lilike_lgy10#zn27.dat
Resolved Specific Ion Data Collections
- Ion
- Zn27+
- Temperature Range
- 13.53 eV → 1.353 x 105 eV
ADF04
- Filename
- lilike_lgy10#zn27.dat
- Full Path
- adf04/copaw#li/lilike_lgy10#zn27.dat
Download data
- Spontaneous Emission: Zn+27(i) → Zn+27(j) + hv
- Electron Impact Excitation: Zn+27(i) + e → Zn+27(j) + e
| 2s1 2S0.5 | 0.0 cm-1 |
| 2p1 2P0.5 | 462814.0 cm-1 |
| 2p1 2P1.5 | 697727.0 cm-1 |
| 3s1 2S0.5 | 12604300.0 cm-1 |
| 3p1 2P0.5 | 12732400.0 cm-1 |
| 3p1 2P1.5 | 12800100.0 cm-1 |
| 3d1 2D1.5 | 12851900.0 cm-1 |
| 3d1 2D2.5 | 12874100.0 cm-1 |
| 4s1 2S0.5 | 16949100.0 cm-1 |
| 4p1 2P0.5 | 17001800.0 cm-1 |
| 4p1 2P1.5 | 17029600.0 cm-1 |
| 4d1 2D1.5 | 17051000.0 cm-1 |
| 4d1 2D2.5 | 17060300.0 cm-1 |
| 4f1 2F2.5 | 17061500.0 cm-1 |
| 4f1 2F3.5 | 17066100.0 cm-1 |
| 5s1 2S0.5 | 18943700.0 cm-1 |
| 5p1 2P0.5 | 18970300.0 cm-1 |
| 5p1 2P1.5 | 18984000.0 cm-1 |
| 5d1 2D1.5 | 18994800.0 cm-1 |
| 5d1 2D2.5 | 18999500.0 cm-1 |
| 5f1 2F2.5 | 19000200.0 cm-1 |
| 5f1 2F3.5 | 19002600.0 cm-1 |
| 5g1 2G3.5 | 19002600.0 cm-1 |
| 5g1 2G4.5 | 19004000.0 cm-1 |
| 1s1 2s2 2S0.5 | 71709100.0 cm-1 |
| 1s1 2s1 2p1 4P0.5 | 71819100.0 cm-1 |
| 1s1 2s1 2p1 4P1.5 | 71878900.0 cm-1 |
| 1s1 2s1 2p1 4P2.5 | 72041400.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 72210000.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 72354000.0 cm-1 |
| 1s1 2p2 4P0.5 | 72397900.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 72481700.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 72517700.0 cm-1 |
| 1s1 2p2 4P1.5 | 72519800.0 cm-1 |
| 1s1 2p2 4P2.5 | 72605100.0 cm-1 |
| 1s1 2p2 2D1.5 | 72759700.0 cm-1 |
| 1s1 2p2 2P0.5 | 72764700.0 cm-1 |
| 1s1 2p2 2D2.5 | 72876800.0 cm-1 |
| 1s1 2p2 2P1.5 | 73012200.0 cm-1 |
| 1s1 2p2 2S0.5 | 73181000.0 cm-1 |
| 1s1 2s1 3s1 4S1.5 | 84489300.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 84617100.0 cm-1 |
| 1s1 2s1 3p1 4P0.5 | 84652700.0 cm-1 |
| 1s1 2s1 3p1 4P1.5 | 84659200.0 cm-1 |
| 1s1 2s1 3p1 4P2.5 | 84713400.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 84723000.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 84723400.0 cm-1 |
| 1s1 2s1 3d1 4D0.5 | 84799500.0 cm-1 |
| 1s1 2s1 3d1 4D1.5 | 84807200.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 84812600.0 cm-1 |
| 1s1 2s1 3d1 4D2.5 | 84818300.0 cm-1 |
| 1s1 2s1 3d1 4D3.5 | 84833300.0 cm-1 |
| 1s1 2p1 3s1 4P0.5 | 84848200.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 84882700.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 84884200.0 cm-1 |
| 1s1 2p1 3s1 4P1.5 | 84890900.0 cm-1 |
| 1s1 2p1 3p1 4D0.5 | 84923300.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 84929700.0 cm-1 |
| 1s1 2p1 3p1 4D1.5 | 84954700.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 84989600.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 84999100.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 85032300.0 cm-1 |
| 1s1 2p1 3p1 4D2.5 | 85044500.0 cm-1 |
| 1s1 2p1 3s1 4P2.5 | 85060600.0 cm-1 |
| 1s1 2p1 3p1 4P0.5 | 85065600.0 cm-1 |
| 1s1 2p1 3d1 4F1.5 | 85079700.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 85085500.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 85107000.0 cm-1 |
| 1s1 2p1 3d1 4F2.5 | 85110400.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 85118200.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 85138500.0 cm-1 |
| 1s1 2p1 3d1 4D2.5 | 85155600.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 85170300.0 cm-1 |
| 1s1 2p1 3d1 4F3.5 | 85171200.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 85180400.0 cm-1 |
| 1s1 2p1 3d1 4D0.5 | 85198200.0 cm-1 |
| 1s1 2p1 3d1 4D1.5 | 85200700.0 cm-1 |
| 1s1 2p1 3p1 4P1.5 | 85202700.0 cm-1 |
| 1s1 2p1 3p1 4D3.5 | 85206000.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 85207000.0 cm-1 |
| 1s1 2p1 3p1 4P2.5 | 85227900.0 cm-1 |
| 1s1 2p1 3p1 4S1.5 | 85245400.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 85261100.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 85268400.0 cm-1 |
