lilike_lgy10#sc18.dat
Resolved Specific Ion Data Collections
- Ion
- Sc18+
- Temperature Range
- 6.221 eV → 6.221 x 104 eV
ADF04
- Filename
- lilike_lgy10#sc18.dat
- Full Path
- adf04/copaw#li/lilike_lgy10#sc18.dat
Download data
- Spontaneous Emission: Sc+18(i) → Sc+18(j) + hv
- Electron Impact Excitation: Sc+18(i) + e → Sc+18(j) + e
| 2s1 2S0.5 | 0.0 cm-1 |
| 2p1 2P0.5 | 307306.0 cm-1 |
| 2p1 2P1.5 | 357395.0 cm-1 |
| 3s1 2S0.5 | 5847710.0 cm-1 |
| 3p1 2P0.5 | 5932750.0 cm-1 |
| 3p1 2P1.5 | 5947380.0 cm-1 |
| 3d1 2D1.5 | 5980540.0 cm-1 |
| 3d1 2D2.5 | 5985250.0 cm-1 |
| 4s1 2S0.5 | 7855390.0 cm-1 |
| 4p1 2P0.5 | 7890390.0 cm-1 |
| 4p1 2P1.5 | 7896470.0 cm-1 |
| 4d1 2D1.5 | 7910220.0 cm-1 |
| 4d1 2D2.5 | 7912200.0 cm-1 |
| 4f1 2F2.5 | 7912920.0 cm-1 |
| 4f1 2F3.5 | 7913910.0 cm-1 |
| 5s1 2S0.5 | 8775740.0 cm-1 |
| 5p1 2P0.5 | 8793440.0 cm-1 |
| 5p1 2P1.5 | 8796490.0 cm-1 |
| 5d1 2D1.5 | 8803480.0 cm-1 |
| 5d1 2D2.5 | 8804480.0 cm-1 |
| 5f1 2F2.5 | 8804890.0 cm-1 |
| 5f1 2F3.5 | 8805390.0 cm-1 |
| 5g1 2G3.5 | 8805400.0 cm-1 |
| 5g1 2G4.5 | 8805700.0 cm-1 |
| 1s1 2s2 2S0.5 | 34271400.0 cm-1 |
| 1s1 2s1 2p1 4P0.5 | 34346900.0 cm-1 |
| 1s1 2s1 2p1 4P1.5 | 34362700.0 cm-1 |
| 1s1 2s1 2p1 4P2.5 | 34393600.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 34594900.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 34620100.0 cm-1 |
| 1s1 2p2 4P0.5 | 34689900.0 cm-1 |
| 1s1 2p2 4P1.5 | 34709700.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 34716300.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 34727000.0 cm-1 |
| 1s1 2p2 4P2.5 | 34735400.0 cm-1 |
| 1s1 2p2 2D1.5 | 34870200.0 cm-1 |
| 1s1 2p2 2D2.5 | 34881800.0 cm-1 |
| 1s1 2p2 2P0.5 | 34899300.0 cm-1 |
| 1s1 2p2 2P1.5 | 34944700.0 cm-1 |
| 1s1 2p2 2S0.5 | 35093400.0 cm-1 |
| 1s1 2s1 3s1 4S1.5 | 40249600.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 40330600.0 cm-1 |
| 1s1 2s1 3p1 4P0.5 | 40357200.0 cm-1 |
| 1s1 2s1 3p1 4P1.5 | 40359500.0 cm-1 |
| 1s1 2s1 3p1 4P2.5 | 40369700.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 40375500.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 40376000.0 cm-1 |
| 1s1 2s1 3d1 4D0.5 | 40430000.0 cm-1 |
| 1s1 2s1 3d1 4D1.5 | 40431700.0 cm-1 |
| 1s1 2s1 3d1 4D2.5 | 40434400.0 cm-1 |
| 1s1 2s1 3d1 4D3.5 | 40437900.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 40458900.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 40476200.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 40476300.0 cm-1 |
| 1s1 2p1 3s1 4P0.5 | 40484900.0 cm-1 |
| 1s1 2p1 3s1 4P1.5 | 40498400.0 cm-1 |
| 1s1 2p1 3s1 4P2.5 | 40529300.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 40532200.0 cm-1 |
| 1s1 2p1 3p1 4D0.5 | 40538000.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 40545000.0 cm-1 |
| 1s1 2p1 3p1 4D1.5 | 40548200.0 cm-1 |
| 1s1 2p1 3p1 4D2.5 | 40568800.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 40576800.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 40580500.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 40583700.0 cm-1 |
| 1s1 2p1 3p1 4D3.5 | 40596600.0 cm-1 |
| 1s1 2p1 3p1 4P0.5 | 40610000.0 cm-1 |
| 1s1 2p1 3p1 4S1.5 | 40610300.0 cm-1 |
| 1s1 2p1 3d1 4F1.5 | 40611100.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 40618600.0 cm-1 |
| 1s1 2p1 3d1 4F2.5 | 40620900.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 40628500.0 cm-1 |
| 1s1 2p1 3p1 4P1.5 | 40630200.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 40631700.0 cm-1 |
| 1s1 2p1 3d1 4F3.5 | 40636600.0 cm-1 |
| 1s1 2p1 3p1 4P2.5 | 40641300.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 40646200.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 40646200.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 40647500.0 cm-1 |
| 1s1 2p1 3d1 4F4.5 | 40660300.0 cm-1 |
| 1s1 2p1 3d1 4D0.5 | 40672500.0 cm-1 |
| 1s1 2p1 3d1 4D1.5 | 40673600.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 40676600.0 cm-1 |
