nelike_lgy09#ge22.dat
Resolved Specific Ion Data Collections
- Ion
- Ge22+
- Temperature Range
- 9.134 eV → 9.134 x 104 eV
ADF04
- Filename
- nelike_lgy09#ge22.dat
- Full Path
- adf04/copaw#ne/nelike_lgy09#ge22.dat
Download data
- Spontaneous Emission: Ge+22(i) → Ge+22(j) + hv
- Electron Impact Excitation: Ge+22(i) + e → Ge+22(j) + e
| 2s2 2p6 1S0.0 | 0.0 cm-1 |
| 2s2 2p5 3s1 3P2.0 | 9976840.0 cm-1 |
| 2s2 2p5 3s1 1P1.0 | 9996990.0 cm-1 |
| 2s2 2p5 3s1 3P0.0 | 10239400.0 cm-1 |
| 2s2 2p5 3s1 3P1.0 | 10250600.0 cm-1 |
| 2s2 2p5 3p1 3S1.0 | 10327400.0 cm-1 |
| 2s2 2p5 3p1 3D2.0 | 10354600.0 cm-1 |
| 2s2 2p5 3p1 3D3.0 | 10403000.0 cm-1 |
| 2s2 2p5 3p1 1P1.0 | 10408400.0 cm-1 |
| 2s2 2p5 3p1 3P2.0 | 10434300.0 cm-1 |
| 2s2 2p5 3p1 3P0.0 | 10529800.0 cm-1 |
| 2s2 2p5 3p1 3D1.0 | 10610300.0 cm-1 |
| 2s2 2p5 3p1 3P1.0 | 10673100.0 cm-1 |
| 2s2 2p5 3p1 1D2.0 | 10681000.0 cm-1 |
| 2s2 2p5 3p1 1S0.0 | 10777500.0 cm-1 |
| 2s2 2p5 3d1 3P0.0 | 10844900.0 cm-1 |
| 2s2 2p5 3d1 3P1.0 | 10860400.0 cm-1 |
| 2s2 2p5 3d1 3F3.0 | 10887800.0 cm-1 |
| 2s2 2p5 3d1 3P2.0 | 10888200.0 cm-1 |
| 2s2 2p5 3d1 3F4.0 | 10888700.0 cm-1 |
| 2s2 2p5 3d1 1D2.0 | 10909900.0 cm-1 |
| 2s2 2p5 3d1 3D3.0 | 10929300.0 cm-1 |
| 2s2 2p5 3d1 3D1.0 | 10997200.0 cm-1 |
| 2s2 2p5 3d1 3F2.0 | 11147300.0 cm-1 |
| 2s2 2p5 3d1 3D2.0 | 11164500.0 cm-1 |
| 2s2 2p5 3d1 1F3.0 | 11173900.0 cm-1 |
| 2s2 2p5 3d1 1P1.0 | 11237800.0 cm-1 |
| 2s1 2p6 3s1 3S1.0 | 11542900.0 cm-1 |
| 2s1 2p6 3s1 1S0.0 | 11620600.0 cm-1 |
| 2s1 2p6 3p1 3P0.0 | 11909100.0 cm-1 |
| 2s1 2p6 3p1 3P1.0 | 11915800.0 cm-1 |
| 2s1 2p6 3p1 3P2.0 | 11971200.0 cm-1 |
| 2s1 2p6 3p1 1P1.0 | 11989900.0 cm-1 |
| 2s1 2p6 3d1 3D1.0 | 12429400.0 cm-1 |
| 2s1 2p6 3d1 3D2.0 | 12435000.0 cm-1 |
| 2s1 2p6 3d1 3D3.0 | 12445900.0 cm-1 |
| 2s1 2p6 3d1 1D2.0 | 12497800.0 cm-1 |
| 2s2 2p5 4s1 3P2.0 | 13503800.0 cm-1 |
| 2s2 2p5 4s1 1P1.0 | 13509600.0 cm-1 |
