nelike_lgy09#br25.dat
Resolved Specific Ion Data Collections
- Ion
- Br25+
- Temperature Range
- 11.63 eV → 1.163 x 105 eV
ADF04
- Filename
- nelike_lgy09#br25.dat
- Full Path
- adf04/copaw#ne/nelike_lgy09#br25.dat
Download data
- Spontaneous Emission: Br+25(i) → Br+25(j) + hv
- Electron Impact Excitation: Br+25(i) + e → Br+25(j) + e
| 2s2 2p6 1S0.0 | 0.0 cm-1 |
| 2s2 2p5 3s1 3P2.0 | 12440000.0 cm-1 |
| 2s2 2p5 3s1 1P1.0 | 12462300.0 cm-1 |
| 2s2 2p5 3s1 3P0.0 | 12833400.0 cm-1 |
| 2s2 2p5 3s1 3P1.0 | 12845300.0 cm-1 |
| 2s2 2p5 3p1 3S1.0 | 12847200.0 cm-1 |
| 2s2 2p5 3p1 3D2.0 | 12872800.0 cm-1 |
| 2s2 2p5 3p1 3D3.0 | 12952800.0 cm-1 |
| 2s2 2p5 3p1 1P1.0 | 12955700.0 cm-1 |
| 2s2 2p5 3p1 3P2.0 | 12988200.0 cm-1 |
| 2s2 2p5 3p1 3P0.0 | 13112400.0 cm-1 |
| 2s2 2p5 3p1 3D1.0 | 13257900.0 cm-1 |
| 2s2 2p5 3p1 3P1.0 | 13353400.0 cm-1 |
| 2s2 2p5 3p1 1D2.0 | 13363400.0 cm-1 |
| 2s2 2p5 3p1 1S0.0 | 13432600.0 cm-1 |
| 2s2 2p5 3d1 3P0.0 | 13451100.0 cm-1 |
| 2s2 2p5 3d1 3P1.0 | 13470700.0 cm-1 |
| 2s2 2p5 3d1 3F3.0 | 13499700.0 cm-1 |
| 2s2 2p5 3d1 3P2.0 | 13505100.0 cm-1 |
| 2s2 2p5 3d1 3F4.0 | 13507400.0 cm-1 |
| 2s2 2p5 3d1 1D2.0 | 13527800.0 cm-1 |
| 2s2 2p5 3d1 3D3.0 | 13553500.0 cm-1 |
| 2s2 2p5 3d1 3D1.0 | 13637100.0 cm-1 |
| 2s2 2p5 3d1 3F2.0 | 13888800.0 cm-1 |
| 2s2 2p5 3d1 3D2.0 | 13914400.0 cm-1 |
| 2s2 2p5 3d1 1F3.0 | 13926100.0 cm-1 |
| 2s2 2p5 3d1 1P1.0 | 13987200.0 cm-1 |
| 2s1 2p6 3s1 3S1.0 | 14297700.0 cm-1 |
| 2s1 2p6 3s1 1S0.0 | 14392500.0 cm-1 |
| 2s1 2p6 3p1 3P0.0 | 14718900.0 cm-1 |
| 2s1 2p6 3p1 3P1.0 | 14727000.0 cm-1 |
| 2s1 2p6 3p1 3P2.0 | 14813500.0 cm-1 |
| 2s1 2p6 3p1 1P1.0 | 14833700.0 cm-1 |
| 2s1 2p6 3d1 3D1.0 | 15331300.0 cm-1 |
| 2s1 2p6 3d1 3D2.0 | 15339500.0 cm-1 |
| 2s1 2p6 3d1 3D3.0 | 15357200.0 cm-1 |
| 2s1 2p6 3d1 1D2.0 | 15414900.0 cm-1 |
| 2s2 2p5 4s1 3P2.0 | 16871900.0 cm-1 |
| 2s2 2p5 4s1 1P1.0 | 16878100.0 cm-1 |
| 2s2 2p5 4p1 3S1.0 | 17035400.0 cm-1 |
| 2s2 2p5 4p1 3D2.0 | 17041600.0 cm-1 |
