lilike_lgy10#br32.dat
Resolved Specific Ion Data Collections
- Ion
- Br32+
- Temperature Range
- 18.78 eV → 1.878 x 105 eV
ADF04
- Filename
- lilike_lgy10#br32.dat
- Full Path
- adf04/copaw#li/lilike_lgy10#br32.dat
Download data
- Spontaneous Emission: Br+32(i) → Br+32(j) + hv
- Electron Impact Excitation: Br+32(i) + e → Br+32(j) + e
| 2s1 2S0.5 | 0.0 cm-1 |
| 2p1 2P0.5 | 555154.0 cm-1 |
| 2p1 2P1.5 | 1008610.0 cm-1 |
| 3s1 2S0.5 | 17526000.0 cm-1 |
| 3p1 2P0.5 | 17679200.0 cm-1 |
| 3p1 2P1.5 | 17808700.0 cm-1 |
| 3d1 2D1.5 | 17871200.0 cm-1 |
| 3d1 2D2.5 | 17914300.0 cm-1 |
| 4s1 2S0.5 | 23571200.0 cm-1 |
| 4p1 2P0.5 | 23634100.0 cm-1 |
| 4p1 2P1.5 | 23686600.0 cm-1 |
| 4d1 2D1.5 | 23712500.0 cm-1 |
| 4d1 2D2.5 | 23730400.0 cm-1 |
| 4f1 2F2.5 | 23731800.0 cm-1 |
| 4f1 2F3.5 | 23740900.0 cm-1 |
| 5s1 2S0.5 | 26346300.0 cm-1 |
| 5p1 2P0.5 | 26378000.0 cm-1 |
| 5p1 2P1.5 | 26403500.0 cm-1 |
| 5d1 2D1.5 | 26416600.0 cm-1 |
| 5d1 2D2.5 | 26425600.0 cm-1 |
| 5f1 2F2.5 | 26426400.0 cm-1 |
| 5f1 2F3.5 | 26431000.0 cm-1 |
| 5g1 2G3.5 | 26431000.0 cm-1 |
| 5g1 2G4.5 | 26433800.0 cm-1 |
| 1s1 2s2 2S0.5 | 98630700.0 cm-1 |
| 1s1 2s1 2p1 4P0.5 | 98758400.0 cm-1 |
| 1s1 2s1 2p1 4P1.5 | 98854200.0 cm-1 |
| 1s1 2s1 2p1 4P2.5 | 99192000.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 99239100.0 cm-1 |
| 1s1 2p2 4P0.5 | 99489200.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 99542900.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 99695100.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 99756800.0 cm-1 |
| 1s1 2p2 4P1.5 | 99768200.0 cm-1 |
| 1s1 2p2 4P2.5 | 99889500.0 cm-1 |
| 1s1 2p2 2P0.5 | 100031000.0 cm-1 |
| 1s1 2p2 2D1.5 | 100051000.0 cm-1 |
| 1s1 2p2 2D2.5 | 100339000.0 cm-1 |
| 1s1 2p2 2P1.5 | 100518000.0 cm-1 |
| 1s1 2p2 2S0.5 | 100690000.0 cm-1 |
| 1s1 2s1 3s1 4S1.5 | 116352000.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 116515000.0 cm-1 |
| 1s1 2s1 3p1 4P0.5 | 116552000.0 cm-1 |
| 1s1 2s1 3p1 4P1.5 | 116561000.0 cm-1 |
| 1s1 2s1 3p1 4P2.5 | 116671000.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 116676000.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 116680000.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 116754000.0 cm-1 |
| 1s1 2s1 3d1 4D0.5 | 116765000.0 cm-1 |
| 1s1 2s1 3d1 4D1.5 | 116781000.0 cm-1 |
| 1s1 2p1 3s1 4P0.5 | 116794000.0 cm-1 |
| 1s1 2s1 3d1 4D2.5 | 116801000.0 cm-1 |
| 1s1 2s1 3d1 4D3.5 | 116830000.0 cm-1 |
| 1s1 2p1 3s1 4P1.5 | 116856000.0 cm-1 |
| 1s1 2p1 3p1 4D0.5 | 116879000.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 116883000.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 116886000.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 116896000.0 cm-1 |
| 1s1 2p1 3p1 4D1.5 | 116922000.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 116964000.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 117031000.0 cm-1 |
| 1s1 2p1 3p1 4S1.5 | 117055000.0 cm-1 |
| 1s1 2p1 3p1 4P0.5 | 117073000.0 cm-1 |
| 1s1 2p1 3p1 4D2.5 | 117084000.0 cm-1 |
| 1s1 2p1 3d1 4F1.5 | 117112000.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 117132000.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 117148000.0 cm-1 |
| 1s1 2p1 3d1 4F2.5 | 117155000.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 117165000.0 cm-1 |
| 1s1 2p1 3s1 4P2.5 | 117194000.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 117211000.0 cm-1 |
| 1s1 2p1 3d1 4D2.5 | 117228000.0 cm-1 |
| 1s1 2p1 3d1 4F3.5 | 117256000.0 cm-1 |
| 1s1 2p1 3d1 4D1.5 | 117258000.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 117264000.0 cm-1 |
| 1s1 2p1 3d1 4D0.5 | 117266000.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 117287000.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 117327000.0 cm-1 |
| 1s1 2p1 3p1 4P1.5 | 117374000.0 cm-1 |
| 1s1 2p1 3p1 4P2.5 | 117404000.0 cm-1 |
| 1s1 2p1 3p1 4D3.5 | 117427000.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 117436000.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 117441000.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 117471000.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 117530000.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 117558000.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 117578000.0 cm-1 |
