nelike_lgy09#zn20.dat
Resolved Specific Ion Data Collections
- Ion
- Zn20+
- Temperature Range
- 7.600 eV → 7.600 x 104 eV
ADF04
- Filename
- nelike_lgy09#zn20.dat
- Full Path
- adf04/copaw#ne/nelike_lgy09#zn20.dat
Download data
- Spontaneous Emission: Zn+20(i) → Zn+20(j) + hv
- Electron Impact Excitation: Zn+20(i) + e → Zn+20(j) + e
| 2s2 2p6 1S0.0 | 0.0 cm-1 |
| 2s2 2p5 3s1 3P2.0 | 8483000.0 cm-1 |
| 2s2 2p5 3s1 1P1.0 | 8501620.0 cm-1 |
| 2s2 2p5 3s1 3P0.0 | 8678950.0 cm-1 |
| 2s2 2p5 3s1 3P1.0 | 8689680.0 cm-1 |
| 2s2 2p5 3p1 3S1.0 | 8797420.0 cm-1 |
| 2s2 2p5 3p1 3D2.0 | 8825650.0 cm-1 |
| 2s2 2p5 3p1 3D3.0 | 8858560.0 cm-1 |
| 2s2 2p5 3p1 1P1.0 | 8865550.0 cm-1 |
| 2s2 2p5 3p1 3P2.0 | 8887260.0 cm-1 |
| 2s2 2p5 3p1 3P0.0 | 8964620.0 cm-1 |
| 2s2 2p5 3p1 3D1.0 | 9015790.0 cm-1 |
| 2s2 2p5 3p1 3P1.0 | 9062430.0 cm-1 |
| 2s2 2p5 3p1 1D2.0 | 9068770.0 cm-1 |
| 2s2 2p5 3p1 1S0.0 | 9177080.0 cm-1 |
| 2s2 2p5 3d1 3P0.0 | 9263130.0 cm-1 |
| 2s2 2p5 3d1 3P1.0 | 9276190.0 cm-1 |
| 2s2 2p5 3d1 3P2.0 | 9299720.0 cm-1 |
| 2s2 2p5 3d1 3F4.0 | 9300150.0 cm-1 |
| 2s2 2p5 3d1 3F3.0 | 9302080.0 cm-1 |
| 2s2 2p5 3d1 1D2.0 | 9321090.0 cm-1 |
| 2s2 2p5 3d1 3D3.0 | 9336840.0 cm-1 |
| 2s2 2p5 3d1 3D1.0 | 9394290.0 cm-1 |
| 2s2 2p5 3d1 3F2.0 | 9495780.0 cm-1 |
| 2s2 2p5 3d1 3D2.0 | 9508960.0 cm-1 |
| 2s2 2p5 3d1 1F3.0 | 9516770.0 cm-1 |
| 2s2 2p5 3d1 1P1.0 | 9580820.0 cm-1 |
| 2s1 2p6 3s1 3S1.0 | 9878960.0 cm-1 |
| 2s1 2p6 3s1 1S0.0 | 9947420.0 cm-1 |
| 2s1 2p6 3p1 3P0.0 | 10210300.0 cm-1 |
| 2s1 2p6 3p1 3P1.0 | 10216100.0 cm-1 |
| 2s1 2p6 3p1 3P2.0 | 10256000.0 cm-1 |
| 2s1 2p6 3p1 1P1.0 | 10273700.0 cm-1 |
| 2s1 2p6 3d1 3D1.0 | 10674800.0 cm-1 |
| 2s1 2p6 3d1 3D2.0 | 10679000.0 cm-1 |
| 2s1 2p6 3d1 3D3.0 | 10686700.0 cm-1 |
| 2s1 2p6 3d1 1D2.0 | 10734300.0 cm-1 |
| 2s2 2p5 4s1 3P2.0 | 11466500.0 cm-1 |
| 2s2 2p5 4s1 1P1.0 | 11471900.0 cm-1 |
