Resolved Specific Ion Data Collections

Temperature Range
10.77 eV → 1.077 x 105 eV


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  • Spontaneous Emission: Cu+24(i) → Cu+24(j) + hv
  • Electron Impact Excitation: Cu+24(i) + e → Cu+24(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 187804.0 cm-1
2s1 2p2 4P0.5 476317.0 cm-1
2s1 2p2 4P1.5 573251.0 cm-1
2s1 2p2 4P2.5 655598.0 cm-1
2s1 2p2 2D1.5 900345.0 cm-1
2s1 2p2 2D2.5 952167.0 cm-1
2s1 2p2 2P0.5 1009410.0 cm-1
2s1 2p2 2S0.5 1209470.0 cm-1
2s1 2p2 2P1.5 1226000.0 cm-1
2p3 4S1.5 1505110.0 cm-1
2p3 2D1.5 1678430.0 cm-1
2p3 2D2.5 1735190.0 cm-1
2p3 2P0.5 1893490.0 cm-1
2p3 2P1.5 2006200.0 cm-1
2s2 3s1 2S0.5 10427000.0 cm-1
2s2 3p1 2P0.5 10633600.0 cm-1
2s2 3p1 2P1.5 10685700.0 cm-1
2s1 2p1 3s1 4P0.5 10834400.0 cm-1
2s2 3d1 2D1.5 10876600.0 cm-1
2s1 2p1 3s1 4P1.5 10879000.0 cm-1
2s2 3d1 2D2.5 10893700.0 cm-1
2s1 2p1 3s1 2P0.5 10951300.0 cm-1
2s1 2p1 3s1 4P2.5 11014400.0 cm-1
2s1 2p1 3p1 4D0.5 11016400.0 cm-1
2s1 2p1 3p1 4D1.5 11056700.0 cm-1
2s1 2p1 3s1 2P1.5 11094600.0 cm-1
2s1 2p1 3p1 2P1.5 11104900.0 cm-1
2s1 2p1 3p1 2P0.5 11126200.0 cm-1
2s1 2p1 3p1 4D2.5 11131800.0 cm-1
2s1 2p1 3p1 4P0.5 11136200.0 cm-1
2s1 2p1 3p1 2D1.5 11172100.0 cm-1
2s1 2p1 3d1 4F1.5 11241100.0 cm-1
2s1 2p1 3p1 4P1.5 11244300.0 cm-1
2s1 2p1 3p1 4D3.5 11255200.0 cm-1
2s1 2p1 3p1 4P2.5 11264900.0 cm-1
2s1 2p1 3d1 4F2.5 11270600.0 cm-1
2s1 2p1 3p1 4S1.5 11280000.0 cm-1
2s1 2p1 3d1 4F3.5 11317100.0 cm-1
2s1 2p1 3d1 4P2.5 11318200.0 cm-1
2s1 2p1 3d1 4D1.5 11332900.0 cm-1
2s1 2p1 3p1 2D2.5 11334700.0 cm-1
2s1 2p1 3d1 4D0.5 11337300.0 cm-1
2s1 2p1 3s1 2P0.5 11345200.0 cm-1
2s1 2p1 3s1 2P1.5 11347900.0 cm-1
2s1 2p1 3p1 2S0.5 11363800.0 cm-1
2s1 2p1 3d1 2D1.5 11384600.0 cm-1
2s1 2p1 3d1 2F2.5 11401800.0 cm-1
2s1 2p1 3d1 4F4.5 11428800.0 cm-1
2s1 2p1 3d1 4D3.5 11460100.0 cm-1
2s1 2p1 3d1 4D2.5 11468300.0 cm-1
2s1 2p1 3d1 4P1.5 11475500.0 cm-1
2s1 2p1 3d1 4P0.5 11477600.0 cm-1
2s1 2p1 3d1 2D2.5 11511200.0 cm-1
2s1 2p1 3p1 2P0.5 11549100.0 cm-1
2s1 2p1 3d1 2P1.5 11553100.0 cm-1
2s1 2p1 3p1 2D1.5 11559200.0 cm-1
2s1 2p1 3d1 2F3.5 11582800.0 cm-1
2p2 3s1 4P0.5 11584700.0 cm-1
2s1 2p1 3p1 2D2.5 11593000.0 cm-1
2s1 2p1 3d1 2P0.5 11601000.0 cm-1
2s1 2p1 3p1 2P1.5 11606500.0 cm-1
2s1 2p1 3p1 2S0.5 11656100.0 cm-1
2p2 3s1 4P1.5 11698400.0 cm-1
