Resolved Specific Ion Data Collections

Temperature Range
16.54 eV → 1.654 x 105 eV


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  • Spontaneous Emission: Br+30(i) → Br+30(j) + hv
  • Electron Impact Excitation: Br+30(i) + e → Br+30(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 424712.0 cm-1
2s1 2p2 4P0.5 653231.0 cm-1
2s1 2p2 4P1.5 916332.0 cm-1
2s1 2p2 4P2.5 1057430.0 cm-1
2s1 2p2 2D1.5 1328740.0 cm-1
2s1 2p2 2P0.5 1405590.0 cm-1
2s1 2p2 2D2.5 1521800.0 cm-1
2s1 2p2 2S0.5 1860660.0 cm-1
2s1 2p2 2P1.5 1876560.0 cm-1
2p3 4S1.5 2116710.0 cm-1
2p3 2D1.5 2441530.0 cm-1
2p3 2D2.5 2544900.0 cm-1
2p3 2P0.5 2732200.0 cm-1
2p3 2P1.5 3051190.0 cm-1
2s2 3s1 2S0.5 15929700.0 cm-1
2s2 3p1 2P0.5 16190300.0 cm-1
2s2 3p1 2P1.5 16306000.0 cm-1
2s1 2p1 3s1 4P0.5 16438500.0 cm-1
2s1 2p1 3s1 4P1.5 16517600.0 cm-1
2s2 3d1 2D1.5 16543800.0 cm-1
2s2 3d1 2D2.5 16582900.0 cm-1
2s1 2p1 3s1 2P0.5 16595000.0 cm-1
2s1 2p1 3p1 4D0.5 16666100.0 cm-1
2s1 2p1 3p1 4D1.5 16738600.0 cm-1
2s1 2p1 3p1 4S1.5 16829000.0 cm-1
2s1 2p1 3p1 4P0.5 16838800.0 cm-1
2s1 2p1 3s1 4P2.5 16850700.0 cm-1
2s1 2p1 3p1 2P0.5 16884600.0 cm-1
2s1 2p1 3p1 4D2.5 16893600.0 cm-1
2s1 2p1 3p1 2D1.5 16929200.0 cm-1
2s1 2p1 3s1 2P1.5 16943100.0 cm-1
2s1 2p1 3d1 4F1.5 17005300.0 cm-1
2s1 2p1 3d1 4F2.5 17061400.0 cm-1
2s1 2p1 3d1 4P2.5 17119600.0 cm-1
2s1 2p1 3p1 4P1.5 17137800.0 cm-1
2s1 2p1 3d1 4D1.5 17145000.0 cm-1
2s1 2p1 3d1 4F3.5 17148700.0 cm-1
2s1 2p1 3d1 4D0.5 17149800.0 cm-1
2s1 2p1 3p1 4P2.5 17161300.0 cm-1
2s1 2p1 3p1 4D3.5 17206200.0 cm-1
2s1 2p1 3d1 2D1.5 17216200.0 cm-1
2s1 2p1 3p1 2P1.5 17231500.0 cm-1
2s1 2p1 3s1 2P0.5 17232000.0 cm-1
2s1 2p1 3d1 2F2.5 17242200.0 cm-1
2s1 2p1 3s1 2P1.5 17250600.0 cm-1
2s1 2p1 3p1 2D2.5 17300400.0 cm-1
2s1 2p1 3p1 2S0.5 17322500.0 cm-1
2p2 3s1 4P0.5 17397000.0 cm-1
2s1 2p1 3d1 4F4.5 17439700.0 cm-1
2s1 2p1 3d1 4D3.5 17466900.0 cm-1
2s1 2p1 3d1 4D2.5 17467500.0 cm-1
2s1 2p1 3d1 4P1.5 17479900.0 cm-1
2s1 2p1 3d1 4P0.5 17482600.0 cm-1
2s1 2p1 3p1 2P0.5 17496400.0 cm-1
2s1 2p1 3p1 2D1.5 17503900.0 cm-1
2s1 2p1 3d1 2D2.5 17532200.0 cm-1
2s1 2p1 3d1 2P1.5 17573600.0 cm-1
2s1 2p1 3p1 2D2.5 17588600.0 cm-1
2p2 3p1 4D0.5 17610200.0 cm-1
2s1 2p1 3p1 2P1.5 17614600.0 cm-1
2s1 2p1 3d1 2F3.5 17620500.0 cm-1
2s1 2p1 3d1 2P0.5 17649800.0 cm-1
2s1 2p1 3p1 2S0.5 17667700.0 cm-1
2p2 3s1 4P1.5 17705200.0 cm-1
2p2 3s1 2P0.5 17767800.0 cm-1
2p2 3p1 4D1.5 17770500.0 cm-1
2p2 3s1 4P2.5 17797500.0 cm-1
2s1 2p1 3d1 2F2.5 17841700.0 cm-1
2p2 3s1 2D1.5 17844100.0 cm-1
2s1 2p1 3d1 2F3.5 17850600.0 cm-1
2s1 2p1 3d1 2D1.5 17852400.0 cm-1
2s1 2p1 3d1 2P0.5 17891900.0 cm-1
2s1 2p1 3d1 2D2.5 17898600.0 cm-1