| 2s2 2p5 4p1 3S1.0 | 11594600.0 cm-1 |
| 2s2 2p5 4p1 3D2.0 | 11601500.0 cm-1 |
| 2s2 2p5 4p1 3D3.0 | 11614100.0 cm-1 |
| 2s2 2p5 4p1 1P1.0 | 11616600.0 cm-1 |
| 2s2 2p5 4p1 3P2.0 | 11623600.0 cm-1 |
| 2s2 2p5 4s1 3P0.0 | 11662600.0 cm-1 |
| 2s2 2p5 4p1 3P0.0 | 11664300.0 cm-1 |
| 2s2 2p5 4s1 3P1.0 | 11665300.0 cm-1 |
| 2s2 2p5 4d1 3P0.0 | 11765600.0 cm-1 |
| 2s2 2p5 4d1 3P1.0 | 11770800.0 cm-1 |
| 2s2 2p5 4d1 3F4.0 | 11778300.0 cm-1 |
| 2s2 2p5 4d1 3F3.0 | 11778500.0 cm-1 |
| 2s2 2p5 4d1 3P2.0 | 11779300.0 cm-1 |
| 2s2 2p5 4d1 1D2.0 | 11785300.0 cm-1 |
| 2s2 2p5 4d1 3D3.0 | 11791100.0 cm-1 |
| 2s2 2p5 4p1 3D1.0 | 11795300.0 cm-1 |
| 2s2 2p5 4p1 3P1.0 | 11812300.0 cm-1 |
| 2s2 2p5 4p1 1D2.0 | 11814800.0 cm-1 |
| 2s2 2p5 4d1 1P1.0 | 11818200.0 cm-1 |
| 2s2 2p5 4p1 1S0.0 | 11832000.0 cm-1 |
| 2s2 2p5 4f1 3D1.0 | 11858800.0 cm-1 |
| 2s2 2p5 4f1 1G4.0 | 11860300.0 cm-1 |
| 2s2 2p5 4f1 3D2.0 | 11861100.0 cm-1 |
| 2s2 2p5 4f1 3G5.0 | 11861900.0 cm-1 |
| 2s2 2p5 4f1 1D2.0 | 11865400.0 cm-1 |
| 2s2 2p5 4f1 3F3.0 | 11865400.0 cm-1 |
| 2s2 2p5 4f1 1F3.0 | 11866100.0 cm-1 |
| 2s2 2p5 4f1 3F4.0 | 11868000.0 cm-1 |
| 2s2 2p5 4d1 3F2.0 | 11973100.0 cm-1 |
| 2s2 2p5 4d1 3D2.0 | 11978100.0 cm-1 |
| 2s2 2p5 4d1 1F3.0 | 11981500.0 cm-1 |
| 2s2 2p5 4d1 3D1.0 | 11998800.0 cm-1 |
| 2s2 2p5 4f1 3G3.0 | 12058200.0 cm-1 |
| 2s2 2p5 4f1 3F2.0 | 12060300.0 cm-1 |
| 2s2 2p5 4f1 3G4.0 | 12060500.0 cm-1 |
| 2s2 2p5 4f1 3D3.0 | 12061300.0 cm-1 |
| 2s2 2p5 5s1 3P2.0 | 12758700.0 cm-1 |
| 2s2 2p5 5s1 1P1.0 | 12761300.0 cm-1 |
| 2s2 2p5 5p1 3S1.0 | 12816100.0 cm-1 |
| 2s2 2p5 5p1 3D2.0 | 12826100.0 cm-1 |
| 2s2 2p5 5p1 1P1.0 | 12832300.0 cm-1 |
| 2s2 2p5 5p1 3D3.0 | 12832400.0 cm-1 |
| 2s2 2p5 5p1 3P2.0 | 12836900.0 cm-1 |
| 2s2 2p5 5p1 1S0.0 | 12853700.0 cm-1 |
| 2s1 2p6 4s1 3S1.0 | 12854600.0 cm-1 |
| 2s1 2p6 4s1 1S0.0 | 12870500.0 cm-1 |
| 2s2 2p5 5d1 3P0.0 | 12906100.0 cm-1 |
