm-1 |
| 1s1 2p1 4d1 4D0.5 | 102216000.0 cm-1 |
| 1s1 2p1 4d1 4F3.5 | 102217000.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 102217000.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 102225000.0 cm-1 |
| 1s1 2p1 4f1 4G3.5 | 102232000.0 cm-1 |
| 1s1 2p1 4f1 4F1.5 | 102234000.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 102237000.0 cm-1 |
| 1s1 2p1 4f1 4G4.5 | 102240000.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 102240000.0 cm-1 |
| 1s1 2p1 4f1 4D3.5 | 102245000.0 cm-1 |
| 1s1 2p1 4s1 4P2.5 | 102332000.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 102360000.0 cm-1 |
| 1s1 2p1 4p1 4P1.5 | 102388000.0 cm-1 |
| 1s1 2p1 4p1 4P2.5 | 102393000.0 cm-1 |
| 1s1 2p1 4p1 4D3.5 | 102404000.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 102421000.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 102441000.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 102454000.0 cm-1 |
| 1s1 2p1 4d1 4F4.5 | 102455000.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 102457000.0 cm-1 |
| 1s1 2p1 4d1 4D3.5 | 102461000.0 cm-1 |
| 1s1 2p1 4d1 4P1.5 | 102467000.0 cm-1 |
| 1s1 2p1 4d1 4P0.5 | 102470000.0 cm-1 |
| 1s1 2p1 4d1 4P2.5 | 102475000.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 102482000.0 cm-1 |
| 1s1 2p1 4f1 4F3.5 | 102488000.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 102491000.0 cm-1 |
| 1s1 2p1 4f1 4F2.5 | 102491000.0 cm-1 |
| 1s1 2p1 4f1 4F4.5 | 102492000.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 102497000.0 cm-1 |
| 1s1 2p1 4f1 4D1.5 | 102498000.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 102500000.0 cm-1 |
| 1s1 2p1 4f1 4G5.5 | 102500000.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 102502000.0 cm-1 |
| 1s1 2p1 4f1 4D2.5 | 102503000.0 cm-1 |
| 1s1 2p1 4f1 4D0.5 | 102504000.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 102512000.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 102513000.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 102515000.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 102561000.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 102561000.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 102586000.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 102597000.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 102606000.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 102627000.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 102632000.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 102634000.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 102644000.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 102649000.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 102653000.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 102658000.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 102661000.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 102666000.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 102669000.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 102671000.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 102678000.0 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 = 1.28313 2S = 1.04911 2P = 0.95269 3S = 1.03535 3P = 0.94399 3D = 0.88597 4S = 1.03389 4P = 0.94367 4D = 0.88758 4F = 1.06038 5S = 1.03614 5P = 0.94566 5D = 0.89117 5F = 0.86168 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 3060.7643 Rydbergs (41644.759066 eV) A fine energy mesh of 0.000005 Z**2 Rydbergs (0.05721323 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (114.42646 eV) was used from the last threshold up to 2.731012 Z**2 Rydbergs (31250 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (114.42646 eV) was used from first threshold up to 2.731012 Z**2 Rydbergs (31250 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 = 1.28845 2S = 1.05074 2P = 0.95459 3S = 1.03740 3P = 0.94591 3D = 0.88805 4S = 1.03733 4P = 0.94689 4D = 0.89202 4F = 1.06267 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 (0.05721323 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (114.42646 eV) was used from the last threshold up to 2.731012 Z**2 Rydbergs (31250 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (114.42646 eV) was used from first threshold up to 2.731012 Z**2 Rydbergs (31250 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 4.54974 3 7.42649 4 131.72365 5 132.99031 6 133.82868 7 134.46657 8 134.69438 12 178.24384 13 178.33496 14 178.55367 15 178.56278 Produced by: Guiyun Liang Date: 13/08/10 ------------------------------------------------------------------------