Resolved Specific Ion Data Collections

Temperature Range
13.53 eV → 1.353 x 105 eV


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  • Spontaneous Emission: Kr+27(i) → Kr+27(j) + hv
  • Electron Impact Excitation: Kr+27(i) + e → Kr+27(j) + e
2s2 2p5 2P1.5 0.0 cm-1
2s2 2p5 2P0.5 446416.0 cm-1
2s1 2p6 2S0.5 1903390.0 cm-1
2s2 2p4 3s1 4P2.5 13945200.0 cm-1
2s2 2p4 3s1 2P1.5 13985200.0 cm-1
2s2 2p4 3s1 4P0.5 14129000.0 cm-1
2s2 2p4 3p1 4P1.5 14331600.0 cm-1
2s2 2p4 3p1 4P2.5 14350000.0 cm-1
2s2 2p4 3s1 4P1.5 14355200.0 cm-1
2s2 2p4 3s1 2P0.5 14387800.0 cm-1
2s2 2p4 3p1 2P0.5 14438800.0 cm-1
2s2 2p4 3p1 2D2.5 14447400.0 cm-1
2s2 2p4 3p1 4D3.5 14454400.0 cm-1
2s2 2p4 3s1 2D2.5 14469700.0 cm-1
2s2 2p4 3s1 2D1.5 14482200.0 cm-1
2s2 2p4 3p1 4D0.5 14530000.0 cm-1
2s2 2p4 3p1 4S1.5 14582500.0 cm-1
2s2 2p4 3p1 4D1.5 14645800.0 cm-1
2s2 2p4 3p1 4P0.5 14732300.0 cm-1
2s2 2p4 3p1 2D1.5 14775300.0 cm-1
2s2 2p4 3p1 4D2.5 14851800.0 cm-1
2s2 2p4 3p1 2F2.5 14860900.0 cm-1
2s2 2p4 3p1 2S0.5 14879100.0 cm-1
2s2 2p4 3p1 2D1.5 14883100.0 cm-1
2s2 2p4 3d1 4D1.5 14933600.0 cm-1
2s2 2p4 3d1 4D2.5 14934300.0 cm-1
2s2 2p4 3d1 2P0.5 14949300.0 cm-1
2s2 2p4 3d1 4D3.5 14949900.0 cm-1
2s2 2p4 3p1 2F3.5 14965700.0 cm-1
2s2 2p4 3p1 2P1.5 14966800.0 cm-1
2s2 2p4 3s1 2S0.5 14970200.0 cm-1
2s2 2p4 3d1 4F4.5 14982200.0 cm-1
2s2 2p4 3d1 2F3.5 14982900.0 cm-1
2s2 2p4 3p1 2P1.5 14994700.0 cm-1
2s2 2p4 3p1 2D2.5 15001300.0 cm-1
2s2 2p4 3d1 4P0.5 15027900.0 cm-1
2s2 2p4 3d1 4P1.5 15063100.0 cm-1
2s2 2p4 3d1 2D2.5 15093100.0 cm-1
2s2 2p4 3p1 2P0.5 15131100.0 cm-1
2s2 2p4 3d1 4F1.5 15148600.0 cm-1
2s2 2p4 3d1 4P2.5 15182800.0 cm-1
2s2 2p4 3d1 4D0.5 15321000.0 cm-1
2s2 2p4 3d1 2D1.5 15358800.0 cm-1
2s2 2p4 3d1 4F3.5 15375600.0 cm-1
2s2 2p4 3d1 4F2.5 15403200.0 cm-1
2s2 2p4 3d1 2F2.5 15418300.0 cm-1
2s2 2p4 3d1 2P1.5 15427800.0 cm-1
2s2 2p4 3p1 2P0.5 15433400.0 cm-1
2s2 2p4 3d1 2G3.5 15460500.0 cm-1
2s2 2p4 3p1 2P1.5 15472800.0 cm-1
2s2 2p4 3d1 2G4.5 15486800.0 cm-1
2s2 2p4 3d1 2S0.5 15506100.0 cm-1
2s2 2p4 3d1 2D2.5 15510800.0 cm-1
2s2 2p4 3d1 2P1.5 15533400.0 cm-1
2s2 2p4 3d1 2F3.5 15537400.0 cm-1
2s2 2p4 3d1 2F2.5 15544600.0 cm-1
2s2 2p4 3d1 2D1.5 15616600.0 cm-1
2s1 2p5 3s1 4P2.5 15624500.0 cm-1
2s2 2p4 3d1 2P0.5 15640900.0 cm-1
2s1 2p5 3s1 2P1.5 15695600.0 cm-1
2s1 2p5 3s1 4P1.5 15850100.0 cm-1
2s1 2p5 3s1 2P0.5 15851600.0 cm-1
2s2 2p4 3d1 2D2.5 16003800.0 cm-1
2s1 2p5 3p1 4S1.5 16008000.0 cm-1
2s2 2p4 3d1 2D1.5 16031000.0 cm-1
2s1 2p5 3p1 4D2.5 16037400.0 cm-1
2s1 2p5 3s1 4P0.5 16101400.0 cm-1
