lilike_lgy10#si11.dat
Resolved Specific Ion Data Collections
- Ion
- Si11+
- Temperature Range
- 2.482 eV → 2.482 x 104 eV
ADF04
- Filename
- lilike_lgy10#si11.dat
- Full Path
- adf04/copaw#li/lilike_lgy10#si11.dat
Download data
- Spontaneous Emission: Si+11(i) → Si+11(j) + hv
- Electron Impact Excitation: Si+11(i) + e → Si+11(j) + e
| 2s1 2S0.5 | 0.0 cm-1 |
| 2p1 2P0.5 | 192910.0 cm-1 |
| 2p1 2P1.5 | 201001.0 cm-1 |
| 3s1 2S0.5 | 2389130.0 cm-1 |
| 3p1 2P0.5 | 2442160.0 cm-1 |
| 3p1 2P1.5 | 2444540.0 cm-1 |
| 3d1 2D1.5 | 2463940.0 cm-1 |
| 3d1 2D2.5 | 2464680.0 cm-1 |
| 4s1 2S0.5 | 3202110.0 cm-1 |
| 4p1 2P0.5 | 3223880.0 cm-1 |
| 4p1 2P1.5 | 3224870.0 cm-1 |
| 4d1 2D1.5 | 3232940.0 cm-1 |
| 4d1 2D2.5 | 3233260.0 cm-1 |
| 4f1 2F2.5 | 3233640.0 cm-1 |
| 4f1 2F3.5 | 3233800.0 cm-1 |
| 5s1 2S0.5 | 3573310.0 cm-1 |
| 5p1 2P0.5 | 3584300.0 cm-1 |
| 5p1 2P1.5 | 3584810.0 cm-1 |
| 5d1 2D1.5 | 3588910.0 cm-1 |
| 5d1 2D2.5 | 3589070.0 cm-1 |
| 5f1 2F2.5 | 3589290.0 cm-1 |
| 5f1 2F3.5 | 3589370.0 cm-1 |
| 5g1 2G3.5 | 3589370.0 cm-1 |
| 5g1 2G4.5 | 3589420.0 cm-1 |
| 1s1 2s2 2S0.5 | 14703700.0 cm-1 |
| 1s1 2s1 2p1 4P0.5 | 14753800.0 cm-1 |
| 1s1 2s1 2p1 4P1.5 | 14756600.0 cm-1 |
| 1s1 2s1 2p1 4P2.5 | 14761400.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 14902500.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 14906200.0 cm-1 |
| 1s1 2p2 4P0.5 | 14959100.0 cm-1 |
| 1s1 2p2 4P1.5 | 14962000.0 cm-1 |
| 1s1 2p2 4P2.5 | 14966600.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 14977900.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 14980000.0 cm-1 |
| 1s1 2p2 2D1.5 | 15059600.0 cm-1 |
| 1s1 2p2 2D2.5 | 15060300.0 cm-1 |
| 1s1 2p2 2P0.5 | 15083400.0 cm-1 |
| 1s1 2p2 2P1.5 | 15089600.0 cm-1 |
| 1s1 2p2 2S0.5 | 15200000.0 cm-1 |
| 1s1 2s1 3s1 4S1.5 | 17183500.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 17234100.0 cm-1 |
| 1s1 2s1 3p1 4P0.5 | 17252100.0 cm-1 |
| 1s1 2s1 3p1 4P1.5 | 17252600.0 cm-1 |
| 1s1 2s1 3p1 4P2.5 | 17254000.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 17256000.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 17256200.0 cm-1 |
| 1s1 2s1 3d1 4D0.5 | 17291400.0 cm-1 |
| 1s1 2s1 3d1 4D1.5 | 17291600.0 cm-1 |
| 1s1 2s1 3d1 4D2.5 | 17292100.0 cm-1 |
| 1s1 2s1 3d1 4D3.5 | 17292700.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 17313500.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 17318400.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 17318400.0 cm-1 |
| 1s1 2p1 3s1 4P0.5 | 17335100.0 cm-1 |
| 1s1 2p1 3s1 4P1.5 | 17337600.0 cm-1 |
| 1s1 2p1 3s1 4P2.5 | 17342200.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 17358500.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 17360300.0 cm-1 |
| 1s1 2p1 3p1 4D0.5 | 17368000.0 cm-1 |
| 1s1 2p1 3p1 4D1.5 | 17369900.0 cm-1 |
| 1s1 2p1 3p1 4D2.5 | 17373100.0 cm-1 |
| 1s1 2p1 3p1 4D3.5 | 17377100.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 17378200.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 17378400.0 cm-1 |
| 1s1 2p1 3p1 4S1.5 | 17394000.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 17394400.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 17400700.0 cm-1 |
| 1s1 2p1 3d1 4F1.5 | 17406400.0 cm-1 |
| 1s1 2p1 3p1 4P0.5 | 17406800.0 cm-1 |
| 1s1 2p1 3d1 4F2.5 | 17408200.0 cm-1 |
| 1s1 2p1 3p1 4P1.5 | 17408800.0 cm-1 |
| 1s1 2p1 3d1 4F3.5 | 17410700.0 cm-1 |
| 1s1 2p1 3p1 4P2.5 | 17411000.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 17412800.0 cm-1 |
| 1s1 2p1 3d1 4F4.5 | 17413900.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 17413900.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 17417400.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 17418000.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 17426100.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 17431900.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 17438100.0 cm-1 |
| 1s1 2p1 3d1 4D0.5 | 17438700.0 cm-1 |
| 1s1 2p1 3d1 4D1.5 | 17439500.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 17439700.0 cm-1 |
| 1s1 2p1 3d1 4D2.5 | 17440300.0 cm-1 |
| 1s1 2p1 3d1 4D3.5 | 17442200.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 17447500.0 cm-1 |