| 1s1 2p1 3d1 4D2.5 | 40678100.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 40680700.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 40681200.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 40692400.0 cm-1 |
| 1s1 2p1 3d1 4D3.5 | 40698000.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 40710700.0 cm-1 |
| 1s1 2p1 3d1 4P2.5 | 40711400.0 cm-1 |
| 1s1 2p1 3d1 4P1.5 | 40714200.0 cm-1 |
| 1s1 2p1 3d1 4P0.5 | 40716700.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 40723800.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 40745400.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 40754900.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 40756100.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 40759500.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 40765900.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 40772500.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 40813100.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 40816500.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 40816600.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 40832700.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 40842000.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 40859100.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 40868600.0 cm-1 |
| 1s1 2s1 4s1 4S1.5 | 42335700.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 42362300.0 cm-1 |
| 1s1 2s1 4p1 4P0.5 | 42374900.0 cm-1 |
| 1s1 2s1 4p1 4P1.5 | 42376300.0 cm-1 |
| 1s1 2s1 4p1 4P2.5 | 42379700.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 42389500.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 42390700.0 cm-1 |
| 1s1 2s1 4d1 4D0.5 | 42405700.0 cm-1 |
| 1s1 2s1 4d1 4D1.5 | 42406100.0 cm-1 |
| 1s1 2s1 4d1 4D2.5 | 42406800.0 cm-1 |
| 1s1 2s1 4d1 4D3.5 | 42407800.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 42420000.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 42420400.0 cm-1 |
| 1s1 2s1 4f1 4F1.5 | 42427600.0 cm-1 |
| 1s1 2s1 4f1 4F2.5 | 42427900.0 cm-1 |
| 1s1 2s1 4f1 4F3.5 | 42428200.0 cm-1 |
| 1s1 2s1 4f1 4F4.5 | 42428700.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 42432400.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 42432700.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 42525800.0 cm-1 |
| 1s1 2p1 4s1 4P0.5 | 42533900.0 cm-1 |
| 1s1 2p1 4s1 4P1.5 | 42545100.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 42555500.0 cm-1 |
| 1s1 2p1 4p1 4D0.5 | 42558800.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 42564100.0 cm-1 |
| 1s1 2p1 4p1 4D1.5 | 42567100.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 42569200.0 cm-1 |
| 1s1 2p1 4p1 4S1.5 | 42577000.0 cm-1 |
| 1s1 2p1 4p1 4D2.5 | 42579700.0 cm-1 |
| 1s1 2p1 4s1 4P2.5 | 42579800.0 cm-1 |
| 1s1 2p1 4p1 4P0.5 | 42584600.0 cm-1 |
| 1s1 2p1 4d1 4F1.5 | 42588900.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 42589900.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 42592200.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 42594300.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 42596400.0 cm-1 |
| 1s1 2p1 4d1 4F2.5 | 42596500.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 42603100.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 42603400.0 cm-1 |
| 1s1 2p1 4d1 4F3.5 | 42607700.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 42609300.0 cm-1 |
| 1s1 2p1 4f1 4G2.5 | 42610000.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 42610500.0 cm-1 |
| 1s1 2p1 4p1 4D3.5 | 42610700.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 42611800.0 cm-1 |
| 1s1 2p1 4f1 4F3.5 | 42611800.0 cm-1 |
| 1s1 2p1 4d1 4D0.5 | 42614400.0 cm-1 |
| 1s1 2p1 4d1 4D1.5 | 42615100.0 cm-1 |
| 1s1 2p1 4p1 4P1.5 | 42617000.0 cm-1 |
| 1s1 2p1 4p1 4P2.5 | 42618100.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 42620800.0 cm-1 |
| 1s1 2p1 4f1 4F1.5 | 42621100.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 42621400.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 42621500.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 42623000.0 cm-1 |
