lilike_lgy10#mg9.dat
Resolved Specific Ion Data Collections
- Ion
- Mg9+
- Temperature Range
- 1.723 eV → 1.723 x 104 eV
ADF04
- Filename
- lilike_lgy10#mg9.dat
- Full Path
- adf04/copaw#li/lilike_lgy10#mg9.dat
Download data
- Spontaneous Emission: Mg+9(i) → Mg+9(j) + hv
- Electron Impact Excitation: Mg+9(i) + e → Mg+9(j) + e
| 2s1 2S0.5 | 0.0 cm-1 |
| 2p1 2P0.5 | 160879.0 cm-1 |
| 2p1 2P1.5 | 164809.0 cm-1 |
| 3s1 2S0.5 | 1682380.0 cm-1 |
| 3p1 2P0.5 | 1726440.0 cm-1 |
| 3p1 2P1.5 | 1727590.0 cm-1 |
| 3d1 2D1.5 | 1743170.0 cm-1 |
| 3d1 2D2.5 | 1743530.0 cm-1 |
| 4s1 2S0.5 | 2252080.0 cm-1 |
| 4p1 2P0.5 | 2270140.0 cm-1 |
| 4p1 2P1.5 | 2270620.0 cm-1 |
| 4d1 2D1.5 | 2277100.0 cm-1 |
| 4d1 2D2.5 | 2277260.0 cm-1 |
| 4f1 2F2.5 | 2277550.0 cm-1 |
| 4f1 2F3.5 | 2277620.0 cm-1 |
| 5s1 2S0.5 | 2511610.0 cm-1 |
| 5p1 2P0.5 | 2520720.0 cm-1 |
| 5p1 2P1.5 | 2520960.0 cm-1 |
| 5d1 2D1.5 | 2524260.0 cm-1 |
| 5d1 2D2.5 | 2524340.0 cm-1 |
| 5f1 2F2.5 | 2524500.0 cm-1 |
| 5f1 2F3.5 | 2524540.0 cm-1 |
| 5g1 2G3.5 | 2524550.0 cm-1 |
| 5g1 2G4.5 | 2524570.0 cm-1 |
| 1s1 2s2 2S0.5 | 10622200.0 cm-1 |
| 1s1 2s1 2p1 4P0.5 | 10665300.0 cm-1 |
| 1s1 2s1 2p1 4P1.5 | 10666600.0 cm-1 |
| 1s1 2s1 2p1 4P2.5 | 10669000.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 10787300.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 10789000.0 cm-1 |
| 1s1 2p2 4P0.5 | 10836600.0 cm-1 |
| 1s1 2p2 4P1.5 | 10838000.0 cm-1 |
| 1s1 2p2 4P2.5 | 10840300.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 10852600.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 10853600.0 cm-1 |
| 1s1 2p2 2D1.5 | 10918100.0 cm-1 |
| 1s1 2p2 2D2.5 | 10918300.0 cm-1 |
| 1s1 2p2 2P0.5 | 10937700.0 cm-1 |
| 1s1 2p2 2P1.5 | 10940700.0 cm-1 |
| 1s1 2p2 2S0.5 | 11037100.0 cm-1 |
| 1s1 2s1 3s1 4S1.5 | 12383300.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 12425700.0 cm-1 |
| 1s1 2s1 3p1 4P0.5 | 12441200.0 cm-1 |
| 1s1 2s1 3p1 4P1.5 | 12441400.0 cm-1 |
| 1s1 2s1 3p1 4P2.5 | 12442100.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 12443000.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 12443100.0 cm-1 |
| 1s1 2s1 3d1 4D0.5 | 12472700.0 cm-1 |
| 1s1 2s1 3d1 4D1.5 | 12472800.0 cm-1 |
| 1s1 2s1 3d1 4D2.5 | 12473000.0 cm-1 |
| 1s1 2s1 3d1 4D3.5 | 12473300.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 12491300.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 12495000.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 12495000.0 cm-1 |
| 1s1 2p1 3s1 4P0.5 | 12512400.0 cm-1 |
| 1s1 2p1 3s1 4P1.5 | 12513600.0 cm-1 |
| 1s1 2p1 3s1 4P2.5 | 12515800.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 12529000.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 12529900.0 cm-1 |
| 1s1 2p1 3p1 4D0.5 | 12539100.0 cm-1 |
| 1s1 2p1 3p1 4D1.5 | 12540000.0 cm-1 |
| 1s1 2p1 3p1 4D2.5 | 12541500.0 cm-1 |
| 1s1 2p1 3p1 4D3.5 | 12543500.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 12545100.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 12545300.0 cm-1 |
| 1s1 2p1 3p1 4S1.5 | 12558700.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 12561000.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 12564000.0 cm-1 |
| 1s1 2p1 3d1 4F1.5 | 12570200.0 cm-1 |
| 1s1 2p1 3d1 4F2.5 | 12571100.0 cm-1 |
| 1s1 2p1 3p1 4P0.5 | 12571700.0 cm-1 |
| 1s1 2p1 3d1 4F3.5 | 12572300.0 cm-1 |
| 1s1 2p1 3p1 4P1.5 | 12572600.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 12573000.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 12573300.0 cm-1 |
| 1s1 2p1 3d1 4F4.5 | 12573800.0 cm-1 |
| 1s1 2p1 3p1 4P2.5 | 12574100.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 12577900.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 12578300.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 12586400.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 12589200.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 12595300.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 12595800.0 cm-1 |
| 1s1 2p1 3d1 4D0.5 | 12596600.0 cm-1 |
| 1s1 2p1 3d1 4D1.5 | 12596800.0 cm-1 |
