Resolved Specific Ion Data Collections

Temperature Range
7.600 eV → 7.600 x 104 eV


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  • Spontaneous Emission: Mn+20(i) → Mn+20(j) + hv
  • Electron Impact Excitation: Mn+20(i) + e → Mn+20(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 118266.0 cm-1
2s1 2p2 4P0.5 404551.0 cm-1
2s1 2p2 4P1.5 460190.0 cm-1
2s1 2p2 4P2.5 513260.0 cm-1
2s1 2p2 2D1.5 736310.0 cm-1
2s1 2p2 2D2.5 759210.0 cm-1
2s1 2p2 2P0.5 853671.0 cm-1
2s1 2p2 2S0.5 978328.0 cm-1
2s1 2p2 2P1.5 992320.0 cm-1
2p3 4S1.5 1255700.0 cm-1
2p3 2D1.5 1396110.0 cm-1
2p3 2D2.5 1426570.0 cm-1
2p3 2P0.5 1569630.0 cm-1
2p3 2P1.5 1627720.0 cm-1
2s2 3s1 2S0.5 7426170.0 cm-1
2s2 3p1 2P0.5 7598030.0 cm-1
2s2 3p1 2P1.5 7625410.0 cm-1
2s1 2p1 3s1 4P0.5 7768250.0 cm-1
2s2 3d1 2D1.5 7785750.0 cm-1
2s2 3d1 2D2.5 7794510.0 cm-1
2s1 2p1 3s1 4P1.5 7794810.0 cm-1
2s1 2p1 3s1 4P2.5 7861070.0 cm-1
2s1 2p1 3s1 2P0.5 7861340.0 cm-1
2s1 2p1 3p1 4D0.5 7920750.0 cm-1
2s1 2p1 3s1 2P1.5 7932430.0 cm-1
2s1 2p1 3p1 4D1.5 7944360.0 cm-1
2s1 2p1 3p1 2P1.5 7976160.0 cm-1
2s1 2p1 3p1 2P0.5 7981890.0 cm-1
2s1 2p1 3p1 4D2.5 7985800.0 cm-1
2s1 2p1 3p1 4P0.5 8008260.0 cm-1
2s1 2p1 3p1 4S1.5 8023410.0 cm-1
2s1 2p1 3p1 4D3.5 8045350.0 cm-1
2s1 2p1 3p1 4P1.5 8056350.0 cm-1
2s1 2p1 3p1 4P2.5 8071880.0 cm-1
2s1 2p1 3p1 2D1.5 8072130.0 cm-1
2s1 2p1 3d1 4F1.5 8090260.0 cm-1
2s1 2p1 3d1 4F2.5 8107220.0 cm-1
2s1 2p1 3p1 2D2.5 8114630.0 cm-1
2s1 2p1 3d1 4F3.5 8133820.0 cm-1
2s1 2p1 3p1 2S0.5 8146570.0 cm-1
2s1 2p1 3d1 4P2.5 8148540.0 cm-1
2s1 2p1 3s1 2P0.5 8154320.0 cm-1
2s1 2p1 3s1 2P1.5 8155340.0 cm-1
2s1 2p1 3d1 4D1.5 8157730.0 cm-1
2s1 2p1 3d1 4D0.5 8159520.0 cm-1
2s1 2p1 3d1 4F4.5 8185820.0 cm-1
2s1 2p1 3d1 2D1.5 8186940.0 cm-1
2s1 2p1 3d1 2D2.5 8200830.0 cm-1
2s1 2p1 3d1 4D3.5 8216350.0 cm-1
2s1 2p1 3d1 4D2.5 8227110.0 cm-1
2s1 2p1 3d1 4P1.5 8230420.0 cm-1
2s1 2p1 3d1 4P0.5 8232240.0 cm-1
2s1 2p1 3d1 2F2.5 8268230.0 cm-1
2s1 2p1 3d1 2P1.5 8302910.0 cm-1
2s1 2p1 3d1 2F3.5 8318430.0 cm-1
2s1 2p1 3p1 2P0.5 8324960.0 cm-1
2s1 2p1 3p1 2D1.5 8331000.0 cm-1
2s1 2p1 3d1 2P0.5 8332470.0 cm-1
2s1 2p1 3p1 2D2.5 8347660.0 cm-1
2s1 2p1 3p1 2P1.5 8354150.0 cm-1
2s1 2p1 3p1 2S0.5 8377000.0 cm-1
2p2 3s1 4P0.5 8403880.0 cm-1
2p2 3s1 4P1.5 8436340.0 cm-1
2p2 3s1 4P2.5 8478160.0 cm-1
2p2 3s1 2P0.5 8501800.0 cm-1
2s1 2p1 3d1 2F3.5 8502660.0 cm-1
2s1 2p1 3d1 2F2.5 8504140.0 cm-1
2s1 2p1 3d1 2D1.5 8515590.0 cm-1
2p2 3p1 4D0.5 8522360.0 cm-1
2s1 2p1 3d1 2D2.5 8526910.0 cm-1
2p2 3s1 2P1.5 8537350.0 cm-1
2s1 2p1 3d1 2P0.5 8549250.0 cm-1
2s1 2p1 3d1 2P1.5 8551490.0 cm-1