| 2s2 2p5 4p1 3D3.0 | 17071100.0 cm-1 |
| 2s2 2p5 4p1 1P1.0 | 17072200.0 cm-1 |
| 2s2 2p5 4p1 3P2.0 | 17082600.0 cm-1 |
| 2s2 2p5 4p1 1S0.0 | 17135500.0 cm-1 |
| 2s2 2p5 4d1 3P0.0 | 17257800.0 cm-1 |
| 2s2 2p5 4d1 3P1.0 | 17264500.0 cm-1 |
| 2s2 2p5 4s1 3P0.0 | 17267700.0 cm-1 |
| 2s2 2p5 4s1 3P1.0 | 17270500.0 cm-1 |
| 2s2 2p5 4d1 3F3.0 | 17274800.0 cm-1 |
| 2s2 2p5 4d1 3D2.0 | 17278400.0 cm-1 |
| 2s2 2p5 4d1 3F4.0 | 17279200.0 cm-1 |
| 2s2 2p5 4d1 1D2.0 | 17285500.0 cm-1 |
| 2s2 2p5 4d1 3D3.0 | 17295000.0 cm-1 |
| 2s2 2p5 4d1 1P1.0 | 17330300.0 cm-1 |
| 2s2 2p5 4f1 3D1.0 | 17381900.0 cm-1 |
| 2s2 2p5 4f1 1G4.0 | 17384900.0 cm-1 |
| 2s2 2p5 4f1 3D2.0 | 17386100.0 cm-1 |
| 2s2 2p5 4f1 3G5.0 | 17389300.0 cm-1 |
| 2s2 2p5 4f1 3F3.0 | 17391500.0 cm-1 |
| 2s2 2p5 4f1 1D2.0 | 17391700.0 cm-1 |
| 2s2 2p5 4f1 1F3.0 | 17393200.0 cm-1 |
| 2s2 2p5 4f1 3F4.0 | 17396600.0 cm-1 |
| 2s2 2p5 4p1 3D1.0 | 17433100.0 cm-1 |
| 2s2 2p5 4p1 3P1.0 | 17467600.0 cm-1 |
| 2s2 2p5 4p1 1D2.0 | 17470800.0 cm-1 |
| 2s2 2p5 4p1 3P0.0 | 17473700.0 cm-1 |
| 2s2 2p5 4d1 3F2.0 | 17667200.0 cm-1 |
| 2s2 2p5 4d1 3P2.0 | 17677600.0 cm-1 |
| 2s2 2p5 4d1 1F3.0 | 17682000.0 cm-1 |
| 2s2 2p5 4d1 3D1.0 | 17697700.0 cm-1 |
| 2s2 2p5 4f1 3G3.0 | 17781100.0 cm-1 |
| 2s2 2p5 4f1 3F2.0 | 17783600.0 cm-1 |
| 2s2 2p5 4f1 3G4.0 | 17786200.0 cm-1 |
| 2s2 2p5 4f1 3D3.0 | 17786700.0 cm-1 |
| 2s1 2p6 4s1 3S1.0 | 18707800.0 cm-1 |
| 2s1 2p6 4s1 1S0.0 | 18736200.0 cm-1 |
| 2s2 2p5 5s1 3P2.0 | 18805500.0 cm-1 |
| 2s2 2p5 5s1 1P1.0 | 18808400.0 cm-1 |
| 2s1 2p6 4p1 3P0.0 | 18877100.0 cm-1 |
| 2s1 2p6 4p1 3P1.0 | 18881800.0 cm-1 |
| 2s2 2p5 5p1 3S1.0 | 18890900.0 cm-1 |
| 2s2 2p5 5p1 3D2.0 | 18891400.0 cm-1 |
| 2s2 2p5 5p1 3D3.0 | 18906000.0 cm-1 |
| 2s2 2p5 5p1 1P1.0 | 18907200.0 cm-1 |
| 2s2 2p5 5p1 3P2.0 | 18911500.0 cm-1 |
| 2s1 2p6 4p1 3P2.0 | 18913500.0 cm-1 |
| 2s1 2p6 4p1 1P1.0 | 18917800.0 cm-1 |
| 2s2 2p5 5p1 1S0.0 | 18937000.0 cm-1 |
| 2s2 2p5 5d1 3P0.0 | 18999400.0 cm-1 |
| 2s2 2p5 5d1 3P1.0 | 19002700.0 cm-1 |