2s1 2p5 3p1 4D3.5 16118500.0 cm-1
2s1 2p5 3p1 4D1.5 16139400.0 cm-1
2s1 2p5 3p1 4P2.5 16162500.0 cm-1
2s1 2p5 3p1 4P0.5 16206600.0 cm-1
2s1 2p5 3p1 2P1.5 16226300.0 cm-1
2s1 2p5 3p1 2S0.5 16240800.0 cm-1
2s1 2p5 3p1 2D2.5 16324900.0 cm-1
2s1 2p5 3p1 2D1.5 16332100.0 cm-1
2s1 2p5 3s1 2P1.5 16344700.0 cm-1
2s1 2p5 3s1 2P0.5 16380700.0 cm-1
2s1 2p5 3p1 4D0.5 16396300.0 cm-1
2s1 2p5 3p1 2P0.5 16515900.0 cm-1
2s1 2p5 3d1 4P0.5 16565900.0 cm-1
2s1 2p5 3p1 4P1.5 16586000.0 cm-1
2s1 2p5 3d1 4P1.5 16588600.0 cm-1
2s1 2p5 3d1 4F4.5 16617200.0 cm-1
2s1 2p5 3d1 4D2.5 16619100.0 cm-1
2s1 2p5 3d1 4F3.5 16621200.0 cm-1
2s1 2p5 3d1 4P2.5 16677400.0 cm-1
2s1 2p5 3d1 2F3.5 16690400.0 cm-1
2s1 2p5 3d1 2D1.5 16717400.0 cm-1
2s1 2p5 3p1 2D1.5 16728900.0 cm-1
2s1 2p5 3d1 4D0.5 16791600.0 cm-1
2s1 2p5 3p1 2P0.5 16819400.0 cm-1
2s1 2p5 3d1 2D2.5 16824700.0 cm-1
2s1 2p5 3d1 2P0.5 16833800.0 cm-1
2s1 2p5 3p1 2D2.5 16836300.0 cm-1
2s1 2p5 3d1 4D1.5 16836900.0 cm-1
2s1 2p5 3d1 4D3.5 16850200.0 cm-1
2s1 2p5 3d1 2F2.5 16851100.0 cm-1
2s1 2p5 3p1 2P1.5 16853800.0 cm-1
2s1 2p5 3p1 2S0.5 16872300.0 cm-1
2s1 2p5 3d1 4F1.5 16913700.0 cm-1
2s1 2p5 3d1 4F2.5 17105100.0 cm-1
2s1 2p5 3d1 2P1.5 17116700.0 cm-1
2s1 2p5 3d1 2F2.5 17322900.0 cm-1
2s1 2p5 3d1 2F3.5 17343100.0 cm-1
2s1 2p5 3d1 2P1.5 17368400.0 cm-1
2s1 2p5 3d1 2D2.5 17386500.0 cm-1
2s1 2p5 3d1 2D1.5 17387300.0 cm-1
2s1 2p5 3d1 2P0.5 17396300.0 cm-1
2s2 2p4 4s1 4P2.5 18935000.0 cm-1
2s2 2p4 4s1 2P1.5 18946900.0 cm-1
2s2 2p4 4p1 4P1.5 19096500.0 cm-1
2s2 2p4 4p1 2D2.5 19100500.0 cm-1
2s2 2p4 4s1 4P0.5 19108900.0 cm-1
2s2 2p4 4p1 4P2.5 19138300.0 cm-1
2s2 2p4 4p1 4D3.5 19139200.0 cm-1
2s2 2p4 4p1 2S0.5 19141800.0 cm-1
2s2 2p4 4p1 2P1.5 19189600.0 cm-1
2s2 2p4 4p1 4D0.5 19269700.0 cm-1
2s2 2p4 4p1 4S1.5 19318400.0 cm-1
2s2 2p4 4d1 4D1.5 19322900.0 cm-1
2s2 2p4 4d1 4D2.5 19323100.0 cm-1
2s2 2p4 4d1 4P0.5 19327700.0 cm-1
2s2 2p4 4d1 4D3.5 19327900.0 cm-1
2s2 2p4 4d1 4F4.5 19338400.0 cm-1
2s2 2p4 4d1 2F3.5 19338500.0 cm-1
2s2 2p4 4s1 4P1.5 19340700.0 cm-1
2s2 2p4 4s1 2P0.5 19347500.0 cm-1
2s2 2p4 4d1 2P0.5 19360500.0 cm-1
2s2 2p4 4d1 2D1.5 19378200.0 cm-1
2s2 2p4 4d1 2D2.5 19382200.0 cm-1
2s2 2p4 4f1 4F3.5 19447200.0 cm-1
2s2 2p4 4f1 4F2.5 19447300.0 cm-1
2s2 2p4 4f1 4F4.5 19449100.0 cm-1
2s2 2p4 4f1 4D1.5 19449500.0 cm-1
2s2 2p4 4s1 2D2.5 19452300.0 cm-1
2s2 2p4 4f1 2G4.5 19452300.0 cm-1
2s2 2p4 4f1 4D0.5 19452400.0 cm-1
2s2 2p4 4f1 4G5.5 19454200.0 cm-1
2s2 2p4 4s1 2D1.5 19455000.0 cm-1
2s2 2p4 4f1 2F3.5 19456300.0 cm-1
2s2 2p4 4f1 2F2.5 19458800.0 cm-1
2s2 2p4 4f1 2D1.5 19459400.0 cm-1