2p2 3p1 4D1.5 8566580.0 cm-1
2p2 3p1 2S0.5 8567330.0 cm-1
2p2 3p1 4P1.5 8603360.0 cm-1
2p2 3p1 4D2.5 8606660.0 cm-1
2p2 3s1 2D2.5 8610950.0 cm-1
2p2 3p1 4P0.5 8621580.0 cm-1
2p2 3s1 2D1.5 8626290.0 cm-1
2p2 3p1 4P2.5 8629220.0 cm-1
2p2 3p1 2D1.5 8641860.0 cm-1
2p2 3p1 4D3.5 8647990.0 cm-1
2p2 3d1 4F1.5 8689990.0 cm-1
2p2 3p1 2P1.5 8696060.0 cm-1
2p2 3p1 2D2.5 8700700.0 cm-1
2p2 3p1 4S1.5 8706220.0 cm-1
2p2 3d1 4F2.5 8710930.0 cm-1
2p2 3p1 2P0.5 8727460.0 cm-1
2p2 3d1 4F3.5 8747060.0 cm-1
2p2 3d1 2P1.5 8750270.0 cm-1
2p2 3d1 4D0.5 8756640.0 cm-1
2p2 3d1 4D2.5 8758000.0 cm-1
2p2 3p1 2F2.5 8767490.0 cm-1
2p2 3d1 4F4.5 8781900.0 cm-1
2p2 3d1 4D3.5 8782250.0 cm-1
2p2 3p1 2F3.5 8782440.0 cm-1
2p2 3d1 4D1.5 8785290.0 cm-1
2p2 3d1 2F2.5 8788480.0 cm-1
2p2 3p1 2D1.5 8808140.0 cm-1
2p2 3s1 2S0.5 8819270.0 cm-1
2p2 3p1 2D2.5 8821600.0 cm-1
2p2 3d1 4P2.5 8828030.0 cm-1
2p2 3p1 2P0.5 8837520.0 cm-1
2p2 3d1 2P0.5 8838170.0 cm-1
2p2 3d1 4P1.5 8840640.0 cm-1
2p2 3d1 4P0.5 8848900.0 cm-1
2p2 3d1 2F3.5 8850890.0 cm-1
2p2 3p1 2P1.5 8895740.0 cm-1
2p2 3d1 2D2.5 8897540.0 cm-1
2p2 3d1 2D1.5 8899430.0 cm-1
2p2 3d1 2G3.5 8905530.0 cm-1
2p2 3d1 2G4.5 8920670.0 cm-1
2p2 3d1 2D1.5 8946090.0 cm-1
2p2 3d1 2D2.5 8953300.0 cm-1
2p2 3d1 2F3.5 8976180.0 cm-1
2p2 3d1 2P0.5 8978690.0 cm-1
2p2 3p1 2P0.5 8998050.0 cm-1
2p2 3d1 2F2.5 9007640.0 cm-1
2p2 3d1 2S0.5 9012430.0 cm-1
2p2 3p1 2P1.5 9013190.0 cm-1
2p2 3d1 2P1.5 9013700.0 cm-1
2p2 3d1 2D2.5 9158790.0 cm-1
2p2 3d1 2D1.5 9166460.0 cm-1
2s2 4s1 2S0.5 10069500.0 cm-1
2s2 4p1 2P0.5 10140300.0 cm-1
2s2 4p1 2P1.5 10151500.0 cm-1
2s2 4d1 2D1.5 10210300.0 cm-1
2s2 4d1 2D2.5 10213900.0 cm-1
2s2 4f1 2F2.5 10248100.0 cm-1
2s2 4f1 2F3.5 10249800.0 cm-1
2s1 2p1 4s1 4P0.5 10407400.0 cm-1
2s1 2p1 4s1 4P1.5 10432100.0 cm-1
2s1 2p1 4s1 2P0.5 10451600.0 cm-1
2s1 2p1 4p1 4D0.5 10470800.0 cm-1
2s1 2p1 4p1 4D1.5 10487900.0 cm-1
2s1 2p1 4p1 4S1.5 10498900.0 cm-1
2s1 2p1 4s1 4P2.5 10500500.0 cm-1
2s1 2p1 4p1 4D2.5 10512800.0 cm-1
2s1 2p1 4p1 4P0.5 10513300.0 cm-1
2s1 2p1 4p1 2P0.5 10516400.0 cm-1
2s1 2p1 4s1 2P1.5 10523600.0 cm-1
2s1 2p1 4p1 2D1.5 10526000.0 cm-1
2s1 2p1 4d1 4F1.5 10537400.0 cm-1
2s1 2p1 4d1 4F2.5 10547700.0 cm-1
2s1 2p1 4d1 4P2.5 10566200.0 cm-1
2s1 2p1 4d1 4F3.5 10570400.0 cm-1
2s1 2p1 4d1 4D1.5 10572800.0 cm-1
2s1 2p1 4d1 4D0.5 10575500.0 cm-1
2s1 2p1 4p1 4D3.5 10576700.0 cm-1
2s1 2p1 4p1 4P1.5 10576800.0 cm-1
2s1 2p1 4p1 4P2.5 10580000.0 cm-1
2s1 2p1 4f1 4G2.5 10580900.0 cm-1
2s1 2p1 4f1 4D3.5 10582800.0 cm-1
2s1 2p1 4p1 2P1.5 10586000.0 cm-1
2s1 2p1 4d1 2D1.5 10587100.0 cm-1
2s1 2p1 4d1 2F2.5 10594300.0 cm-1