| 2s2 2p5 5d1 3P1.0 | 12908700.0 cm-1 |
| 2s2 2p5 5d1 3F3.0 | 12912400.0 cm-1 |
| 2s2 2p5 5d1 3F4.0 | 12912600.0 cm-1 |
| 2s2 2p5 5d1 3P2.0 | 12913000.0 cm-1 |
| 2s2 2p5 5d1 1D2.0 | 12915500.0 cm-1 |
| 2s2 2p5 5d1 3D3.0 | 12918400.0 cm-1 |
| 2s2 2p5 5d1 1P1.0 | 12931500.0 cm-1 |
| 2s2 2p5 5s1 3P0.0 | 12951100.0 cm-1 |
| 2s2 2p5 5f1 3D1.0 | 12951200.0 cm-1 |
| 2s2 2p5 5f1 3D2.0 | 12952700.0 cm-1 |
| 2s2 2p5 5f1 1G4.0 | 12953300.0 cm-1 |
| 2s2 2p5 5f1 3G5.0 | 12954100.0 cm-1 |
| 2s2 2p5 5s1 3P1.0 | 12954600.0 cm-1 |
| 2s2 2p5 5f1 3D3.0 | 12955200.0 cm-1 |
| 2s2 2p5 5f1 1D2.0 | 12955700.0 cm-1 |
| 2s2 2p5 5f1 1F3.0 | 12955800.0 cm-1 |
| 2s2 2p5 5g1 3F2.0 | 12956900.0 cm-1 |
| 2s2 2p5 5f1 3F4.0 | 12957000.0 cm-1 |
| 2s2 2p5 5g1 3F3.0 | 12957300.0 cm-1 |
| 2s2 2p5 5g1 1H5.0 | 12958700.0 cm-1 |
| 2s2 2p5 5g1 3G3.0 | 12959100.0 cm-1 |
| 2s2 2p5 5g1 1G4.0 | 12959600.0 cm-1 |
| 2s2 2p5 5g1 3H6.0 | 12959600.0 cm-1 |
| 2s2 2p5 5g1 3G4.0 | 12960000.0 cm-1 |
| 2s2 2p5 5g1 3G5.0 | 12960800.0 cm-1 |
| 2s1 2p6 4p1 3P1.0 | 12983600.0 cm-1 |
| 2s1 2p6 4p1 3P0.0 | 12984900.0 cm-1 |
| 2s1 2p6 4p1 3P2.0 | 12996700.0 cm-1 |
| 2s1 2p6 4p1 1P1.0 | 13003400.0 cm-1 |
| 2s2 2p5 5p1 3D1.0 | 13021300.0 cm-1 |
| 2s2 2p5 5p1 3P1.0 | 13030400.0 cm-1 |
| 2s2 2p5 5p1 1D2.0 | 13030500.0 cm-1 |
| 2s2 2p5 5p1 3P0.0 | 13036600.0 cm-1 |
| 2s2 2p5 5d1 3F2.0 | 13108000.0 cm-1 |
| 2s2 2p5 5d1 3D2.0 | 13110600.0 cm-1 |
| 2s2 2p5 5d1 1F3.0 | 13112000.0 cm-1 |
| 2s2 2p5 5d1 3D1.0 | 13119500.0 cm-1 |
| 2s2 2p5 5f1 3F3.0 | 13145800.0 cm-1 |
| 2s2 2p5 5f1 3F2.0 | 13147400.0 cm-1 |
| 2s2 2p5 5f1 3G3.0 | 13150200.0 cm-1 |
| 2s2 2p5 5f1 3G4.0 | 13151500.0 cm-1 |
| 2s2 2p5 5g1 1F3.0 | 13153400.0 cm-1 |
| 2s2 2p5 5g1 3F4.0 | 13154000.0 cm-1 |
| 2s1 2p6 4d1 3D1.0 | 13154900.0 cm-1 |
| 2s2 2p5 5g1 3H4.0 | 13155600.0 cm-1 |
| 2s2 2p5 5g1 3H5.0 | 13156300.0 cm-1 |
| 2s1 2p6 4d1 3D2.0 | 13159900.0 cm-1 |