| 1s1 2p1 3d1 4F4.5 | 85320200.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 85321000.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 85323800.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 85339500.0 cm-1 |
| 1s1 2p1 3d1 4D3.5 | 85357400.0 cm-1 |
| 1s1 2p1 3d1 4P1.5 | 85375700.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 85382500.0 cm-1 |
| 1s1 2p1 3d1 4P0.5 | 85383600.0 cm-1 |
| 1s1 2p1 3d1 4P2.5 | 85385100.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 85386100.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 85408100.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 85410400.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 85416300.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 85458600.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 85468200.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 85504500.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 85517900.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 85525700.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 85543400.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 85568100.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 85576300.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 85606200.0 cm-1 |
| 1s1 2s1 4s1 4S1.5 | 88948200.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 88989700.0 cm-1 |
| 1s1 2s1 4p1 4P0.5 | 89008300.0 cm-1 |
| 1s1 2s1 4p1 4P1.5 | 89012400.0 cm-1 |
| 1s1 2s1 4p1 4P2.5 | 89031600.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 89044700.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 89048200.0 cm-1 |
| 1s1 2s1 4d1 4D0.5 | 89070400.0 cm-1 |
| 1s1 2s1 4d1 4D1.5 | 89071900.0 cm-1 |
| 1s1 2s1 4d1 4D2.5 | 89074800.0 cm-1 |
| 1s1 2s1 4d1 4D3.5 | 89080200.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 89095600.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 89097600.0 cm-1 |
| 1s1 2s1 4f1 4F1.5 | 89109000.0 cm-1 |
| 1s1 2s1 4f1 4F2.5 | 89109800.0 cm-1 |
| 1s1 2s1 4f1 4F3.5 | 89111000.0 cm-1 |
| 1s1 2s1 4f1 4F4.5 | 89114000.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 89118000.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 89119100.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 89240300.0 cm-1 |
| 1s1 2p1 4s1 4P0.5 | 89246100.0 cm-1 |
| 1s1 2p1 4s1 4P1.5 | 89279500.0 cm-1 |
| 1s1 2p1 4p1 4D0.5 | 89283000.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 89291300.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 89308000.0 cm-1 |
| 1s1 2p1 4p1 4D1.5 | 89312500.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 89320500.0 cm-1 |
| 1s1 2p1 4p1 4S1.5 | 89327100.0 cm-1 |
| 1s1 2p1 4d1 4F1.5 | 89346600.0 cm-1 |
| 1s1 2p1 4p1 4P0.5 | 89349000.0 cm-1 |
| 1s1 2p1 4p1 4D2.5 | 89350100.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 89357900.0 cm-1 |
| 1s1 2p1 4d1 4F2.5 | 89366400.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 89367600.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 89370600.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 89372100.0 cm-1 |
| 1s1 2p1 4d1 4D2.5 | 89379000.0 cm-1 |
| 1s1 2p1 4f1 4G2.5 | 89382500.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 89388200.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 89392000.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 89395400.0 cm-1 |
| 1s1 2p1 4d1 4D1.5 | 89401900.0 cm-1 |
| 1s1 2p1 4d1 4F3.5 | 89404200.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 89405700.0 cm-1 |
| 1s1 2p1 4d1 4D0.5 | 89406400.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 89413500.0 cm-1 |
| 1s1 2p1 4f1 4G3.5 | 89419100.0 cm-1 |
| 1s1 2p1 4f1 4F1.5 | 89421100.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 89423500.0 cm-1 |
| 1s1 2p1 4f1 4G4.5 | 89425900.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 89427100.0 cm-1 |
| 1s1 2p1 4f1 4D3.5 | 89431400.0 cm-1 |
| 1s1 2p1 4s1 4P2.5 | 89472100.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 89498600.0 cm-1 |
