lilike_lgy10#cu26.dat
Resolved Specific Ion Data Collections
- Ion
- Cu26+
- Temperature Range
- 12.58 eV → 1.258 x 105 eV
ADF04
- Filename
- lilike_lgy10#cu26.dat
- Full Path
- adf04/copaw#li/lilike_lgy10#cu26.dat
Download data
- Spontaneous Emission: Cu+26(i) → Cu+26(j) + hv
- Electron Impact Excitation: Cu+26(i) + e → Cu+26(j) + e
| 2s1 2S0.5 | 0.0 cm-1 |
| 2p1 2P0.5 | 444923.0 cm-1 |
| 2p1 2P1.5 | 648063.0 cm-1 |
| 3s1 2S0.5 | 11721800.0 cm-1 |
| 3p1 2P0.5 | 11845000.0 cm-1 |
| 3p1 2P1.5 | 11903700.0 cm-1 |
| 3d1 2D1.5 | 11953300.0 cm-1 |
| 3d1 2D2.5 | 11972600.0 cm-1 |
| 4s1 2S0.5 | 15761500.0 cm-1 |
| 4p1 2P0.5 | 15812200.0 cm-1 |
| 4p1 2P1.5 | 15836300.0 cm-1 |
| 4d1 2D1.5 | 15856800.0 cm-1 |
| 4d1 2D2.5 | 15864800.0 cm-1 |
| 4f1 2F2.5 | 15866000.0 cm-1 |
| 4f1 2F3.5 | 15870000.0 cm-1 |
| 5s1 2S0.5 | 17615900.0 cm-1 |
| 5p1 2P0.5 | 17641500.0 cm-1 |
| 5p1 2P1.5 | 17653400.0 cm-1 |
| 5d1 2D1.5 | 17663800.0 cm-1 |
| 5d1 2D2.5 | 17667900.0 cm-1 |
| 5f1 2F2.5 | 17668500.0 cm-1 |
| 5f1 2F3.5 | 17670600.0 cm-1 |
| 5g1 2G3.5 | 17670600.0 cm-1 |
| 5g1 2G4.5 | 17671800.0 cm-1 |
| 1s1 2s2 2S0.5 | 66855500.0 cm-1 |
| 1s1 2s1 2p1 4P0.5 | 66961600.0 cm-1 |
| 1s1 2s1 2p1 4P1.5 | 67015100.0 cm-1 |
| 1s1 2s1 2p1 4P2.5 | 67153500.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 67335800.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 67457800.0 cm-1 |
| 1s1 2p2 4P0.5 | 67511300.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 67581200.0 cm-1 |
| 1s1 2p2 4P1.5 | 67613000.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 67613400.0 cm-1 |
| 1s1 2p2 4P2.5 | 67690800.0 cm-1 |
| 1s1 2p2 2D1.5 | 67844300.0 cm-1 |
| 1s1 2p2 2P0.5 | 67853700.0 cm-1 |
| 1s1 2p2 2D2.5 | 67939400.0 cm-1 |
| 1s1 2p2 2P1.5 | 68065800.0 cm-1 |
| 1s1 2p2 2S0.5 | 68233700.0 cm-1 |
| 1s1 2s1 3s1 4S1.5 | 78748600.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 78870400.0 cm-1 |
| 1s1 2s1 3p1 4P0.5 | 78905300.0 cm-1 |
| 1s1 2s1 3p1 4P1.5 | 78911400.0 cm-1 |
| 1s1 2s1 3p1 4P2.5 | 78957700.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 78967300.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 78967400.0 cm-1 |
| 1s1 2s1 3d1 4D0.5 | 79041300.0 cm-1 |
| 1s1 2s1 3d1 4D1.5 | 79048000.0 cm-1 |
| 1s1 2s1 3d1 4D2.5 | 79057700.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 79057900.0 cm-1 |
| 1s1 2s1 3d1 4D3.5 | 79070800.0 cm-1 |
| 1s1 2p1 3s1 4P0.5 | 79092500.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 79119300.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 79120400.0 cm-1 |
| 1s1 2p1 3s1 4P1.5 | 79131400.0 cm-1 |
| 1s1 2p1 3p1 4D0.5 | 79165400.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 79170000.0 cm-1 |
| 1s1 2p1 3p1 4D1.5 | 79194300.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 79228600.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 79229700.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 79264000.0 cm-1 |
| 1s1 2p1 3p1 4D2.5 | 79272900.0 cm-1 |
| 1s1 2p1 3s1 4P2.5 | 79276100.0 cm-1 |
| 1s1 2p1 3p1 4P0.5 | 79297000.0 cm-1 |
| 1s1 2p1 3d1 4F1.5 | 79309500.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 79312800.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 79334800.0 cm-1 |
| 1s1 2p1 3d1 4F2.5 | 79337500.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 79345600.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 79362200.0 cm-1 |
| 1s1 2p1 3d1 4D2.5 | 79380100.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 79384600.0 cm-1 |
| 1s1 2p1 3d1 4F3.5 | 79391700.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 79401500.0 cm-1 |
| 1s1 2p1 3p1 4D3.5 | 79409400.0 cm-1 |
| 1s1 2p1 3p1 4P1.5 | 79413000.0 cm-1 |
| 1s1 2p1 3d1 4D0.5 | 79421000.0 cm-1 |
| 1s1 2p1 3d1 4D1.5 | 79423400.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 79428800.0 cm-1 |
| 1s1 2p1 3p1 4P2.5 | 79437000.0 cm-1 |
| 1s1 2p1 3p1 4S1.5 | 79448300.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 79470600.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 79478000.0 cm-1 |
| 1s1 2p1 3d1 4F4.5 | 79516800.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 79521200.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 79528500.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 79537900.0 cm-1 |
