Resolved Specific Ion Data Collections

Temperature Range
12.58 eV → 1.258 x 105 eV


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  • Spontaneous Emission: Br+26(i) → Br+26(j) + hv
  • Electron Impact Excitation: Br+26(i) + e → Br+26(j) + e
2s2 2p5 2P1.5 0.0 cm-1
2s2 2p5 2P0.5 394492.0 cm-1
2s1 2p6 2S0.5 1801680.0 cm-1
2s2 2p4 3s1 4P2.5 13037900.0 cm-1
2s2 2p4 3s1 2P1.5 13076900.0 cm-1
2s2 2p4 3s1 4P0.5 13212800.0 cm-1
2s2 2p4 3s1 4P1.5 13399000.0 cm-1
2s2 2p4 3p1 4P1.5 13409900.0 cm-1
2s2 2p4 3p1 4P2.5 13427300.0 cm-1
2s2 2p4 3s1 2P0.5 13430600.0 cm-1
2s2 2p4 3p1 2P0.5 13505600.0 cm-1
2s2 2p4 3s1 2D2.5 13510700.0 cm-1
2s2 2p4 3p1 2D2.5 13512500.0 cm-1
2s2 2p4 3p1 4D3.5 13519200.0 cm-1
2s2 2p4 3s1 2D1.5 13522200.0 cm-1
2s2 2p4 3p1 4D0.5 13597800.0 cm-1
2s2 2p4 3p1 4S1.5 13640500.0 cm-1
2s2 2p4 3p1 4D1.5 13699000.0 cm-1
2s2 2p4 3p1 4P0.5 13761700.0 cm-1
2s2 2p4 3p1 2D1.5 13804400.0 cm-1
2s2 2p4 3p1 4D2.5 13867900.0 cm-1
2s2 2p4 3p1 2F2.5 13887200.0 cm-1
2s2 2p4 3p1 2S0.5 13894300.0 cm-1
2s2 2p4 3p1 2D1.5 13898600.0 cm-1
2s2 2p4 3s1 2S0.5 13960900.0 cm-1
2s2 2p4 3p1 2F3.5 13978700.0 cm-1
2s2 2p4 3d1 4D2.5 13981100.0 cm-1
2s2 2p4 3d1 4D1.5 13981300.0 cm-1
2s2 2p4 3p1 2P1.5 13981900.0 cm-1
2s2 2p4 3d1 4D3.5 13994800.0 cm-1
2s2 2p4 3d1 2P0.5 13996500.0 cm-1
2s2 2p4 3p1 2D2.5 14013500.0 cm-1
2s2 2p4 3p1 2P1.5 14016300.0 cm-1
2s2 2p4 3d1 4F4.5 14025800.0 cm-1
2s2 2p4 3d1 2F3.5 14028100.0 cm-1
2s2 2p4 3d1 4P0.5 14069500.0 cm-1
2s2 2p4 3d1 4P1.5 14103000.0 cm-1
2s2 2p4 3d1 2D2.5 14130800.0 cm-1
2s2 2p4 3p1 2P0.5 14137200.0 cm-1
2s2 2p4 3d1 4F1.5 14184800.0 cm-1
2s2 2p4 3d1 4P2.5 14214500.0 cm-1
2s2 2p4 3d1 4D0.5 14320800.0 cm-1
2s2 2p4 3d1 2D1.5 14356800.0 cm-1
2s2 2p4 3d1 4F3.5 14370600.0 cm-1
2s2 2p4 3d1 4F2.5 14399600.0 cm-1
2s2 2p4 3p1 2P0.5 14407500.0 cm-1
2s2 2p4 3d1 2F2.5 14412900.0 cm-1
2s2 2p4 3d1 2P1.5 14420900.0 cm-1
2s2 2p4 3p1 2P1.5 14436000.0 cm-1
2s2 2p4 3d1 2G3.5 14455900.0 cm-1
2s2 2p4 3d1 2G4.5 14478500.0 cm-1
2s2 2p4 3d1 2S0.5 14499600.0 cm-1
2s2 2p4 3d1 2D2.5 14502400.0 cm-1
2s2 2p4 3d1 2P1.5 14526500.0 cm-1