| 2s2 2p5 5d1 3F3.0 | 19005500.0 cm-1 |
| 2s2 2p5 5d1 3D2.0 | 19007900.0 cm-1 |
| 2s2 2p5 5d1 3F4.0 | 19008200.0 cm-1 |
| 2s2 2p5 5d1 1D2.0 | 19010700.0 cm-1 |
| 2s2 2p5 5d1 3D3.0 | 19015400.0 cm-1 |
| 2s2 2p5 5d1 1P1.0 | 19032300.0 cm-1 |
| 2s2 2p5 5f1 3D1.0 | 19054300.0 cm-1 |
| 2s2 2p5 5f1 3D2.0 | 19057400.0 cm-1 |
| 2s2 2p5 5f1 1G4.0 | 19060600.0 cm-1 |
| 2s2 2p5 5f1 3F3.0 | 19062100.0 cm-1 |
| 2s2 2p5 5f1 3G5.0 | 19063100.0 cm-1 |
| 2s2 2p5 5f1 1F3.0 | 19063400.0 cm-1 |
| 2s2 2p5 5f1 1D2.0 | 19063400.0 cm-1 |
| 2s2 2p5 5g1 3F2.0 | 19064400.0 cm-1 |
| 2s2 2p5 5g1 3F3.0 | 19065200.0 cm-1 |
| 2s2 2p5 5f1 3F4.0 | 19066200.0 cm-1 |
| 2s2 2p5 5g1 3G3.0 | 19068300.0 cm-1 |
| 2s2 2p5 5g1 1H5.0 | 19068800.0 cm-1 |
| 2s2 2p5 5g1 1G4.0 | 19069300.0 cm-1 |
| 2s2 2p5 5g1 3G4.0 | 19070200.0 cm-1 |
| 2s2 2p5 5g1 3H6.0 | 19071100.0 cm-1 |
| 2s2 2p5 5g1 3G5.0 | 19072000.0 cm-1 |
| 2s1 2p6 4d1 3D1.0 | 19111500.0 cm-1 |
| 2s1 2p6 4d1 3D2.0 | 19113800.0 cm-1 |
| 2s1 2p6 4d1 3D3.0 | 19119900.0 cm-1 |
| 2s1 2p6 4d1 1D2.0 | 19138000.0 cm-1 |
| 2s2 2p5 5s1 3P0.0 | 19202800.0 cm-1 |
| 2s2 2p5 5s1 3P1.0 | 19204100.0 cm-1 |
| 2s1 2p6 4f1 3F3.0 | 19220300.0 cm-1 |
| 2s1 2p6 4f1 3F2.0 | 19222500.0 cm-1 |
| 2s1 2p6 4f1 3F4.0 | 19223600.0 cm-1 |
| 2s1 2p6 4f1 1F3.0 | 19228300.0 cm-1 |
| 2s2 2p5 5p1 3D1.0 | 19285800.0 cm-1 |
| 2s2 2p5 5p1 3P0.0 | 19302200.0 cm-1 |
| 2s2 2p5 5p1 3P1.0 | 19302400.0 cm-1 |
| 2s2 2p5 5p1 1D2.0 | 19304000.0 cm-1 |
| 2s2 2p5 5d1 3F2.0 | 19399300.0 cm-1 |
| 2s2 2p5 5d1 3P2.0 | 19404600.0 cm-1 |
| 2s2 2p5 5d1 1F3.0 | 19406600.0 cm-1 |
| 2s2 2p5 5d1 3D1.0 | 19413000.0 cm-1 |
| 2s2 2p5 5f1 3G3.0 | 19455700.0 cm-1 |
| 2s2 2p5 5f1 3F2.0 | 19457200.0 cm-1 |
| 2s2 2p5 5f1 3G4.0 | 19458500.0 cm-1 |
| 2s2 2p5 5f1 3D3.0 | 19458700.0 cm-1 |
| 2s2 2p5 5g1 3H4.0 | 19464000.0 cm-1 |
| 2s2 2p5 5g1 1F3.0 | 19465100.0 cm-1 |
| 2s2 2p5 5g1 3H5.0 | 19465500.0 cm-1 |
| 2s2 2p5 5g1 3F4.0 | 19466700.0 cm-1 |
| 2s2 2p5 6s1 3P2.0 | 19830200.0 cm-1 |
| 2s2 2p5 6s1 1P1.0 | 19831800.0 cm-1 |