| 1s1 2p1 4f1 4F4.5 | 42623100.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 42627000.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 42628800.0 cm-1 |
| 1s1 2p1 4d1 4F4.5 | 42636900.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 42637600.0 cm-1 |
| 1s1 2p1 4d1 4D3.5 | 42644300.0 cm-1 |
| 1s1 2p1 4d1 4D2.5 | 42644700.0 cm-1 |
| 1s1 2p1 4d1 4P2.5 | 42650500.0 cm-1 |
| 1s1 2p1 4d1 4P1.5 | 42650800.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 42650900.0 cm-1 |
| 1s1 2p1 4d1 4P0.5 | 42652300.0 cm-1 |
| 1s1 2p1 4f1 4G3.5 | 42657400.0 cm-1 |
| 1s1 2p1 4f1 4G4.5 | 42658000.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 42658500.0 cm-1 |
| 1s1 2p1 4f1 4F2.5 | 42660200.0 cm-1 |
| 1s1 2p1 4f1 4D3.5 | 42660400.0 cm-1 |
| 1s1 2p1 4f1 4G5.5 | 42661900.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 42662500.0 cm-1 |
| 1s1 2p1 4f1 4D1.5 | 42664600.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 42664900.0 cm-1 |
| 1s1 2p1 4f1 4D2.5 | 42665300.0 cm-1 |
| 1s1 2p1 4f1 4D0.5 | 42667300.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 42669400.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 42670300.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 42707200.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 42707600.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 42736700.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 42737000.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 42739700.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 42742800.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 42755600.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 42762600.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 42764100.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 42765400.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 42769200.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 42772300.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 42773200.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 42777100.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 42780800.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 42781300.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 42781500.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 42786400.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 42787700.0 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 = 1.28193 2S = 1.04314 2P = 0.94401 3S = 1.03128 3P = 0.93667 3D = 0.87263 4S = 1.02921 4P = 0.93620 4D = 0.87438 4F = 0.98597 5S = 1.03061 5P = 0.93744 5D = 0.87959 5F = 0.87433 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 1243.9074 Rydbergs (16924.604084 eV) A fine energy mesh of 0.000004 Z**2 Rydbergs (0.017633376 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (44.08344 eV) was used from the last threshold up to 2.955758 Z**2 Rydbergs (13030 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (44.08344 eV) was used from first threshold up to 2.955758 Z**2 Rydbergs (13030 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: 13/10/10 ------------------------------------------------------------------------ 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 = 1.28688 2S = 1.04502 2P = 0.94633 3S = 1.03243 3P = 0.93759 3D = 0.88082 4S = 1.03235 4P = 0.93872 4D = 0.88503 4F = 0.98601 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 0.000006 Z**2 Rydbergs (0.026450064 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (44.08344 eV) was used from the last threshold up to 2.955758 Z**2 Rydbergs (13030 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (44.08344 eV) was used from first threshold up to 2.955758 Z**2 Rydbergs (13030 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 2.795 3 3.257 4 53.36 5 54.05 6 54.18 7 54.48 8 54.51 10 71.90 12 72.07 13 72.1 17 80.1 19 80.2 33 315.88 36 317.5 38 317.7 40 319.37 Produced by: Guiyun Liang Date: 26/11/10 ------------------------------------------------------------------------