2p2 3p1 2S0.5 17906500.0 cm-1
2s1 2p1 3d1 2P1.5 17928300.0 cm-1
2p2 3d1 4F1.5 17946200.0 cm-1
2p2 3p1 4P1.5 17947500.0 cm-1
2p2 3p1 4P2.5 18008600.0 cm-1
2p2 3d1 2F2.5 18025400.0 cm-1
2p2 3p1 4D2.5 18048900.0 cm-1
2p2 3p1 4P0.5 18068600.0 cm-1
2p2 3p1 2D1.5 18096200.0 cm-1
2p2 3p1 4D3.5 18136500.0 cm-1
2p2 3p1 4S1.5 18144900.0 cm-1
2p2 3p1 2P1.5 18186800.0 cm-1
2p2 3s1 2D2.5 18195100.0 cm-1
2p2 3p1 2F2.5 18223100.0 cm-1
2p2 3s1 2P1.5 18234600.0 cm-1
2p2 3d1 2P1.5 18253900.0 cm-1
2p2 3d1 4F2.5 18262100.0 cm-1
2p2 3d1 4D0.5 18264600.0 cm-1
2p2 3d1 4F3.5 18281500.0 cm-1
2p2 3p1 2P0.5 18293500.0 cm-1
2p2 3d1 4D3.5 18327800.0 cm-1
2p2 3d1 4P2.5 18342600.0 cm-1
2p2 3d1 4D1.5 18345300.0 cm-1
2p2 3d1 4F4.5 18366800.0 cm-1
2p2 3d1 4D2.5 18412700.0 cm-1
2p2 3d1 4P1.5 18429000.0 cm-1
2p2 3d1 4P0.5 18438200.0 cm-1
2p2 3s1 2S0.5 18471800.0 cm-1
2p2 3p1 2D1.5 18476300.0 cm-1
2p2 3d1 2G3.5 18479000.0 cm-1
2p2 3d1 2D2.5 18486800.0 cm-1
2p2 3d1 2D1.5 18498900.0 cm-1
2p2 3p1 2D2.5 18504800.0 cm-1
2p2 3d1 2P0.5 18512100.0 cm-1
2p2 3p1 2D2.5 18521600.0 cm-1
2p2 3p1 2F3.5 18533500.0 cm-1
2p2 3p1 2P0.5 18542700.0 cm-1
2p2 3p1 2P1.5 18714500.0 cm-1
2p2 3d1 2F3.5 18750000.0 cm-1
2p2 3p1 2P0.5 18753500.0 cm-1
2p2 3d1 2G4.5 18769700.0 cm-1
2p2 3d1 2D1.5 18785700.0 cm-1
2p2 3d1 2D2.5 18790800.0 cm-1
2p2 3d1 2P0.5 18792000.0 cm-1
2p2 3d1 2F3.5 18826500.0 cm-1
2p2 3p1 2P1.5 18845000.0 cm-1
2p2 3d1 2S0.5 18875600.0 cm-1
2p2 3d1 2P1.5 18910000.0 cm-1
2p2 3d1 2F2.5 18923800.0 cm-1
2p2 3d1 2D1.5 19091900.0 cm-1
2p2 3d1 2D2.5 19092300.0 cm-1
2s2 4s1 2S0.5 21570900.0 cm-1
2s2 4p1 2P0.5 21679700.0 cm-1
2s2 4p1 2P1.5 21726900.0 cm-1
2s2 4d1 2D1.5 21815200.0 cm-1
2s2 4d1 2D2.5 21831000.0 cm-1
2s2 4f1 2F2.5 21884000.0 cm-1
2s2 4f1 2F3.5 21891600.0 cm-1
2s1 2p1 4s1 4P0.5 22067200.0 cm-1
2s1 2p1 4s1 4P1.5 22141000.0 cm-1
2s1 2p1 4p1 4D0.5 22163100.0 cm-1
2s1 2p1 4s1 2P0.5 22168600.0 cm-1
2s1 2p1 4p1 4D1.5 22220900.0 cm-1
2s1 2p1 4p1 4S1.5 22239200.0 cm-1
2s1 2p1 4p1 4P0.5 22269200.0 cm-1
2s1 2p1 4d1 4F1.5 22296100.0 cm-1
2s1 2p1 4p1 4D2.5 22298000.0 cm-1
2s1 2p1 4p1 2P0.5 22300100.0 cm-1
2s1 2p1 4p1 2D1.5 22309800.0 cm-1
2s1 2p1 4d1 4P2.5 22322800.0 cm-1
2s1 2p1 4f1 4G2.5 22368500.0 cm-1
2s1 2p1 4d1 4F2.5 22371400.0 cm-1
2s1 2p1 4f1 4D3.5 22376900.0 cm-1
2s1 2p1 4d1 4D1.5 22386700.0 cm-1
2s1 2p1 4d1 4D0.5 22391300.0 cm-1
2s1 2p1 4d1 4F3.5 22396500.0 cm-1
2s1 2p1 4d1 2D1.5 22415500.0 cm-1
2s1 2p1 4d1 2F2.5 22420800.0 cm-1
2s1 2p1 4f1 4F1.5 22444800.0 cm-1
2s1 2p1 4f1 4G3.5 22446000.0 cm-1
2s1 2p1 4f1 4D2.5 22448900.0 cm-1
2s1 2p1 4f1 4F4.5 22452800.0 cm-1
2s1 2p1 4f1 2D2.5 22457600.0 cm-1
2s1 2p1 4f1 2G3.5 22460600.0 cm-1