| 1s1 2p1 3d1 4D2.5 | 12597200.0 cm-1 |
| 1s1 2p1 3d1 4D3.5 | 12598000.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 12603400.0 cm-1 |
| 1s1 2p1 3d1 4P2.5 | 12606200.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 12606400.0 cm-1 |
| 1s1 2p1 3d1 4P1.5 | 12606900.0 cm-1 |
| 1s1 2p1 3d1 4P0.5 | 12607300.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 12611600.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 12629800.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 12631500.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 12635000.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 12635100.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 12635100.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 12636400.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 12656900.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 12657300.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 12665100.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 12668000.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 12668800.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 12685400.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 12686200.0 cm-1 |
| 1s1 2s1 4s1 4S1.5 | 12996800.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 13010300.0 cm-1 |
| 1s1 2s1 4p1 4P0.5 | 13017000.0 cm-1 |
| 1s1 2s1 4p1 4P1.5 | 13017200.0 cm-1 |
| 1s1 2s1 4p1 4P2.5 | 13017400.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 13022600.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 13022700.0 cm-1 |
| 1s1 2s1 4d1 4D0.5 | 13030100.0 cm-1 |
| 1s1 2s1 4d1 4D1.5 | 13030100.0 cm-1 |
| 1s1 2s1 4d1 4D2.5 | 13030200.0 cm-1 |
| 1s1 2s1 4d1 4D3.5 | 13030300.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 13037100.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 13037200.0 cm-1 |
| 1s1 2s1 4f1 4F1.5 | 13040600.0 cm-1 |
| 1s1 2s1 4f1 4F2.5 | 13040600.0 cm-1 |
| 1s1 2s1 4f1 4F3.5 | 13040600.0 cm-1 |
| 1s1 2s1 4f1 4F4.5 | 13040700.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 13043200.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 13043200.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 13094200.0 cm-1 |
| 1s1 2p1 4s1 4P0.5 | 13105200.0 cm-1 |
| 1s1 2p1 4s1 4P1.5 | 13106400.0 cm-1 |
| 1s1 2p1 4s1 4P2.5 | 13108700.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 13109300.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 13110000.0 cm-1 |
| 1s1 2p1 4p1 4D0.5 | 13118300.0 cm-1 |
| 1s1 2p1 4p1 4D1.5 | 13119100.0 cm-1 |
| 1s1 2p1 4p1 4D2.5 | 13120300.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 13120400.0 cm-1 |
| 1s1 2p1 4p1 4D3.5 | 13122100.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 13122800.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 13123000.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 13123500.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 13125600.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 13125700.0 cm-1 |
| 1s1 2p1 4p1 4S1.5 | 13126200.0 cm-1 |
| 1s1 2p1 4p1 4P0.5 | 13126700.0 cm-1 |
| 1s1 2p1 4p1 4P1.5 | 13128400.0 cm-1 |
| 1s1 2p1 4p1 4P2.5 | 13128700.0 cm-1 |
| 1s1 2p1 4d1 4F1.5 | 13130800.0 cm-1 |
| 1s1 2p1 4d1 4F2.5 | 13131600.0 cm-1 |
| 1s1 2p1 4d1 4F3.5 | 13132700.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 13133500.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 13133600.0 cm-1 |
| 1s1 2p1 4d1 4F4.5 | 13134300.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 13134400.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 13134400.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 13134700.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 13136900.0 cm-1 |
| 1s1 2p1 4d1 4D0.5 | 13138000.0 cm-1 |
| 1s1 2p1 4d1 4D1.5 | 13138200.0 cm-1 |
| 1s1 2p1 4d1 4D2.5 | 13138500.0 cm-1 |
| 1s1 2p1 4d1 4D3.5 | 13139500.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 13140300.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 13140600.0 cm-1 |
| 1s1 2p1 4f1 4F2.5 | 13140700.0 cm-1 |
| 1s1 2p1 4f1 4F1.5 | 13140700.0 cm-1 |