2s2 2p4 4p1 4P0.5 19498900.0 cm-1
2s2 2p4 4d1 4F1.5 19501200.0 cm-1
2s2 2p4 4p1 4D1.5 19516100.0 cm-1
2s2 2p4 4d1 4P2.5 19520700.0 cm-1
2s2 2p4 4p1 4D2.5 19542800.0 cm-1
2s2 2p4 4p1 2D1.5 19552300.0 cm-1
2s2 2p4 4p1 2P0.5 19561500.0 cm-1
2s2 2p4 4p1 2F2.5 19611900.0 cm-1
2s2 2p4 4f1 4G2.5 19618800.0 cm-1
2s2 2p4 4f1 2G3.5 19624900.0 cm-1
2s2 2p4 4p1 2P1.5 19637300.0 cm-1
2s2 2p4 4p1 2F3.5 19651800.0 cm-1
2s2 2p4 4p1 2D1.5 19654900.0 cm-1
2s2 2p4 4p1 2D2.5 19663700.0 cm-1
2s2 2p4 4p1 2P0.5 19700400.0 cm-1
2s2 2p4 4d1 4D0.5 19723000.0 cm-1
2s2 2p4 4d1 4P1.5 19736400.0 cm-1
2s2 2p4 4d1 4F3.5 19740300.0 cm-1
2s2 2p4 4d1 4F2.5 19748700.0 cm-1
2s2 2p4 4d1 2F2.5 19753900.0 cm-1
2s2 2p4 4d1 2P1.5 19768600.0 cm-1
2s2 2p4 4d1 2G3.5 19837800.0 cm-1
2s2 2p4 4d1 2G4.5 19848700.0 cm-1
2s2 2p4 4f1 4F1.5 19849900.0 cm-1
2s2 2p4 4d1 2S0.5 19853000.0 cm-1
2s2 2p4 4f1 4G3.5 19853300.0 cm-1
2s2 2p4 4f1 4D2.5 19855900.0 cm-1
2s2 2p4 4f1 4G4.5 19856900.0 cm-1
2s2 2p4 4d1 2P1.5 19857000.0 cm-1
2s2 2p4 4d1 2D2.5 19857700.0 cm-1
2s2 2p4 4f1 2D2.5 19861000.0 cm-1
2s2 2p4 4d1 2F2.5 19861000.0 cm-1
2s2 2p4 4f1 4D3.5 19863700.0 cm-1
2s2 2p4 4d1 2F3.5 19865400.0 cm-1
2s2 2p4 4d1 2D1.5 19887100.0 cm-1
2s2 2p4 4d1 2P0.5 19896200.0 cm-1
2s2 2p4 4s1 2S0.5 19953300.0 cm-1
2s2 2p4 4f1 2P0.5 19956000.0 cm-1
2s2 2p4 4f1 2H4.5 19957300.0 cm-1
2s2 2p4 4f1 2P1.5 19959300.0 cm-1
2s2 2p4 4f1 2H5.5 19962600.0 cm-1
2s2 2p4 4f1 2D2.5 19965200.0 cm-1
2s2 2p4 4f1 2D1.5 19966600.0 cm-1
2s2 2p4 4f1 2G3.5 19968000.0 cm-1
2s2 2p4 4f1 2F2.5 19970600.0 cm-1
2s2 2p4 4f1 2F3.5 19972600.0 cm-1
2s2 2p4 4f1 2G4.5 19973600.0 cm-1
2s2 2p4 4p1 2P0.5 20126700.0 cm-1
2s2 2p4 4p1 2P1.5 20153400.0 cm-1
2s2 2p4 4d1 2D2.5 20353000.0 cm-1
2s2 2p4 4d1 2D1.5 20357600.0 cm-1
2s2 2p4 4f1 2F2.5 20460800.0 cm-1
2s2 2p4 4f1 2F3.5 20465400.0 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 = 1.4038
         2S = 1.2148
         2P = 1.1496
         3S = 1.1395
         3P = 1.0897
         3D = 1.1259
         4S = 1.1565
         4P = 1.1031
         4D = 1.1283
         4F = 1.1413

 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 (0.04959387 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (9.918774 eV) was used
 from the last threshold up to 0.928436 Z**2 Rydbergs (9208.94673 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (9.918774 eV) was used
 from first threshold up to 0.928436 Z**2 Rydbergs (9208.94673 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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