| 2s1 2p6 4d1 3D3.0 | 13164600.0 cm-1 |
| 2s1 2p6 4d1 1D2.0 | 13175500.0 cm-1 |
| 2s1 2p6 4f1 3F2.0 | 13238500.0 cm-1 |
| 2s1 2p6 4f1 3F3.0 | 13240000.0 cm-1 |
| 2s1 2p6 4f1 3F4.0 | 13242100.0 cm-1 |
| 2s1 2p6 4f1 1F3.0 | 13242400.0 cm-1 |
| 2s2 2p5 6s1 3P2.0 | 13441800.0 cm-1 |
| 2s2 2p5 6s1 1P1.0 | 13443100.0 cm-1 |
| 2s2 2p5 6p1 3S1.0 | 13478400.0 cm-1 |
| 2s2 2p5 6p1 3D2.0 | 13479900.0 cm-1 |
| 2s2 2p5 6p1 3D3.0 | 13483200.0 cm-1 |
| 2s2 2p5 6p1 1P1.0 | 13483900.0 cm-1 |
| 2s2 2p5 6p1 3P2.0 | 13485600.0 cm-1 |
| 2s2 2p5 6p1 1S0.0 | 13497100.0 cm-1 |
| 2s2 2p5 6d1 3P0.0 | 13524800.0 cm-1 |
| 2s2 2p5 6d1 3P1.0 | 13526200.0 cm-1 |
| 2s2 2p5 6d1 3F4.0 | 13528100.0 cm-1 |
| 2s2 2p5 6d1 3F3.0 | 13528100.0 cm-1 |
| 2s2 2p5 6d1 3D2.0 | 13528500.0 cm-1 |
| 2s2 2p5 6d1 1D2.0 | 13529900.0 cm-1 |
| 2s2 2p5 6d1 3D3.0 | 13531400.0 cm-1 |
| 2s2 2p5 6d1 1P1.0 | 13539400.0 cm-1 |
| 2s2 2p5 6s1 3P0.0 | 13636900.0 cm-1 |
| 2s2 2p5 6s1 3P1.0 | 13637600.0 cm-1 |
| 2s2 2p5 6p1 3D1.0 | 13674300.0 cm-1 |
| 2s2 2p5 6p1 3P1.0 | 13678800.0 cm-1 |
| 2s2 2p5 6p1 1D2.0 | 13679500.0 cm-1 |
| 2s2 2p5 6p1 3P0.0 | 13681800.0 cm-1 |
| 2s2 2p5 6d1 3F2.0 | 13722700.0 cm-1 |
| 2s2 2p5 6d1 3P2.0 | 13724100.0 cm-1 |
| 2s2 2p5 6d1 1F3.0 | 13725000.0 cm-1 |
| 2s2 2p5 6d1 3D1.0 | 13728800.0 cm-1 |
| 2s2 2p5 7s1 3P2.0 | 13841700.0 cm-1 |
| 2s2 2p5 7s1 1P1.0 | 13842500.0 cm-1 |
| 2s2 2p5 7p1 3S1.0 | 13864500.0 cm-1 |
| 2s2 2p5 7p1 3D2.0 | 13865300.0 cm-1 |
| 2s2 2p5 7p1 3D3.0 | 13867300.0 cm-1 |
| 2s2 2p5 7p1 1P1.0 | 13867700.0 cm-1 |
| 2s2 2p5 7p1 3P2.0 | 13868700.0 cm-1 |
| 2s2 2p5 7p1 1S0.0 | 13875900.0 cm-1 |
| 2s2 2p5 7d1 3P0.0 | 13893200.0 cm-1 |
| 2s2 2p5 7d1 3P1.0 | 13894000.0 cm-1 |
| 2s2 2p5 7d1 3F4.0 | 13895100.0 cm-1 |
| 2s2 2p5 7d1 3F3.0 | 13895100.0 cm-1 |
| 2s2 2p5 7d1 3D2.0 | 13895300.0 cm-1 |
| 2s2 2p5 7d1 1D2.0 | 13896200.0 cm-1 |
| 2s2 2p5 7d1 3D3.0 | 13897100.0 cm-1 |