| 1s1 2p1 4f1 4F3.5 | 13140900.0 cm-1 |
| 1s1 2p1 4f1 4F4.5 | 13141300.0 cm-1 |
| 1s1 2p1 4d1 4P2.5 | 13142200.0 cm-1 |
| 1s1 2p1 4d1 4P1.5 | 13142900.0 cm-1 |
| 1s1 2p1 4d1 4P0.5 | 13143300.0 cm-1 |
| 1s1 2p1 4f1 4G2.5 | 13143700.0 cm-1 |
| 1s1 2p1 4f1 4G3.5 | 13144400.0 cm-1 |
| 1s1 2p1 4f1 4G4.5 | 13145400.0 cm-1 |
| 1s1 2p1 4f1 4G5.5 | 13146400.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 13146500.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 13146700.0 cm-1 |
| 1s1 2p1 4f1 4D3.5 | 13148300.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 13148300.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 13148500.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 13148800.0 cm-1 |
| 1s1 2p1 4f1 4D2.5 | 13149000.0 cm-1 |
| 1s1 2p1 4f1 4D1.5 | 13149600.0 cm-1 |
| 1s1 2p1 4f1 4D0.5 | 13150100.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 13150600.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 13150900.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 13151800.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 13152400.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 13176000.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 13176000.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 13190800.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 13190900.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 13191000.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 13191500.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 13200000.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 13201400.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 13201600.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 13203300.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 13203700.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 13205300.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 13205400.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 13210000.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 13210000.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 13210300.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 13210600.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 13213600.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 13213700.0 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 = 1.27930 2S = 1.03013 2P = 0.92365 3S = 1.01801 3P = 0.91745 3D = 0.84911 4S = 1.01666 4P = 0.91720 4D = 0.85103 4F = 0.97842 5S = 1.01805 5P = 0.91875 5D = 0.85430 5F = 0.83558 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 384.1702 Rydbergs (5227.019741 eV) A fine energy mesh of 0.000004 Z**2 Rydbergs (0.004408344 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (11.02086 eV) was used from the last threshold up to 3.595001 Z**2 Rydbergs (3962 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (11.02086 eV) was used from first threshold up to 3.595001 Z**2 Rydbergs (3962 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 = 1.28343 2S = 1.03229 2P = 0.92693 3S = 1.02068 3P = 0.91919 3D = 0.85310 4S = 1.02002 4P = 0.92012 4D = 0.85826 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 0.000010 Z**2 Rydbergs (0.01102086 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (11.02086 eV) was used from the last threshold up to 3.334558 Z**2 Rydbergs (3674.97 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (11.02086 eV) was used from first threshold up to 3.334558 Z**2 Rydbergs (3674.97 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 1.45816 3 1.4944 4 15.3339 5 15.7332 6 15.7451 7 15.888 8 15.8915 9 20.527 10 20.6871 11 20.6871 12 20.7530 13 20.756 14 20.7592 15 20.7599 16 22.887 17 22.972 18 22.972 19 23.004 20 23.006 21 23.0097 22 23.0100 26 97.01695 27 97.0262 28 97.0509 29 98.1544 31 98.5690 32 98.58570 33 98.6037 34 98.681 35 98.681 36 99.273 38 99.510 40 100.31 46 113.17 58 113.94 64 114.07 80 114.46 Produced by: Guiyun Liang Date: 25/11/10 ------------------------------------------------------------------------