| 2s2 2p5 4p1 3S1.0 | 13646000.0 cm-1 |
| 2s2 2p5 4p1 3D2.0 | 13652600.0 cm-1 |
| 2s2 2p5 4p1 3D3.0 | 13670900.0 cm-1 |
| 2s2 2p5 4p1 1P1.0 | 13672900.0 cm-1 |
| 2s2 2p5 4p1 3P2.0 | 13681300.0 cm-1 |
| 2s2 2p5 4p1 1S0.0 | 13726900.0 cm-1 |
| 2s2 2p5 4s1 3P0.0 | 13766800.0 cm-1 |
| 2s2 2p5 4s1 3P1.0 | 13769500.0 cm-1 |
| 2s2 2p5 4d1 3P0.0 | 13837000.0 cm-1 |
| 2s2 2p5 4d1 3P1.0 | 13843000.0 cm-1 |
| 2s2 2p5 4d1 3F3.0 | 13851100.0 cm-1 |
| 2s2 2p5 4d1 3F4.0 | 13852300.0 cm-1 |
| 2s2 2p5 4d1 3D2.0 | 13852900.0 cm-1 |
| 2s2 2p5 4d1 1D2.0 | 13859100.0 cm-1 |
| 2s2 2p5 4d1 3D3.0 | 13866300.0 cm-1 |
| 2s2 2p5 4d1 1P1.0 | 13896600.0 cm-1 |
| 2s2 2p5 4p1 3D1.0 | 13913000.0 cm-1 |
| 2s2 2p5 4p1 3P1.0 | 13936000.0 cm-1 |
| 2s2 2p5 4p1 1D2.0 | 13938700.0 cm-1 |
| 2s2 2p5 4f1 3D1.0 | 13941800.0 cm-1 |
| 2s2 2p5 4f1 1G4.0 | 13943800.0 cm-1 |
| 2s2 2p5 4f1 3D2.0 | 13944800.0 cm-1 |
| 2s2 2p5 4f1 3G5.0 | 13946300.0 cm-1 |
| 2s2 2p5 4f1 1D2.0 | 13949500.0 cm-1 |
| 2s2 2p5 4f1 3F3.0 | 13949500.0 cm-1 |
| 2s2 2p5 4f1 1F3.0 | 13950500.0 cm-1 |
| 2s2 2p5 4p1 3P0.0 | 13951300.0 cm-1 |
| 2s2 2p5 4f1 3F4.0 | 13953000.0 cm-1 |
| 2s2 2p5 4d1 3F2.0 | 14112300.0 cm-1 |
| 2s2 2p5 4d1 3P2.0 | 14119100.0 cm-1 |
| 2s2 2p5 4d1 1F3.0 | 14122900.0 cm-1 |
| 2s2 2p5 4d1 3D1.0 | 14139900.0 cm-1 |
| 2s2 2p5 4f1 3G3.0 | 14208600.0 cm-1 |
| 2s2 2p5 4f1 3F2.0 | 14210900.0 cm-1 |
| 2s2 2p5 4f1 3G4.0 | 14211900.0 cm-1 |
| 2s2 2p5 4f1 3D3.0 | 14212500.0 cm-1 |
| 2s2 2p5 5s1 3P2.0 | 15037100.0 cm-1 |
| 2s2 2p5 5s1 1P1.0 | 15040000.0 cm-1 |
| 2s1 2p6 4s1 3S1.0 | 15047500.0 cm-1 |
| 2s1 2p6 4s1 1S0.0 | 15074600.0 cm-1 |
| 2s2 2p5 5p1 3D2.0 | 15111800.0 cm-1 |
| 2s2 2p5 5p1 3S1.0 | 15112700.0 cm-1 |
| 2s2 2p5 5p1 3D3.0 | 15120800.0 cm-1 |
| 2s2 2p5 5p1 1P1.0 | 15123100.0 cm-1 |
| 2s2 2p5 5p1 3P2.0 | 15125700.0 cm-1 |
| 2s2 2p5 5p1 1S0.0 | 15148700.0 cm-1 |
| 2s1 2p6 4p1 3P0.0 | 15193300.0 cm-1 |