| 1s1 2p1 3d1 4D3.5 | 79554800.0 cm-1 |
| 1s1 2p1 3d1 4P1.5 | 79573500.0 cm-1 |
| 1s1 2p1 3d1 4P2.5 | 79580300.0 cm-1 |
| 1s1 2p1 3d1 4P0.5 | 79580600.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 79587600.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 79589700.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 79604200.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 79604300.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 79615000.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 79653700.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 79660300.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 79699700.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 79710900.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 79718100.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 79735300.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 79761100.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 79765100.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 79794800.0 cm-1 |
| 1s1 2s1 4s1 4S1.5 | 82898200.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 82937900.0 cm-1 |
| 1s1 2s1 4p1 4P0.5 | 82955800.0 cm-1 |
| 1s1 2s1 4p1 4P1.5 | 82959600.0 cm-1 |
| 1s1 2s1 4p1 4P2.5 | 82975900.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 82988700.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 82991900.0 cm-1 |
| 1s1 2s1 4d1 4D0.5 | 83013300.0 cm-1 |
| 1s1 2s1 4d1 4D1.5 | 83014700.0 cm-1 |
| 1s1 2s1 4d1 4D2.5 | 83017200.0 cm-1 |
| 1s1 2s1 4d1 4D3.5 | 83021800.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 83037000.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 83038700.0 cm-1 |
| 1s1 2s1 4f1 4F1.5 | 83049700.0 cm-1 |
| 1s1 2s1 4f1 4F2.5 | 83050400.0 cm-1 |
| 1s1 2s1 4f1 4F3.5 | 83051500.0 cm-1 |
| 1s1 2s1 4f1 4F4.5 | 83054000.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 83058000.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 83059000.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 83177900.0 cm-1 |
| 1s1 2p1 4s1 4P0.5 | 83184400.0 cm-1 |
| 1s1 2p1 4s1 4P1.5 | 83214900.0 cm-1 |
| 1s1 2p1 4p1 4D0.5 | 83220000.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 83226600.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 83242900.0 cm-1 |
| 1s1 2p1 4p1 4D1.5 | 83246400.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 83252400.0 cm-1 |
| 1s1 2p1 4p1 4S1.5 | 83260400.0 cm-1 |
| 1s1 2p1 4d1 4F1.5 | 83278600.0 cm-1 |
| 1s1 2p1 4p1 4D2.5 | 83280500.0 cm-1 |
| 1s1 2p1 4p1 4P0.5 | 83281000.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 83288600.0 cm-1 |
| 1s1 2p1 4d1 4F2.5 | 83296700.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 83297200.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 83299600.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 83301900.0 cm-1 |
| 1s1 2p1 4d1 4D2.5 | 83308500.0 cm-1 |
| 1s1 2p1 4f1 4G2.5 | 83312400.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 83317500.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 83320500.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 83323500.0 cm-1 |
| 1s1 2p1 4d1 4D1.5 | 83329600.0 cm-1 |
| 1s1 2p1 4d1 4F3.5 | 83331000.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 83333400.0 cm-1 |
| 1s1 2p1 4d1 4D0.5 | 83334200.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 83340700.0 cm-1 |
| 1s1 2p1 4f1 4G3.5 | 83345900.0 cm-1 |
| 1s1 2p1 4f1 4F1.5 | 83347600.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 83349600.0 cm-1 |
| 1s1 2p1 4f1 4G4.5 | 83351900.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 83353600.0 cm-1 |
| 1s1 2p1 4f1 4D3.5 | 83357500.0 cm-1 |
| 1s1 2p1 4s1 4P2.5 | 83379900.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 83405500.0 cm-1 |
| 1s1 2p1 4p1 4P1.5 | 83430100.0 cm-1 |
| 1s1 2p1 4p1 4P2.5 | 83433900.0 cm-1 |
| 1s1 2p1 4p1 4D3.5 | 83436100.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 83451400.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 83470000.0 cm-1 |