2s2 2p4 3d1 2F3.5 14527700.0 cm-1
2s2 2p4 3d1 2F2.5 14538000.0 cm-1
2s2 2p4 3d1 2D1.5 14603700.0 cm-1
2s1 2p5 3s1 4P2.5 14625300.0 cm-1
2s2 2p4 3d1 2P0.5 14626200.0 cm-1
2s1 2p5 3s1 2P1.5 14692900.0 cm-1
2s1 2p5 3s1 4P1.5 14834800.0 cm-1
2s1 2p5 3s1 2P0.5 14837400.0 cm-1
2s2 2p4 3d1 2D2.5 14945500.0 cm-1
2s2 2p4 3d1 2D1.5 14974000.0 cm-1
2s1 2p5 3p1 4S1.5 14993500.0 cm-1
2s1 2p5 3p1 4D2.5 15022900.0 cm-1
2s1 2p5 3s1 4P0.5 15051200.0 cm-1
2s1 2p5 3p1 4D3.5 15091900.0 cm-1
2s1 2p5 3p1 4D1.5 15112600.0 cm-1
2s1 2p5 3p1 4P2.5 15134500.0 cm-1
2s1 2p5 3p1 4P0.5 15176900.0 cm-1
2s1 2p5 3p1 2P1.5 15197500.0 cm-1
2s1 2p5 3p1 2S0.5 15212500.0 cm-1
2s1 2p5 3p1 2D2.5 15283800.0 cm-1
2s1 2p5 3p1 2D1.5 15290400.0 cm-1
2s1 2p5 3s1 2P1.5 15295300.0 cm-1
2s1 2p5 3s1 2P0.5 15326700.0 cm-1
2s1 2p5 3p1 4D0.5 15346900.0 cm-1
2s1 2p5 3p1 2P0.5 15454200.0 cm-1
2s1 2p5 3p1 4P1.5 15507800.0 cm-1
2s1 2p5 3d1 4P0.5 15523400.0 cm-1
2s1 2p5 3d1 4P1.5 15544700.0 cm-1
2s1 2p5 3d1 4F4.5 15570100.0 cm-1
2s1 2p5 3d1 4D2.5 15573700.0 cm-1
2s1 2p5 3d1 4F3.5 15576000.0 cm-1
2s1 2p5 3d1 4F2.5 15627800.0 cm-1
2s1 2p5 3d1 2F3.5 15640800.0 cm-1
2s1 2p5 3p1 2D1.5 15664800.0 cm-1
2s1 2p5 3d1 2D1.5 15665500.0 cm-1
2s1 2p5 3d1 4D0.5 15734300.0 cm-1
2s1 2p5 3p1 2P0.5 15745600.0 cm-1
2s1 2p5 3p1 2D2.5 15758800.0 cm-1
2s1 2p5 3d1 2D2.5 15766200.0 cm-1
2s1 2p5 3p1 2P1.5 15776400.0 cm-1
2s1 2p5 3d1 4D1.5 15777800.0 cm-1
2s1 2p5 3d1 2P0.5 15779100.0 cm-1
2s1 2p5 3d1 4D3.5 15787600.0 cm-1
2s1 2p5 3d1 2F2.5 15787700.0 cm-1
2s1 2p5 3p1 2S0.5 15799800.0 cm-1
2s1 2p5 3d1 4F1.5 15844900.0 cm-1
2s1 2p5 3d1 4P2.5 16006200.0 cm-1
2s1 2p5 3d1 2P1.5 16024300.0 cm-1
2s1 2p5 3d1 2F2.5 16228100.0 cm-1
2s1 2p5 3d1 2F3.5 16245000.0 cm-1
2s1 2p5 3d1 2P1.5 16270100.0 cm-1
2s1 2p5 3d1 2D2.5 16286700.0 cm-1
2s1 2p5 3d1 2D1.5 16288100.0 cm-1
2s1 2p5 3d1 2P0.5 16297300.0 cm-1
2s2 2p4 4s1 4P2.5 17696400.0 cm-1
2s2 2p4 4s1 2P1.5 17708000.0 cm-1
2s2 2p4 4p1 4P1.5 17851700.0 cm-1
2s2 2p4 4p1 4P2.5 17855500.0 cm-1
2s2 2p4 4s1 4P0.5 17861900.0 cm-1
2s2 2p4 4p1 2D2.5 17888500.0 cm-1