2s1 2p1 4p1 2D2.5 10601400.0 cm-1
2s1 2p1 4f1 4F1.5 10605000.0 cm-1
2s1 2p1 4f1 4G3.5 10606700.0 cm-1
2s1 2p1 4f1 2F2.5 10606800.0 cm-1
2s1 2p1 4f1 4G4.5 10607200.0 cm-1
2s1 2p1 4f1 2D2.5 10612800.0 cm-1
2s1 2p1 4p1 2S0.5 10613000.0 cm-1
2s1 2p1 4f1 2G3.5 10613500.0 cm-1
2s1 2p1 4d1 4F4.5 10632000.0 cm-1
2s1 2p1 4d1 4D3.5 10639400.0 cm-1
2s1 2p1 4d1 4D2.5 10642500.0 cm-1
2s1 2p1 4d1 4P1.5 10645200.0 cm-1
2s1 2p1 4d1 4P0.5 10646200.0 cm-1
2s1 2p1 4d1 2D2.5 10654700.0 cm-1
2s1 2p1 4d1 2P1.5 10665500.0 cm-1
2s1 2p1 4d1 2F3.5 10674300.0 cm-1
2s1 2p1 4f1 4F3.5 10676400.0 cm-1
2s1 2p1 4f1 4F4.5 10676600.0 cm-1
2s1 2p1 4f1 4F2.5 10678500.0 cm-1
2s1 2p1 4d1 2P0.5 10679300.0 cm-1
2s1 2p1 4f1 2F3.5 10680600.0 cm-1
2s1 2p1 4f1 4G5.5 10680700.0 cm-1
2s1 2p1 4f1 4D1.5 10682200.0 cm-1
2s1 2p1 4f1 4D0.5 10684800.0 cm-1
2s1 2p1 4f1 2G4.5 10685000.0 cm-1
2s1 2p1 4f1 4D2.5 10685200.0 cm-1
2s1 2p1 4f1 2D1.5 10690800.0 cm-1
2s1 2p1 4s1 2P0.5 10786500.0 cm-1
2s1 2p1 4s1 2P1.5 10787900.0 cm-1
2s1 2p1 4p1 2D1.5 10855300.0 cm-1
2s1 2p1 4p1 2P0.5 10857100.0 cm-1
2s1 2p1 4p1 2D2.5 10863100.0 cm-1
2s1 2p1 4p1 2P1.5 10868100.0 cm-1
2s1 2p1 4p1 2S0.5 10877500.0 cm-1
2s1 2p1 4d1 2D1.5 10923600.0 cm-1
2s1 2p1 4d1 2F2.5 10923900.0 cm-1
2s1 2p1 4d1 2F3.5 10924200.0 cm-1
2s1 2p1 4d1 2D2.5 10928200.0 cm-1
2s1 2p1 4d1 2P0.5 10937000.0 cm-1
2s1 2p1 4d1 2P1.5 10940600.0 cm-1
2s1 2p1 4f1 2F2.5 10952000.0 cm-1
2s1 2p1 4f1 2F3.5 10953700.0 cm-1
2s1 2p1 4f1 2G3.5 10962000.0 cm-1
2s1 2p1 4f1 2G4.5 10963600.0 cm-1
2s1 2p1 4f1 2D1.5 10968200.0 cm-1
2s1 2p1 4f1 2D2.5 10969700.0 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 = 1.37987
         2S = 1.25137
         2P = 1.17495
         3S = 1.58327
         3P = 1.37281
         3D = 1.48564
         4S = 1.50016
         4P = 1.38294
         4D = 1.53668
         4F = 1.57186

 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 1425.6504 Rydbergs (19397.399342 eV)

 A fine energy mesh of 0.000002 Z**2 Rydbergs (0.0108848 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (5.4424 eV) was used
 from the last threshold up to 0.890232 Z**2 Rydbergs (4845 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (5.4424 eV) was used
 from first threshold up to 0.890232 Z**2 Rydbergs (4845 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:        19/04/12

 Those data points with same collision strength in OMEGAU at higher energies
 are deleted. The adf04 file is generated based upon this correction.

 Date:  Tue May 28 22:44:48 2013


  • Guiyun Liang
  • Nigel Badnell
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