| 1s1 2p1 3d1 4F4.5 | 117581000.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 117587000.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 117600000.0 cm-1 |
| 1s1 2p1 3d1 4D3.5 | 117610000.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 117625000.0 cm-1 |
| 1s1 2p1 3d1 4P0.5 | 117637000.0 cm-1 |
| 1s1 2p1 3d1 4P2.5 | 117652000.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 117661000.0 cm-1 |
| 1s1 2p1 3d1 4P1.5 | 117673000.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 117684000.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 117722000.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 117751000.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 117766000.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 117792000.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 117802000.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 117827000.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 117841000.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 117875000.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 117906000.0 cm-1 |
| 1s1 2s1 4s1 4S1.5 | 122534000.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 122586000.0 cm-1 |
| 1s1 2s1 4p1 4P0.5 | 122607000.0 cm-1 |
| 1s1 2s1 4p1 4P1.5 | 122613000.0 cm-1 |
| 1s1 2s1 4p1 4P2.5 | 122652000.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 122667000.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 122672000.0 cm-1 |
| 1s1 2s1 4d1 4D0.5 | 122698000.0 cm-1 |
| 1s1 2s1 4d1 4D1.5 | 122701000.0 cm-1 |
| 1s1 2s1 4d1 4D2.5 | 122705000.0 cm-1 |
| 1s1 2s1 4d1 4D3.5 | 122717000.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 122733000.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 122736000.0 cm-1 |
| 1s1 2s1 4f1 4F1.5 | 122750000.0 cm-1 |
| 1s1 2s1 4f1 4F2.5 | 122752000.0 cm-1 |
| 1s1 2s1 4f1 4F3.5 | 122753000.0 cm-1 |
| 1s1 2s1 4f1 4F4.5 | 122760000.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 122764000.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 122766000.0 cm-1 |
| 1s1 2p1 4s1 4P0.5 | 122894000.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 122895000.0 cm-1 |
| 1s1 2p1 4p1 4D0.5 | 122937000.0 cm-1 |
| 1s1 2p1 4s1 4P1.5 | 122943000.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 122958000.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 122974000.0 cm-1 |
| 1s1 2p1 4p1 4D1.5 | 122984000.0 cm-1 |
| 1s1 2p1 4p1 4S1.5 | 123004000.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 123009000.0 cm-1 |
| 1s1 2p1 4p1 4P0.5 | 123028000.0 cm-1 |
| 1s1 2p1 4d1 4F1.5 | 123031000.0 cm-1 |
| 1s1 2p1 4p1 4D2.5 | 123045000.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 123053000.0 cm-1 |
| 1s1 2p1 4d1 4F2.5 | 123062000.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 123065000.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 123068000.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 123075000.0 cm-1 |
| 1s1 2p1 4d1 4D2.5 | 123078000.0 cm-1 |
| 1s1 2p1 4f1 4G2.5 | 123080000.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 123090000.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 123100000.0 cm-1 |
| 1s1 2p1 4d1 4P1.5 | 123107000.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 123107000.0 cm-1 |
| 1s1 2p1 4d1 4D0.5 | 123113000.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 123116000.0 cm-1 |
| 1s1 2p1 4d1 4F3.5 | 123118000.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 123125000.0 cm-1 |
| 1s1 2p1 4f1 4G3.5 | 123133000.0 cm-1 |
| 1s1 2p1 4f1 4F1.5 | 123136000.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 123139000.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 123144000.0 cm-1 |
| 1s1 2p1 4f1 4F4.5 | 123145000.0 cm-1 |
| 1s1 2p1 4f1 4D3.5 | 123149000.0 cm-1 |
| 1s1 2p1 4s1 4P2.5 | 123330000.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 123361000.0 cm-1 |