2s2 2p4 4p1 4D3.5 17889400.0 cm-1
2s2 2p4 4p1 2S0.5 17892200.0 cm-1
2s2 2p4 4p1 2P1.5 17937800.0 cm-1
2s2 2p4 4p1 4D0.5 18016600.0 cm-1
2s2 2p4 4s1 4P1.5 18053100.0 cm-1
2s2 2p4 4p1 4S1.5 18059800.0 cm-1
2s2 2p4 4s1 2P0.5 18061600.0 cm-1
2s2 2p4 4d1 4D2.5 18066200.0 cm-1
2s2 2p4 4d1 4D1.5 18066500.0 cm-1
2s2 2p4 4d1 4D3.5 18070500.0 cm-1
2s2 2p4 4d1 4P0.5 18071200.0 cm-1
2s2 2p4 4d1 4F4.5 18080200.0 cm-1
2s2 2p4 4d1 2F3.5 18080800.0 cm-1
2s2 2p4 4d1 2P0.5 18099400.0 cm-1
2s2 2p4 4d1 2D1.5 18118000.0 cm-1
2s2 2p4 4d1 2D2.5 18121600.0 cm-1
2s2 2p4 4s1 2D2.5 18162500.0 cm-1
2s2 2p4 4s1 2D1.5 18164300.0 cm-1
2s2 2p4 4f1 4F3.5 18184300.0 cm-1
2s2 2p4 4f1 4F2.5 18184500.0 cm-1
2s2 2p4 4f1 4F4.5 18186100.0 cm-1
2s2 2p4 4f1 4D1.5 18186700.0 cm-1
2s2 2p4 4f1 2G4.5 18188800.0 cm-1
2s2 2p4 4f1 4D0.5 18189500.0 cm-1
2s2 2p4 4f1 4G5.5 18190700.0 cm-1
2s2 2p4 4f1 2F3.5 18192500.0 cm-1
2s2 2p4 4f1 2F2.5 18195000.0 cm-1
2s2 2p4 4f1 2D1.5 18195800.0 cm-1
2s2 2p4 4p1 4P0.5 18205000.0 cm-1
2s2 2p4 4p1 4D1.5 18221800.0 cm-1
2s2 2p4 4d1 4F1.5 18236000.0 cm-1
2s2 2p4 4p1 4D2.5 18243800.0 cm-1
2s2 2p4 4p1 2D1.5 18253100.0 cm-1
2s2 2p4 4d1 4P2.5 18253400.0 cm-1
2s2 2p4 4p1 2P0.5 18262000.0 cm-1
2s2 2p4 4p1 2F2.5 18315300.0 cm-1
2s2 2p4 4p1 2P1.5 18339600.0 cm-1
2s2 2p4 4f1 4G2.5 18347500.0 cm-1
2s2 2p4 4p1 2F3.5 18350100.0 cm-1
2s2 2p4 4f1 2G3.5 18353000.0 cm-1
2s2 2p4 4p1 2D1.5 18353500.0 cm-1
2s2 2p4 4p1 2D2.5 18361800.0 cm-1
2s2 2p4 4p1 2P0.5 18397000.0 cm-1
2s2 2p4 4d1 4D0.5 18417500.0 cm-1
2s2 2p4 4d1 4P1.5 18430300.0 cm-1
2s2 2p4 4d1 4F3.5 18433000.0 cm-1
2s2 2p4 4d1 4F2.5 18442200.0 cm-1
2s2 2p4 4d1 2F2.5 18446300.0 cm-1
2s2 2p4 4d1 2P1.5 18460500.0 cm-1
2s2 2p4 4d1 2G3.5 18529300.0 cm-1
2s2 2p4 4f1 4F1.5 18538100.0 cm-1
2s2 2p4 4d1 2G4.5 18538700.0 cm-1
2s2 2p4 4f1 4G3.5 18541200.0 cm-1
2s2 2p4 4f1 4D2.5 18543500.0 cm-1
2s2 2p4 4d1 2S0.5 18543700.0 cm-1
2s2 2p4 4f1 4G4.5 18544100.0 cm-1
2s2 2p4 4d1 2D2.5 18547600.0 cm-1
2s2 2p4 4d1 2P1.5 18547700.0 cm-1
2s2 2p4 4f1 2D2.5 18548300.0 cm-1
2s2 2p4 4f1 4D3.5 18550700.0 cm-1
