lilike_lgy10#f6.dat
Resolved Specific Ion Data Collections
- Ion
- F6+
- Temperature Range
- 0.844 eV → 8444 eV
ADF04
- Filename
- lilike_lgy10#f6.dat
- Full Path
- adf04/copaw#li/lilike_lgy10#f6.dat
Download data
- Spontaneous Emission: F+6(i) → F+6(j) + hv
- Electron Impact Excitation: F+6(i) + e → F+6(j) + e
| 2s1 2S0.5 | 0.0 cm-1 |
| 2p1 2P0.5 | 113084.0 cm-1 |
| 2p1 2P1.5 | 114041.0 cm-1 |
| 3s1 2S0.5 | 853982.0 cm-1 |
| 3p1 2P0.5 | 884678.0 cm-1 |
| 3p1 2P1.5 | 884960.0 cm-1 |
| 3d1 2D1.5 | 894894.0 cm-1 |
| 3d1 2D2.5 | 894980.0 cm-1 |
| 4s1 2S0.5 | 1139670.0 cm-1 |
| 4p1 2P0.5 | 1152200.0 cm-1 |
| 4p1 2P1.5 | 1152320.0 cm-1 |
| 4d1 2D1.5 | 1156470.0 cm-1 |
| 4d1 2D2.5 | 1156510.0 cm-1 |
| 4f1 2F2.5 | 1156670.0 cm-1 |
| 4f1 2F3.5 | 1156690.0 cm-1 |
| 5s1 2S0.5 | 1269080.0 cm-1 |
| 5p1 2P0.5 | 1275380.0 cm-1 |
| 5p1 2P1.5 | 1275440.0 cm-1 |
| 5d1 2D1.5 | 1277560.0 cm-1 |
| 5d1 2D2.5 | 1277580.0 cm-1 |
| 5f1 2F2.5 | 1277670.0 cm-1 |
| 5f1 2F3.5 | 1277680.0 cm-1 |
| 5g1 2G3.5 | 1277680.0 cm-1 |
| 5g1 2G4.5 | 1277690.0 cm-1 |
| 1s1 2s2 2S0.5 | 5747140.0 cm-1 |
| 1s1 2s1 2p1 4P0.5 | 5780130.0 cm-1 |
| 1s1 2s1 2p1 4P1.5 | 5780470.0 cm-1 |
| 1s1 2s1 2p1 4P2.5 | 5781050.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 5862930.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 5863370.0 cm-1 |
| 1s1 2p2 4P0.5 | 5902990.0 cm-1 |
| 1s1 2p2 4P1.5 | 5903330.0 cm-1 |
| 1s1 2p2 4P2.5 | 5903900.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 5913780.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 5914030.0 cm-1 |
| 1s1 2p2 2D1.5 | 5957550.0 cm-1 |
| 1s1 2p2 2D2.5 | 5957580.0 cm-1 |
| 1s1 2p2 2P0.5 | 5969950.0 cm-1 |
| 1s1 2p2 2P1.5 | 5970660.0 cm-1 |
| 1s1 2p2 2S0.5 | 6044650.0 cm-1 |
| 1s1 2s1 3s1 4S1.5 | 6661770.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 6692120.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 6703450.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 6703510.0 cm-1 |
| 1s1 2s1 3p1 4P0.5 | 6703860.0 cm-1 |
| 1s1 2s1 3p1 4P1.5 | 6703950.0 cm-1 |
| 1s1 2s1 3p1 4P2.5 | 6704050.0 cm-1 |
| 1s1 2s1 3d1 4D0.5 | 6724490.0 cm-1 |
| 1s1 2s1 3d1 4D1.5 | 6724520.0 cm-1 |
| 1s1 2s1 3d1 4D2.5 | 6724570.0 cm-1 |
| 1s1 2s1 3d1 4D3.5 | 6724640.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 6736960.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 6739910.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 6739910.0 cm-1 |
| 1s1 2p1 3s1 4P0.5 | 6757960.0 cm-1 |
| 1s1 2p1 3s1 4P1.5 | 6758270.0 cm-1 |
| 1s1 2p1 3s1 4P2.5 | 6758790.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 6764200.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 6764380.0 cm-1 |
| 1s1 2p1 3p1 4D0.5 | 6775280.0 cm-1 |
| 1s1 2p1 3p1 4D1.5 | 6775500.0 cm-1 |
| 1s1 2p1 3p1 4D2.5 | 6775860.0 cm-1 |
| 1s1 2p1 3p1 4D3.5 | 6776320.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 6777600.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 6777670.0 cm-1 |
| 1s1 2p1 3p1 4S1.5 | 6787870.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 6790190.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 6790970.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 6793390.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 6793520.0 cm-1 |
| 1s1 2p1 3d1 4F1.5 | 6796600.0 cm-1 |
| 1s1 2p1 3d1 4F2.5 | 6796810.0 cm-1 |
| 1s1 2p1 3d1 4F3.5 | 6797090.0 cm-1 |
| 1s1 2p1 3d1 4F4.5 | 6797450.0 cm-1 |
| 1s1 2p1 3p1 4P0.5 | 6800100.0 cm-1 |
| 1s1 2p1 3p1 4P1.5 | 6800300.0 cm-1 |
| 1s1 2p1 3p1 4P2.5 | 6800610.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 6801230.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 6801330.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 6807460.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 6808160.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 6812100.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 6812250.0 cm-1 |
| 1s1 2p1 3d1 4D0.5 | 6814720.0 cm-1 |
| 1s1 2p1 3d1 4D1.5 | 6814780.0 cm-1 |