| 2s2 2p5 7d1 1P1.0 | 13902200.0 cm-1 |
| 2s2 2p5 7s1 3P0.0 | 14036800.0 cm-1 |
| 2s2 2p5 7s1 3P1.0 | 14037200.0 cm-1 |
| 2s2 2p5 7p1 3D1.0 | 14060000.0 cm-1 |
| 2s2 2p5 7p1 3P1.0 | 14062500.0 cm-1 |
| 2s2 2p5 7p1 1D2.0 | 14063100.0 cm-1 |
| 2s2 2p5 7p1 3P0.0 | 14064500.0 cm-1 |
| 2s2 2p5 7d1 3F2.0 | 14089900.0 cm-1 |
| 2s2 2p5 7d1 3P2.0 | 14090700.0 cm-1 |
| 2s2 2p5 7d1 1F3.0 | 14091300.0 cm-1 |
| 2s2 2p5 7d1 3D1.0 | 14093600.0 cm-1 |
| 2s1 2p6 5s1 3S1.0 | 14137100.0 cm-1 |
| 2s1 2p6 5s1 1S0.0 | 14145700.0 cm-1 |
| 2s1 2p6 5p1 3P0.0 | 14203200.0 cm-1 |
| 2s1 2p6 5p1 3P1.0 | 14203900.0 cm-1 |
| 2s1 2p6 5p1 3P2.0 | 14210900.0 cm-1 |
| 2s1 2p6 5p1 1P1.0 | 14213500.0 cm-1 |
| 2s1 2p6 5d1 3D1.0 | 14287700.0 cm-1 |
| 2s1 2p6 5d1 3D2.0 | 14288400.0 cm-1 |
| 2s1 2p6 5d1 3D3.0 | 14289900.0 cm-1 |
| 2s1 2p6 5d1 1D2.0 | 14297500.0 cm-1 |
| 2s1 2p6 5f1 3F2.0 | 14328800.0 cm-1 |
| 2s1 2p6 5f1 3F3.0 | 14329100.0 cm-1 |
| 2s1 2p6 5f1 3F4.0 | 14329900.0 cm-1 |
| 2s1 2p6 5f1 1F3.0 | 14330900.0 cm-1 |
| 2s1 2p6 5g1 3G3.0 | 14334000.0 cm-1 |
| 2s1 2p6 5g1 3G4.0 | 14334000.0 cm-1 |
| 2s1 2p6 5g1 3G5.0 | 14334600.0 cm-1 |
| 2s1 2p6 5g1 1G4.0 | 14334700.0 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 = 1.44425 2P = 1.10831 3S = 1.32832 3P = 1.11769 3D = 1.07230 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 518.7332 Rydbergs (7057.883919 eV) A fine energy mesh of 0.000010 Z**2 Rydbergs (0.054424 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.002000 Z**2 Rydbergs (10.8848 eV) was used from the last threshold up to 0.933779 Z**2 Rydbergs (5082 eV) in the excitation calculation. A coarse energy mesh of 0.002000 Z**2 Rydbergs (10.8848 eV) was used from first threshold up to 0.933779 Z**2 Rydbergs (5082 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: 09/11/09 ------------------------------------------------------------------------