2s2 2p4 4d1 2F2.5 18551800.0 cm-1
2s2 2p4 4d1 2F3.5 18554900.0 cm-1
2s2 2p4 4d1 2D1.5 18576000.0 cm-1
2s2 2p4 4d1 2P0.5 18582700.0 cm-1
2s2 2p4 4s1 2S0.5 18614500.0 cm-1
2s2 2p4 4f1 2P0.5 18641500.0 cm-1
2s2 2p4 4f1 2H4.5 18642700.0 cm-1
2s2 2p4 4f1 2P1.5 18644500.0 cm-1
2s2 2p4 4f1 2H5.5 18647300.0 cm-1
2s2 2p4 4f1 2D2.5 18650200.0 cm-1
2s2 2p4 4f1 2D1.5 18651300.0 cm-1
2s2 2p4 4f1 2G3.5 18653100.0 cm-1
2s2 2p4 4f1 2F2.5 18655300.0 cm-1
2s2 2p4 4f1 2F3.5 18657000.0 cm-1
2s2 2p4 4f1 2G4.5 18657900.0 cm-1
2s2 2p4 4p1 2P0.5 18779400.0 cm-1
2s2 2p4 4p1 2P1.5 18801700.0 cm-1
2s2 2p4 4d1 2D2.5 18992900.0 cm-1
2s2 2p4 4d1 2D1.5 18998400.0 cm-1
2s2 2p4 4f1 2F2.5 19096000.0 cm-1
2s2 2p4 4f1 2F3.5 19100100.0 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

     Calculation details

 The following scaling parameters on bound orbitals were used:

         1S = 1.4045
         2S = 1.2143
         2P = 1.1492
         3S = 1.1389
         3P = 1.0890
         3D = 1.1252
         4S = 1.1558
         4P = 1.1024
         4D = 1.1275
         4F = 1.1401

 An exchange calculation was performed up to J=12
 A non-exchange calculation was then performed up to J=40
 Followed by a top-up calculation to J -> infinity.

 30 continuum basis orbitals were used.

 A fine energy mesh of 0.000005 Z**2 Rydbergs (0.04598828 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (9.197656 eV) was used
 from the last threshold up to 0.881964 Z**2 Rydbergs (8112 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (9.197656 eV) was used
 from first threshold up to 0.881964 Z**2 Rydbergs (8112 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

      M C Witthoeft, A D Whiteford and N R Badnell
      J Phys B 40 2969-2993 (2007)
      DOI: 10.1088/0953-4075/40/15/001

 Produced by: Mike Witthoeft
 Date:        18/07/06

 Update: Allan Whiteford, 14/03/08 
         Added Journal reference
         Removed incomplete comment about basis orbitals
         Added parent specification



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