| 2s1 2p6 4p1 3P1.0 | 15198000.0 cm-1 |
| 2s2 2p5 5d1 3P0.0 | 15207200.0 cm-1 |
| 2s2 2p5 5d1 3F3.0 | 15208600.0 cm-1 |
| 2s2 2p5 5d1 3P1.0 | 15208600.0 cm-1 |
| 2s2 2p5 5d1 3D2.0 | 15208600.0 cm-1 |
| 2s2 2p5 5d1 3F4.0 | 15209500.0 cm-1 |
| 2s2 2p5 5d1 1D2.0 | 15212100.0 cm-1 |
| 2s2 2p5 5d1 3D3.0 | 15215900.0 cm-1 |
| 2s1 2p6 4p1 1P1.0 | 15223900.0 cm-1 |
| 2s1 2p6 4p1 3P2.0 | 15224100.0 cm-1 |
| 2s2 2p5 5d1 1P1.0 | 15234500.0 cm-1 |
| 2s2 2p5 5f1 3D1.0 | 15252100.0 cm-1 |
| 2s2 2p5 5f1 3D2.0 | 15253900.0 cm-1 |
| 2s2 2p5 5f1 1G4.0 | 15254900.0 cm-1 |
| 2s2 2p5 5f1 3G5.0 | 15256300.0 cm-1 |
| 2s2 2p5 5f1 3F3.0 | 15257000.0 cm-1 |
| 2s2 2p5 5f1 1D2.0 | 15257600.0 cm-1 |
| 2s2 2p5 5f1 1F3.0 | 15257600.0 cm-1 |
| 2s2 2p5 5g1 3F2.0 | 15258900.0 cm-1 |
| 2s2 2p5 5f1 3F4.0 | 15259300.0 cm-1 |
| 2s2 2p5 5g1 3F3.0 | 15259400.0 cm-1 |
| 2s2 2p5 5g1 1H5.0 | 15261400.0 cm-1 |
| 2s2 2p5 5g1 3G3.0 | 15261600.0 cm-1 |
| 2s2 2p5 5g1 1G4.0 | 15262300.0 cm-1 |
| 2s2 2p5 5g1 3H6.0 | 15262700.0 cm-1 |
| 2s2 2p5 5g1 3G4.0 | 15262800.0 cm-1 |
| 2s2 2p5 5g1 3G5.0 | 15263900.0 cm-1 |
| 2s2 2p5 5s1 3P0.0 | 15303000.0 cm-1 |
| 2s2 2p5 5s1 3P1.0 | 15304300.0 cm-1 |
| 2s2 2p5 5p1 3D1.0 | 15371400.0 cm-1 |
| 2s2 2p5 5p1 1D2.0 | 15383100.0 cm-1 |
| 2s2 2p5 5p1 3P1.0 | 15385100.0 cm-1 |
| 2s2 2p5 5p1 3P0.0 | 15389900.0 cm-1 |
| 2s1 2p6 4d1 3D1.0 | 15399300.0 cm-1 |
| 2s1 2p6 4d1 3D2.0 | 15399900.0 cm-1 |
| 2s1 2p6 4d1 3D3.0 | 15401300.0 cm-1 |
| 2s1 2p6 4d1 1D2.0 | 15420600.0 cm-1 |
| 2s2 2p5 5d1 3F2.0 | 15471000.0 cm-1 |
| 2s2 2p5 5d1 3P2.0 | 15474400.0 cm-1 |
| 2s2 2p5 5d1 1F3.0 | 15475900.0 cm-1 |
| 2s2 2p5 5d1 3D1.0 | 15483400.0 cm-1 |
| 2s1 2p6 4f1 3F3.0 | 15485200.0 cm-1 |
| 2s1 2p6 4f1 3F4.0 | 15486600.0 cm-1 |
| 2s1 2p6 4f1 3F2.0 | 15490900.0 cm-1 |
| 2s1 2p6 4f1 1F3.0 | 15494900.0 cm-1 |
| 2s2 2p5 5f1 3G3.0 | 15518700.0 cm-1 |
| 2s2 2p5 5f1 3F2.0 | 15520300.0 cm-1 |