| 2s2 2p5 6p1 3S1.0 | 19877100.0 cm-1 |
| 2s2 2p5 6p1 3D2.0 | 19878500.0 cm-1 |
| 2s2 2p5 6p1 3D3.0 | 19886300.0 cm-1 |
| 2s2 2p5 6p1 1P1.0 | 19886900.0 cm-1 |
| 2s2 2p5 6p1 3P2.0 | 19889300.0 cm-1 |
| 2s2 2p5 6p1 1S0.0 | 19903400.0 cm-1 |
| 2s2 2p5 6d1 3P0.0 | 19938200.0 cm-1 |
| 2s2 2p5 6d1 3P1.0 | 19940200.0 cm-1 |
| 2s2 2p5 6d1 3F3.0 | 19942300.0 cm-1 |
| 2s2 2p5 6d1 3D2.0 | 19943200.0 cm-1 |
| 2s2 2p5 6d1 3F4.0 | 19943500.0 cm-1 |
| 2s2 2p5 6d1 1D2.0 | 19945400.0 cm-1 |
| 2s2 2p5 6d1 3D3.0 | 19947700.0 cm-1 |
| 2s2 2p5 6d1 1P1.0 | 19957500.0 cm-1 |
| 2s2 2p5 6s1 3P0.0 | 20224400.0 cm-1 |
| 2s2 2p5 6s1 3P1.0 | 20225200.0 cm-1 |
| 2s2 2p5 6p1 3D1.0 | 20271900.0 cm-1 |
| 2s2 2p5 6p1 3P0.0 | 20280500.0 cm-1 |
| 2s2 2p5 6p1 3P1.0 | 20280900.0 cm-1 |
| 2s2 2p5 6p1 1D2.0 | 20281900.0 cm-1 |
| 2s2 2p5 6d1 3F2.0 | 20335900.0 cm-1 |
| 2s2 2p5 6d1 3P2.0 | 20338700.0 cm-1 |
| 2s2 2p5 6d1 1F3.0 | 20339900.0 cm-1 |
| 2s2 2p5 6d1 3D1.0 | 20343100.0 cm-1 |
| 2s2 2p5 7s1 3P2.0 | 20433900.0 cm-1 |
| 2s2 2p5 7s1 1P1.0 | 20434800.0 cm-1 |
| 2s2 2p5 7p1 3S1.0 | 20463000.0 cm-1 |
| 2s2 2p5 7p1 3D2.0 | 20463900.0 cm-1 |
| 2s2 2p5 7p1 3D3.0 | 20468500.0 cm-1 |
| 2s2 2p5 7p1 1P1.0 | 20468800.0 cm-1 |
| 2s2 2p5 7p1 3P2.0 | 20470300.0 cm-1 |
| 2s2 2p5 7p1 1S0.0 | 20478900.0 cm-1 |
| 2s2 2p5 7d1 3P0.0 | 20500800.0 cm-1 |
| 2s2 2p5 7d1 3P1.0 | 20501900.0 cm-1 |
| 2s2 2p5 7d1 3F3.0 | 20503200.0 cm-1 |
| 2s2 2p5 7d1 3D2.0 | 20503800.0 cm-1 |
| 2s2 2p5 7d1 3F4.0 | 20503900.0 cm-1 |
| 2s2 2p5 7d1 1D2.0 | 20505100.0 cm-1 |
| 2s2 2p5 7d1 3D3.0 | 20506400.0 cm-1 |
| 2s2 2p5 7d1 1P1.0 | 20512600.0 cm-1 |
| 2s1 2p6 5s1 3S1.0 | 20642700.0 cm-1 |
| 2s1 2p6 5s1 1S0.0 | 20653800.0 cm-1 |
| 2s1 2p6 5p1 3P0.0 | 20726100.0 cm-1 |
| 2s1 2p6 5p1 3P1.0 | 20727400.0 cm-1 |
| 2s1 2p6 5p1 3P2.0 | 20742500.0 cm-1 |
| 2s1 2p6 5p1 1P1.0 | 20745200.0 cm-1 |
| 2s2 2p5 7s1 3P0.0 | 20828500.0 cm-1 |
| 2s2 2p5 7s1 3P1.0 | 20829000.0 cm-1 |
| 2s1 2p6 5d1 3D1.0 | 20837400.0 cm-1 |