| 1s1 2p1 4p1 4P1.5 | 123393000.0 cm-1 |
| 1s1 2p1 4p1 4P2.5 | 123399000.0 cm-1 |
| 1s1 2p1 4p1 4D3.5 | 123422000.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 123440000.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 123461000.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 123475000.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 123480000.0 cm-1 |
| 1s1 2p1 4d1 4F4.5 | 123483000.0 cm-1 |
| 1s1 2p1 4d1 4D3.5 | 123486000.0 cm-1 |
| 1s1 2p1 4d1 4D1.5 | 123491000.0 cm-1 |
| 1s1 2p1 4d1 4P0.5 | 123495000.0 cm-1 |
| 1s1 2p1 4d1 4P2.5 | 123504000.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 123510000.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 123518000.0 cm-1 |
| 1s1 2p1 4f1 4F3.5 | 123519000.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 123521000.0 cm-1 |
| 1s1 2p1 4f1 4F2.5 | 123523000.0 cm-1 |
| 1s1 2p1 4f1 4G4.5 | 123525000.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 123527000.0 cm-1 |
| 1s1 2p1 4f1 4D1.5 | 123530000.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 123531000.0 cm-1 |
| 1s1 2p1 4f1 4G5.5 | 123535000.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 123535000.0 cm-1 |
| 1s1 2p1 4f1 4D0.5 | 123536000.0 cm-1 |
| 1s1 2p1 4f1 4D2.5 | 123538000.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 123541000.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 123548000.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 123579000.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 123579000.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 123617000.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 123630000.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 123639000.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 123664000.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 123669000.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 123674000.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 123680000.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 123692000.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 123697000.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 123704000.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 123704000.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 123711000.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 123715000.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 123715000.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 123725000.0 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 = 1.28329 2S = 1.05004 2P = 0.95416 3S = 1.03628 3P = 0.94728 3D = 0.87994 4S = 1.03591 4P = 0.94648 4D = 0.88231 4F = 1.06575 5S = 1.03719 5P = 0.94691 5D = 0.88770 5F = 0.83535 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 3727.4412 Rydbergs (50715.564967 eV) A fine energy mesh of 0.000004 Z**2 Rydbergs (0.055730176 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (139.32544 eV) was used from the last threshold up to 2.718097 Z**2 Rydbergs (37870 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (139.32544 eV) was used from first threshold up to 2.718097 Z**2 Rydbergs (37870 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: 12/10/10 ------------------------------------------------------------------------ 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 = 1.28874 2S = 1.05165 2P = 0.95599 3S = 1.03895 3P = 0.94790 3D = 0.88744 4S = 1.03891 4P = 0.94850 4D = 0.89165 4F = 1.03607 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 0.000004 Z**2 Rydbergs (0.055730176 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (139.32544 eV) was used from the last threshold up to 2.718097 Z**2 Rydbergs (37870 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (139.32544 eV) was used from first threshold up to 2.718097 Z**2 Rydbergs (37870 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 5.07029 3 9.298569 Produced by: Guiyun Liang Date: 13/08/10 ------------------------------------------------------------------------