2s1 2p1 4s1 4P2.5 22481400.0 cm-1
2s1 2p1 4s1 2P1.5 22512200.0 cm-1
2s1 2p1 4p1 4P1.5 22595500.0 cm-1
2s1 2p1 4p1 4P2.5 22601300.0 cm-1
2s1 2p1 4p1 4D3.5 22626500.0 cm-1
2s1 2p1 4p1 2P1.5 22638700.0 cm-1
2s1 2p1 4p1 2D2.5 22659400.0 cm-1
2s1 2p1 4p1 2S0.5 22672500.0 cm-1
2s1 2p1 4d1 4F4.5 22719900.0 cm-1
2s1 2p1 4d1 4D3.5 22724600.0 cm-1
2s1 2p1 4d1 4D2.5 22724600.0 cm-1
2s1 2p1 4d1 4P1.5 22729200.0 cm-1
2s1 2p1 4d1 4P0.5 22730600.0 cm-1
2s1 2p1 4d1 2D2.5 22750300.0 cm-1
2s1 2p1 4d1 2P1.5 22763400.0 cm-1
2s1 2p1 4d1 2F3.5 22774900.0 cm-1
2s1 2p1 4d1 2P0.5 22786100.0 cm-1
2s1 2p1 4f1 4F3.5 22786500.0 cm-1
2s1 2p1 4f1 4F2.5 22789100.0 cm-1
2s1 2p1 4f1 4G4.5 22790200.0 cm-1
2s1 2p1 4f1 4D1.5 22794800.0 cm-1
2s1 2p1 4f1 2F3.5 22797500.0 cm-1
2s1 2p1 4f1 4G5.5 22798500.0 cm-1
2s1 2p1 4f1 4D0.5 22799400.0 cm-1
2s1 2p1 4f1 2G4.5 22802100.0 cm-1
2s1 2p1 4f1 2F2.5 22804200.0 cm-1
2s1 2p1 4f1 2D1.5 22813200.0 cm-1
2s1 2p1 4s1 2P0.5 22846100.0 cm-1
2s1 2p1 4s1 2P1.5 22850200.0 cm-1
2s1 2p1 4p1 2P0.5 22953500.0 cm-1
2s1 2p1 4p1 2D1.5 22953800.0 cm-1
2s1 2p1 4p1 2D2.5 22969600.0 cm-1
2s1 2p1 4p1 2P1.5 22991600.0 cm-1
2s1 2p1 4p1 2S0.5 23003000.0 cm-1
2s1 2p1 4d1 2D1.5 23058600.0 cm-1
2s1 2p1 4d1 2F2.5 23084500.0 cm-1
2s1 2p1 4d1 2F3.5 23087500.0 cm-1
2s1 2p1 4d1 2D2.5 23093600.0 cm-1
2s1 2p1 4d1 2P0.5 23103700.0 cm-1
2s1 2p1 4d1 2P1.5 23111700.0 cm-1
2s1 2p1 4f1 2F2.5 23138900.0 cm-1
2s1 2p1 4f1 2F3.5 23146200.0 cm-1
2s1 2p1 4f1 2G3.5 23152400.0 cm-1
2s1 2p1 4f1 2G4.5 23159100.0 cm-1
2s1 2p1 4f1 2D1.5 23159400.0 cm-1
2s1 2p1 4f1 2D2.5 23166700.0 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 = 1.37597
         2S = 1.25318
         2P = 1.17656
         3S = 1.57226
         3P = 1.37829
         3D = 1.49035
         4S = 1.50894
         4P = 1.39015
         4D = 1.53934
         4F = 1.61280

 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.

 40 continuum basis orbitals were used, giving a smallest maximum
 basis-orbital energy of 3044.9876 Rydbergs (41430.101286 eV)

 A fine energy mesh of 0.000001 Z**2 Rydbergs (0.0122454 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (12.2454 eV) was used
 from the last threshold up to 0.835171 Z**2 Rydbergs (10227 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (12.2454 eV) was used
 from first threshold up to 0.835171 Z**2 Rydbergs (10227 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

      G Y Liang, N R Badnell and G Zhao
      A&A 547, A87 (2012)
      DOI: 10.1051/0004-6361/201220277

 Produced by: Guiyun Liang
 Date:        09/08/12


  • Guiyun Liang
  • Nigel Badnell
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