| 1s1 2p1 3d1 4P2.5 | 17451200.0 cm-1 |
| 1s1 2p1 3d1 4P1.5 | 17452600.0 cm-1 |
| 1s1 2p1 3d1 4P0.5 | 17453400.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 17453600.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 17458100.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 17479300.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 17482800.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 17486100.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 17486400.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 17486600.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 17489000.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 17514300.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 17515100.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 17522300.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 17527600.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 17529200.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 17547500.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 17549100.0 cm-1 |
| 1s1 2s1 4s1 4S1.5 | 18048000.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 18064300.0 cm-1 |
| 1s1 2s1 4p1 4P0.5 | 18072300.0 cm-1 |
| 1s1 2s1 4p1 4P1.5 | 18072600.0 cm-1 |
| 1s1 2s1 4p1 4P2.5 | 18073000.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 18079400.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 18079600.0 cm-1 |
| 1s1 2s1 4d1 4D0.5 | 18088800.0 cm-1 |
| 1s1 2s1 4d1 4D1.5 | 18088800.0 cm-1 |
| 1s1 2s1 4d1 4D2.5 | 18088900.0 cm-1 |
| 1s1 2s1 4d1 4D3.5 | 18089100.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 18097300.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 18097300.0 cm-1 |
| 1s1 2s1 4f1 4F1.5 | 18101600.0 cm-1 |
| 1s1 2s1 4f1 4F2.5 | 18101600.0 cm-1 |
| 1s1 2s1 4f1 4F3.5 | 18101700.0 cm-1 |
| 1s1 2s1 4f1 4F4.5 | 18101700.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 18104500.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 18104600.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 18165700.0 cm-1 |
| 1s1 2p1 4s1 4P0.5 | 18175600.0 cm-1 |
| 1s1 2p1 4s1 4P1.5 | 18177900.0 cm-1 |
| 1s1 2p1 4s1 4P2.5 | 18182800.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 18183400.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 18184900.0 cm-1 |
| 1s1 2p1 4p1 4D0.5 | 18191300.0 cm-1 |
| 1s1 2p1 4p1 4D1.5 | 18192900.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 18195000.0 cm-1 |
| 1s1 2p1 4p1 4D2.5 | 18195300.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 18198700.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 18198800.0 cm-1 |
| 1s1 2p1 4p1 4D3.5 | 18199300.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 18199800.0 cm-1 |
| 1s1 2p1 4p1 4P0.5 | 18202400.0 cm-1 |
| 1s1 2p1 4p1 4S1.5 | 18203000.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 18204200.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 18204400.0 cm-1 |
| 1s1 2p1 4p1 4P1.5 | 18206400.0 cm-1 |
| 1s1 2p1 4p1 4P2.5 | 18206600.0 cm-1 |
| 1s1 2p1 4d1 4F1.5 | 18206900.0 cm-1 |
| 1s1 2p1 4d1 4F2.5 | 18208500.0 cm-1 |
| 1s1 2p1 4d1 4F3.5 | 18210800.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 18211900.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 18212100.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 18212600.0 cm-1 |
| 1s1 2p1 4d1 4F4.5 | 18214300.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 18214600.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 18214900.0 cm-1 |
| 1s1 2p1 4d1 4D0.5 | 18216800.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 18216900.0 cm-1 |
| 1s1 2p1 4d1 4D1.5 | 18217100.0 cm-1 |
| 1s1 2p1 4d1 4D2.5 | 18217900.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 18219300.0 cm-1 |
| 1s1 2p1 4f1 4F3.5 | 18219600.0 cm-1 |
| 1s1 2p1 4f1 4F2.5 | 18220200.0 cm-1 |
| 1s1 2p1 4d1 4D3.5 | 18220300.0 cm-1 |
| 1s1 2p1 4f1 4F1.5 | 18220400.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 18220700.0 cm-1 |
| 1s1 2p1 4f1 4F4.5 | 18221300.0 cm-1 |
| 1s1 2p1 4d1 4P2.5 | 18223300.0 cm-1 |
| 1s1 2p1 4f1 4G2.5 | 18224100.0 cm-1 |
| 1s1 2p1 4d1 4P1.5 | 18224400.0 cm-1 |
| 1s1 2p1 4f1 4G3.5 | 18225100.0 cm-1 |