| 2s2 2p5 5f1 3G4.0 | 15520500.0 cm-1 |
| 2s2 2p5 5f1 3D3.0 | 15521300.0 cm-1 |
| 2s2 2p5 5g1 3H4.0 | 15525200.0 cm-1 |
| 2s2 2p5 5g1 3H5.0 | 15526200.0 cm-1 |
| 2s2 2p5 5g1 1F3.0 | 15531000.0 cm-1 |
| 2s2 2p5 5g1 3F4.0 | 15532100.0 cm-1 |
| 2s2 2p5 6s1 3P2.0 | 15847900.0 cm-1 |
| 2s2 2p5 6s1 1P1.0 | 15849300.0 cm-1 |
| 2s2 2p5 6p1 3S1.0 | 15888600.0 cm-1 |
| 2s2 2p5 6p1 3D2.0 | 15890000.0 cm-1 |
| 2s2 2p5 6p1 3D3.0 | 15894900.0 cm-1 |
| 2s2 2p5 6p1 1P1.0 | 15895500.0 cm-1 |
| 2s2 2p5 6p1 3P2.0 | 15897500.0 cm-1 |
| 2s2 2p5 6p1 1S0.0 | 15910000.0 cm-1 |
| 2s2 2p5 6d1 3P0.0 | 15940600.0 cm-1 |
| 2s2 2p5 6d1 3P1.0 | 15942200.0 cm-1 |
| 2s2 2p5 6d1 3F3.0 | 15944200.0 cm-1 |
| 2s2 2p5 6d1 3F4.0 | 15944600.0 cm-1 |
| 2s2 2p5 6d1 3D2.0 | 15944800.0 cm-1 |
| 2s2 2p5 6d1 1D2.0 | 15946400.0 cm-1 |
| 2s2 2p5 6d1 3D3.0 | 15948200.0 cm-1 |
| 2s2 2p5 6d1 1P1.0 | 15957000.0 cm-1 |
| 2s2 2p5 6s1 3P0.0 | 16110000.0 cm-1 |
| 2s2 2p5 6s1 3P1.0 | 16110800.0 cm-1 |
| 2s2 2p5 6p1 3D1.0 | 16151500.0 cm-1 |
| 2s2 2p5 6p1 3P1.0 | 16157500.0 cm-1 |
| 2s2 2p5 6p1 1D2.0 | 16158200.0 cm-1 |
| 2s2 2p5 6p1 3P0.0 | 16159400.0 cm-1 |
| 2s2 2p5 6d1 3F2.0 | 16205800.0 cm-1 |
| 2s2 2p5 6d1 3P2.0 | 16207600.0 cm-1 |
| 2s2 2p5 6d1 1F3.0 | 16208700.0 cm-1 |
| 2s2 2p5 6d1 3D1.0 | 16212300.0 cm-1 |
| 2s2 2p5 7s1 3P2.0 | 16324200.0 cm-1 |
| 2s2 2p5 7s1 1P1.0 | 16325100.0 cm-1 |
| 2s2 2p5 7p1 3S1.0 | 16349500.0 cm-1 |
| 2s2 2p5 7p1 3D2.0 | 16350400.0 cm-1 |
| 2s2 2p5 7p1 3D3.0 | 16353300.0 cm-1 |
| 2s2 2p5 7p1 1P1.0 | 16353700.0 cm-1 |
| 2s2 2p5 7p1 3P2.0 | 16354900.0 cm-1 |
| 2s2 2p5 7p1 1S0.0 | 16362600.0 cm-1 |
| 2s2 2p5 7d1 3P0.0 | 16381700.0 cm-1 |
| 2s2 2p5 7d1 3P1.0 | 16382700.0 cm-1 |
| 2s2 2p5 7d1 3F3.0 | 16383900.0 cm-1 |
| 2s2 2p5 7d1 3F4.0 | 16384100.0 cm-1 |
| 2s2 2p5 7d1 3D2.0 | 16384200.0 cm-1 |
| 2s2 2p5 7d1 1D2.0 | 16385200.0 cm-1 |
| 2s2 2p5 7d1 3D3.0 | 16386300.0 cm-1 |