| 1s1 2p1 3d1 4D2.5 | 6814890.0 cm-1 |
| 1s1 2p1 3d1 4D3.5 | 6815060.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 6818510.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 6819250.0 cm-1 |
| 1s1 2p1 3d1 4P2.5 | 6821270.0 cm-1 |
| 1s1 2p1 3d1 4P1.5 | 6821470.0 cm-1 |
| 1s1 2p1 3d1 4P0.5 | 6821580.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 6823540.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 6837750.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 6838170.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 6840040.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 6840070.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 6840110.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 6840440.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 6853560.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 6853680.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 6861230.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 6861340.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 6861420.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 6874550.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 6874740.0 cm-1 |
| 1s1 2s1 4s1 4S1.5 | 6979630.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 6989070.0 cm-1 |
| 1s1 2s1 4p1 4P0.5 | 6993810.0 cm-1 |
| 1s1 2s1 4p1 4P1.5 | 6993830.0 cm-1 |
| 1s1 2s1 4p1 4P2.5 | 6993880.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 6997490.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 6997510.0 cm-1 |
| 1s1 2s1 4d1 4D0.5 | 7002150.0 cm-1 |
| 1s1 2s1 4d1 4D1.5 | 7002150.0 cm-1 |
| 1s1 2s1 4d1 4D2.5 | 7002170.0 cm-1 |
| 1s1 2s1 4d1 4D3.5 | 7002180.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 7007050.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 7007060.0 cm-1 |
| 1s1 2s1 4f1 4F1.5 | 7009320.0 cm-1 |
| 1s1 2s1 4f1 4F2.5 | 7009330.0 cm-1 |
| 1s1 2s1 4f1 4F3.5 | 7009330.0 cm-1 |
| 1s1 2s1 4f1 4F4.5 | 7009340.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 7011440.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 7011440.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 7046640.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 7057840.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 7057930.0 cm-1 |
| 1s1 2p1 4s1 4P0.5 | 7060160.0 cm-1 |
| 1s1 2p1 4s1 4P1.5 | 7060470.0 cm-1 |
| 1s1 2p1 4s1 4P2.5 | 7060990.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 7067900.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 7067930.0 cm-1 |
| 1s1 2p1 4p1 4D0.5 | 7069270.0 cm-1 |
| 1s1 2p1 4p1 4D1.5 | 7069450.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 7069470.0 cm-1 |
| 1s1 2p1 4p1 4D2.5 | 7069750.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 7070090.0 cm-1 |
| 1s1 2p1 4p1 4D3.5 | 7070170.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 7071410.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 7071620.0 cm-1 |
| 1s1 2p1 4p1 4S1.5 | 7073720.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 7073900.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 7073950.0 cm-1 |
| 1s1 2p1 4p1 4P0.5 | 7074660.0 cm-1 |
| 1s1 2p1 4p1 4P1.5 | 7074920.0 cm-1 |
| 1s1 2p1 4p1 4P2.5 | 7075120.0 cm-1 |
| 1s1 2p1 4d1 4F1.5 | 7077380.0 cm-1 |
| 1s1 2p1 4d1 4F2.5 | 7077570.0 cm-1 |
| 1s1 2p1 4d1 4F3.5 | 7077850.0 cm-1 |
| 1s1 2p1 4d1 4F4.5 | 7078200.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 7078300.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 7078430.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 7079690.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 7080240.0 cm-1 |
| 1s1 2p1 4d1 4D0.5 | 7081640.0 cm-1 |
| 1s1 2p1 4d1 4D1.5 | 7081690.0 cm-1 |
| 1s1 2p1 4d1 4D2.5 | 7081780.0 cm-1 |
| 1s1 2p1 4d1 4D3.5 | 7081960.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 7083010.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 7083120.0 cm-1 |
| 1s1 2p1 4f1 4F1.5 | 7083320.0 cm-1 |
| 1s1 2p1 4f1 4F2.5 | 7083340.0 cm-1 |