| 1s1 2p1 4p1 4P1.5 | 89524500.0 cm-1 |
| 1s1 2p1 4p1 4P2.5 | 89528700.0 cm-1 |
| 1s1 2p1 4p1 4D3.5 | 89533300.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 89549000.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 89568100.0 cm-1 |
| 1s1 2p1 4d1 4F4.5 | 89579000.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 89581200.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 89582300.0 cm-1 |
| 1s1 2p1 4d1 4D3.5 | 89585400.0 cm-1 |
| 1s1 2p1 4d1 4P1.5 | 89591900.0 cm-1 |
| 1s1 2p1 4d1 4P0.5 | 89595000.0 cm-1 |
| 1s1 2p1 4d1 4P2.5 | 89597400.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 89604800.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 89609300.0 cm-1 |
| 1s1 2p1 4f1 4F2.5 | 89612500.0 cm-1 |
| 1s1 2p1 4f1 4F4.5 | 89612800.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 89613300.0 cm-1 |
| 1s1 2p1 4f1 4F3.5 | 89616400.0 cm-1 |
| 1s1 2p1 4f1 4D1.5 | 89619200.0 cm-1 |
| 1s1 2p1 4f1 4G5.5 | 89619800.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 89621800.0 cm-1 |
| 1s1 2p1 4f1 4D2.5 | 89622900.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 89623400.0 cm-1 |
| 1s1 2p1 4f1 4D0.5 | 89624100.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 89631200.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 89643100.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 89643200.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 89687900.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 89688500.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 89706300.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 89715400.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 89726200.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 89744100.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 89748200.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 89749400.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 89760400.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 89762000.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 89765800.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 89770000.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 89774500.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 89778400.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 89780200.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 89783200.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 89788700.0 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 = 1.28301 2S = 1.04839 2P = 0.95206 3S = 1.03473 3P = 0.94290 3D = 0.88518 4S = 1.03326 4P = 0.94263 4D = 0.88661 4F = 1.05384 5S = 1.03535 5P = 0.94453 5D = 0.89020 5F = 0.86629 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 2674.3636 Rydbergs (36387.391142 eV) A fine energy mesh of 0.000004 Z**2 Rydbergs (0.039675096 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (99.18774 eV) was used from the last threshold up to 2.739250 Z**2 Rydbergs (27170 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (99.18774 eV) was used from first threshold up to 2.739250 Z**2 Rydbergs (27170 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: 11/10/10 ------------------------------------------------------------------------ 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 = 1.28823 2S = 1.05004 2P = 0.95394 3S = 1.03678 3P = 0.94486 3D = 0.88718 4S = 1.03671 4P = 0.94586 4D = 0.89118 4F = 1.04952 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 0.000004 Z**2 Rydbergs (0.039675096 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (99.18774 eV) was used from the last threshold up to 2.739250 Z**2 Rydbergs (27170 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (99.18774 eV) was used from first threshold up to 2.739250 Z**2 Rydbergs (27170 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 4.21767 3 6.39638 Produced by: Guiyun Liang Date: 12/08/10 ------------------------------------------------------------------------