| 2s2 2p5 7d1 1P1.0 | 16391800.0 cm-1 |
| 2s1 2p6 5s1 3S1.0 | 16583500.0 cm-1 |
| 2s2 2p5 7s1 3P0.0 | 16586100.0 cm-1 |
| 2s2 2p5 7s1 3P1.0 | 16586600.0 cm-1 |
| 2s1 2p6 5s1 1S0.0 | 16593700.0 cm-1 |
| 2s2 2p5 7p1 3D1.0 | 16612200.0 cm-1 |
| 2s2 2p5 7p1 1D2.0 | 16616100.0 cm-1 |
| 2s2 2p5 7p1 3P1.0 | 16616400.0 cm-1 |
| 2s2 2p5 7p1 3P0.0 | 16616900.0 cm-1 |
| 2s2 2p5 7d1 3F2.0 | 16645600.0 cm-1 |
| 2s2 2p5 7d1 3P2.0 | 16646600.0 cm-1 |
| 2s2 2p5 7d1 1F3.0 | 16647400.0 cm-1 |
| 2s2 2p5 7d1 3D1.0 | 16649300.0 cm-1 |
| 2s1 2p6 5p1 3P0.0 | 16657600.0 cm-1 |
| 2s1 2p6 5p1 3P1.0 | 16658700.0 cm-1 |
| 2s1 2p6 5p1 3P2.0 | 16668100.0 cm-1 |
| 2s1 2p6 5p1 1P1.0 | 16670800.0 cm-1 |
| 2s1 2p6 5d1 3D1.0 | 16752300.0 cm-1 |
| 2s1 2p6 5d1 3D2.0 | 16753300.0 cm-1 |
| 2s1 2p6 5d1 3D3.0 | 16755400.0 cm-1 |
| 2s1 2p6 5d1 1D2.0 | 16763600.0 cm-1 |
| 2s1 2p6 5f1 3F2.0 | 16798700.0 cm-1 |
| 2s1 2p6 5f1 3F3.0 | 16799000.0 cm-1 |
| 2s1 2p6 5f1 3F4.0 | 16800100.0 cm-1 |
| 2s1 2p6 5f1 1F3.0 | 16801300.0 cm-1 |
| 2s1 2p6 5g1 3G3.0 | 16804900.0 cm-1 |
| 2s1 2p6 5g1 3G4.0 | 16804900.0 cm-1 |
| 2s1 2p6 5g1 3G5.0 | 16805700.0 cm-1 |
| 2s1 2p6 5g1 1G4.0 | 16805800.0 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 = 1.56998 2P = 1.13722 3S = 1.38861 3P = 1.14226 3D = 1.08194 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 618.5643 Rydbergs (8416.185866 eV) A fine energy mesh of 0.000005 Z**2 Rydbergs (0.03292652 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.002000 Z**2 Rydbergs (13.170608 eV) was used from the last threshold up to 0.917953 Z**2 Rydbergs (6045 eV) in the excitation calculation. A coarse energy mesh of 0.002000 Z**2 Rydbergs (13.170608 eV) was used from first threshold up to 0.917953 Z**2 Rydbergs (6045 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: 11/11/09 ------------------------------------------------------------------------