| 2s1 2p6 5d1 3D2.0 | 20839300.0 cm-1 |
| 2s1 2p6 5d1 3D3.0 | 20843100.0 cm-1 |
| 2s1 2p6 5d1 1D2.0 | 20851300.0 cm-1 |
| 2s2 2p5 7p1 3D1.0 | 20858400.0 cm-1 |
| 2s2 2p5 7p1 3P0.0 | 20862700.0 cm-1 |
| 2s2 2p5 7p1 3P1.0 | 20863300.0 cm-1 |
| 2s2 2p5 7p1 1D2.0 | 20864600.0 cm-1 |
| 2s1 2p6 5f1 3F2.0 | 20892800.0 cm-1 |
| 2s1 2p6 5f1 3F3.0 | 20893300.0 cm-1 |
| 2s1 2p6 5f1 3F4.0 | 20895100.0 cm-1 |
| 2s1 2p6 5f1 1F3.0 | 20896100.0 cm-1 |
| 2s2 2p5 7d1 3F2.0 | 20897000.0 cm-1 |
| 2s2 2p5 7d1 3P2.0 | 20898800.0 cm-1 |
| 2s2 2p5 7d1 1F3.0 | 20899800.0 cm-1 |
| 2s1 2p6 5g1 3G3.0 | 20900700.0 cm-1 |
| 2s1 2p6 5g1 3G4.0 | 20900800.0 cm-1 |
| 2s2 2p5 7d1 3D1.0 | 20901500.0 cm-1 |
| 2s1 2p6 5g1 3G5.0 | 20902100.0 cm-1 |
| 2s1 2p6 5g1 1G4.0 | 20902100.0 cm-1 |
------------------------------------------------------------------------ Result of ICFT R-matrix calculation +++++++++++++++++++++++++++++++++++ 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 = 1.00000 2S = 1.85007 2P = 1.19293 3S = 1.50166 3P = 1.18969 3D = 1.09746 4S = 1.000 4P = 1.000 4D = 1.000 4F = 1.000 5S = 1.000 5P = 1.000 5D = 1.000 5F = 1.000 5G = 1.000 6S = 1.000 6P = 1.000 6D = 1.000 7S = 1.000 7P = 1.000 7D = 1.000 An exchange calculation was performed up to J=11.5 A non-exchange calculation was then performed up to J=39.5 Followed by a top-up calculation to J -> infinity. 60 continuum basis orbitals were used, giving a smallest maximum basis-orbital energy of 792.0180 Rydbergs (10776.196908 eV) A fine energy mesh of 0.000005 Z**2 Rydbergs (0.04251875 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.002000 Z**2 Rydbergs (17.0075 eV) was used from the last threshold up to 0.896428 Z**2 Rydbergs (7623 eV) in the excitation calculation. A coarse energy mesh of 0.002000 Z**2 Rydbergs (17.0075 eV) was used from first threshold up to 0.896428 Z**2 Rydbergs (7623 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: 16/11/09 ------------------------------------------------------------------------