| 1s1 2p1 4d1 4F4.5 | 83479200.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 83483000.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 83483300.0 cm-1 |
| 1s1 2p1 4d1 4D3.5 | 83486000.0 cm-1 |
| 1s1 2p1 4d1 4P1.5 | 83492700.0 cm-1 |
| 1s1 2p1 4d1 4P0.5 | 83495600.0 cm-1 |
| 1s1 2p1 4d1 4P2.5 | 83497100.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 83504400.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 83508400.0 cm-1 |
| 1s1 2p1 4f1 4F4.5 | 83511400.0 cm-1 |
| 1s1 2p1 4f1 4F2.5 | 83511500.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 83512600.0 cm-1 |
| 1s1 2p1 4f1 4F3.5 | 83514800.0 cm-1 |
| 1s1 2p1 4f1 4D1.5 | 83517900.0 cm-1 |
| 1s1 2p1 4f1 4G5.5 | 83518000.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 83520300.0 cm-1 |
| 1s1 2p1 4f1 4D2.5 | 83521200.0 cm-1 |
| 1s1 2p1 4f1 4D0.5 | 83522700.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 83522700.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 83529100.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 83545700.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 83546100.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 83589000.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 83589700.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 83604600.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 83613000.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 83624200.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 83640700.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 83644500.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 83645400.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 83656900.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 83656900.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 83660600.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 83664200.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 83669400.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 83672800.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 83674300.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 83677700.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 83682600.0 cm-1 |
Contributors
- Guiyun Liang
- Nigel Badnell
U+26 29 27 20349369.( ) ------------------------------------------------------------------------ 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 = 1.28290 2S = 1.04799 2P = 0.95136 3S = 1.03437 3P = 0.94238 3D = 0.88449 4S = 1.03290 4P = 0.94206 4D = 0.88609 4F = 1.04301 5S = 1.03505 5P = 0.94406 5D = 0.88967 5F = 0.86587 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 2490.9287 Rydbergs (33891.575892 eV) A fine energy mesh of 0.000004 Z**2 Rydbergs (0.036790624 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (91.97656 eV) was used from the last threshold up to 2.743090 Z**2 Rydbergs (25230 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (91.97656 eV) was used from first threshold up to 2.743090 Z**2 Rydbergs (25230 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 = 1.28817 2S = 1.04967 2P = 0.95326 3S = 1.03645 3P = 0.94430 3D = 0.88669 4S = 1.03637 4P = 0.94530 4D = 0.89070 4F = 1.03000 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 (0.04598828 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (91.97656 eV) was used from the last threshold up to 2.743090 Z**2 Rydbergs (25230 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (91.97656 eV) was used from first threshold up to 2.743090 Z**2 Rydbergs (25230 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 4.05387 3 5.93610 4 106.74929 5 107.87324 6 108.43057 7 108.85495 8 109.03101 9 143.54042 10 144.01218 11 144.24710 12 144.42580 13 144.50016 14 144.53060 15 144.56340 16 160.43950 17 160.68026 18 160.80036 19 160.89176 20 160.92976 25 607.97004 26 609.01800 27 609.41895 29 615.26017 30 613.51965 31 614.02996 32 614.68608 33 615.08703 34 615.01413 35 615.66113 36 617.07360 37 617.03715 38 617.96664 39 619.16040 40 620.65488 86 722.27026 165 757.17179 Produced by: Guiyun Liang Date: 12/08/10 ------------------------------------------------------------------------