| 1s1 2p1 4f1 4F3.5 | 7083400.0 cm-1 |
| 1s1 2p1 4f1 4F4.5 | 7083500.0 cm-1 |
| 1s1 2p1 4d1 4P2.5 | 7084110.0 cm-1 |
| 1s1 2p1 4d1 4P1.5 | 7084320.0 cm-1 |
| 1s1 2p1 4d1 4P0.5 | 7084450.0 cm-1 |
| 1s1 2p1 4f1 4G2.5 | 7085600.0 cm-1 |
| 1s1 2p1 4f1 4G3.5 | 7085780.0 cm-1 |
| 1s1 2p1 4f1 4G4.5 | 7086020.0 cm-1 |
| 1s1 2p1 4f1 4G5.5 | 7086300.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 7087350.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 7087600.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 7087830.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 7088180.0 cm-1 |
| 1s1 2p1 4f1 4D3.5 | 7088580.0 cm-1 |
| 1s1 2p1 4f1 4D2.5 | 7088800.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 7088810.0 cm-1 |
| 1s1 2p1 4f1 4D1.5 | 7088970.0 cm-1 |
| 1s1 2p1 4f1 4D0.5 | 7089070.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 7090200.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 7090530.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 7090640.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 7091010.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 7105340.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 7105340.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 7115770.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 7115770.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 7115940.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 7116050.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 7122200.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 7122560.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 7122600.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 7124060.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 7124160.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 7125100.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 7125120.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 7128320.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 7128330.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 7128990.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 7129070.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 7131100.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 7131130.0 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 = 1.27708 2S = 1.01900 2P = 0.90652 3S = 1.00748 3P = 0.90137 3D = 0.82978 4S = 1.00632 4P = 0.90117 4D = 0.83202 4F = 0.92080 5S = 1.00767 5P = 0.90270 5D = 0.83556 5F = 0.81770 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 189.0733 Rydbergs (2572.531320 eV) A fine energy mesh of 0.000004 Z**2 Rydbergs (0.001959264 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (4.89816 eV) was used from the last threshold up to 3.780767 Z**2 Rydbergs (1851.88 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (4.89816 eV) was used from first threshold up to 3.780767 Z**2 Rydbergs (1851.88 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 = 1.28049 2S = 1.02155 2P = 0.91054 3S = 1.01036 3P = 0.90308 3D = 0.83523 4S = 1.01000 4P = 0.90410 4D = 0.84055 4F = 0.99000 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 0.000020 Z**2 Rydbergs (0.00979632 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (4.89816 eV) was used from the last threshold up to 3.780767 Z**2 Rydbergs (1851.88 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (4.89816 eV) was used from first threshold up to 3.780767 Z**2 Rydbergs (1851.88 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 1.02299 3 1.03188 4 7.78788 5 8.06588 6 8.06849 7 8.16148 8 8.16227 9 10.39238 10 10.50593 11 10.50700 12 10.54563 13 10.54596 14 10.54813 16 11.57201 17 11.62915 18 11.62974 19 11.64936 20 11.64953 21 11.65070 22 11.65070 23 11.65089 24 11.65089 29 53.31550 34 53.71099 36 54.11377 38 54.27233 40 54.48739 67 61.84678 136 64.53411 Produced by: Guiyun Liang Date: 13/08/10 ------------------------------------------------------------------------