| 1s1 2p1 4d1 4P0.5 | 18225100.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 18227200.0 cm-1 |
| 1s1 2p1 4f1 4G4.5 | 18227500.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 18228300.0 cm-1 |
| 1s1 2p1 4f1 4G5.5 | 18229100.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 18229800.0 cm-1 |
| 1s1 2p1 4f1 4D3.5 | 18230200.0 cm-1 |
| 1s1 2p1 4f1 4D2.5 | 18231100.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 18231500.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 18231600.0 cm-1 |
| 1s1 2p1 4f1 4D1.5 | 18232600.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 18232900.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 18233300.0 cm-1 |
| 1s1 2p1 4f1 4D0.5 | 18233300.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 18235300.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 18235800.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 18264700.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 18264800.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 18282600.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 18282800.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 18282900.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 18283800.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 18293700.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 18296000.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 18296300.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 18298100.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 18298800.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 18300900.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 18301100.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 18306400.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 18306500.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 18306500.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 18307000.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 18310600.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 18310800.0 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 = 1.28020 2S = 1.03447 2P = 0.93064 3S = 1.02229 3P = 0.92303 3D = 0.85820 4S = 1.02083 4P = 0.92294 4D = 0.86031 4F = 0.99336 5S = 1.02230 5P = 0.92504 5D = 0.86440 5F = 0.84214 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. 63 continuum basis orbitals were used, giving a smallest maximum basis-orbital energy of 548.5781 Rydbergs (7463.953629 eV) A fine energy mesh of 0.000004 Z**2 Rydbergs (0.006585304 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (16.46326 eV) was used from the last threshold up to 3.354135 Z**2 Rydbergs (5522 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (16.46326 eV) was used from first threshold up to 3.354135 Z**2 Rydbergs (5522 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: 14/10/10 ------------------------------------------------------------------------ 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 = 1.28463 2S = 1.03666 2P = 0.93361 3S = 1.02470 3P = 0.92509 3D = 0.86246 4S = 1.02459 4P = 0.92640 4D = 0.86792 4F = 0.99341 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. 45 continuum basis orbitals were used, giving a smallest maximum basis-orbital energy of 0 Rydbergs (0.000000 eV) A fine energy mesh of 0.000010 Z**2 Rydbergs (0.01646326 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (16.46326 eV) was used from the last threshold up to 3.179324 Z**2 Rydbergs (5234.203 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (16.46326 eV) was used from first threshold up to 3.179324 Z**2 Rydbergs (5234.203 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 1.75020 3 1.82470 4 21.76899 5 22.25259 6 22.27437 7 22.45171 8 22.45799 9 29.17968 10 29.37424 11 29.38426 12 29.45853 13 29.46126 14 29.46737 15 29.46883 16 32.56367 17 32.66118 18 32.66573 19 32.70446 20 32.70583 21 32.70948 22 32.70948 25 133.79952 26 134.25060 27 134.26973 28 134.31985 29 135.60474 30 135.64483 31 136.11414 32 136.14694 33 136.18430 34 136.23442 35 136.25356 36 136.98804 37 136.99807 38 137.21130 39 137.28238 40 138.21734 Produced by: Guiyun Liang Date: 25/11/10 ------------------------------------------------------------------------