2p2 3p1 4D0.5 11751100.0 cm-1
2p2 3s1 4P2.5 11761900.0 cm-1
2p2 3s1 2P0.5 11763700.0 cm-1
2s1 2p1 3d1 2F3.5 11786300.0 cm-1
2s1 2p1 3d1 2F2.5 11786900.0 cm-1
2s1 2p1 3d1 2D1.5 11796900.0 cm-1
2p2 3s1 2P1.5 11815800.0 cm-1
2s1 2p1 3d1 2D2.5 11818500.0 cm-1
2p2 3p1 4D1.5 11822400.0 cm-1
2s1 2p1 3d1 2P0.5 11834600.0 cm-1
2s1 2p1 3d1 2P1.5 11853300.0 cm-1
2p2 3p1 2S0.5 11857000.0 cm-1
2p2 3p1 4P1.5 11894600.0 cm-1
2p2 3p1 4D2.5 11921400.0 cm-1
2p2 3p1 4P2.5 11939800.0 cm-1
2p2 3p1 4P0.5 11942600.0 cm-1
2p2 3s1 2D2.5 11958300.0 cm-1
2p2 3p1 2D1.5 11966100.0 cm-1
2p2 3d1 4F1.5 11973200.0 cm-1
2p2 3s1 2D1.5 11985700.0 cm-1
2p2 3p1 4D3.5 11986800.0 cm-1
2p2 3d1 4F2.5 12012800.0 cm-1
2p2 3p1 4S1.5 12029400.0 cm-1
2p2 3p1 2P1.5 12041600.0 cm-1
2p2 3p1 2D2.5 12053700.0 cm-1
2p2 3d1 2P1.5 12092100.0 cm-1
2p2 3p1 2P0.5 12099000.0 cm-1
2p2 3d1 4F3.5 12099100.0 cm-1
2p2 3d1 4D2.5 12100400.0 cm-1
2p2 3d1 4D0.5 12101600.0 cm-1
2p2 3d1 4D3.5 12141500.0 cm-1
2p2 3d1 4D1.5 12147500.0 cm-1
2p2 3d1 2F2.5 12148900.0 cm-1
2p2 3d1 4F4.5 12154500.0 cm-1
2p2 3p1 2F2.5 12167700.0 cm-1
2p2 3p1 2F3.5 12184100.0 cm-1
2p2 3p1 2D1.5 12186700.0 cm-1
2p2 3s1 2S0.5 12196700.0 cm-1
2p2 3d1 4P2.5 12202000.0 cm-1
2p2 3p1 2D2.5 12209500.0 cm-1
2p2 3d1 4P1.5 12217800.0 cm-1
2p2 3p1 2P0.5 12218800.0 cm-1
2p2 3d1 4P0.5 12229800.0 cm-1
2p2 3d1 2P0.5 12242800.0 cm-1
2p2 3d1 2G3.5 12245300.0 cm-1
2p2 3d1 2D2.5 12274500.0 cm-1
2p2 3d1 2D1.5 12277700.0 cm-1
2p2 3p1 2P1.5 12325900.0 cm-1
2p2 3d1 2F3.5 12336200.0 cm-1
2p2 3d1 2G4.5 12357500.0 cm-1
2p2 3d1 2D1.5 12382600.0 cm-1
2p2 3d1 2D2.5 12388000.0 cm-1
2p2 3d1 2P0.5 12403900.0 cm-1
2p2 3p1 2P0.5 12415900.0 cm-1
2p2 3d1 2F3.5 12418300.0 cm-1
2p2 3p1 2P1.5 12450000.0 cm-1
2p2 3d1 2S0.5 12457900.0 cm-1
2p2 3d1 2P1.5 12470700.0 cm-1
2p2 3d1 2F2.5 12473000.0 cm-1
2p2 3d1 2D2.5 12632100.0 cm-1
2p2 3d1 2D1.5 12640400.0 cm-1
2s2 4s1 2S0.5 14128800.0 cm-1
2s2 4p1 2P0.5 14214300.0 cm-1
2s2 4p1 2P1.5 14235700.0 cm-1
2s2 4d1 2D1.5 14306300.0 cm-1
2s2 4d1 2D2.5 14313200.0 cm-1
2s2 4f1 2F2.5 14354700.0 cm-1
2s2 4f1 2F3.5 14358000.0 cm-1
2s1 2p1 4s1 4P0.5 14529100.0 cm-1
2s1 2p1 4s1 4P1.5 14570800.0 cm-1
2s1 2p1 4s1 2P0.5 14592900.0 cm-1
2s1 2p1 4p1 4D0.5 14605200.0 cm-1
2s1 2p1 4p1 4D1.5 14634500.0 cm-1
2s1 2p1 4p1 4S1.5 14649700.0 cm-1
2s1 2p1 4p1 4P0.5 14670700.0 cm-1
2s1 2p1 4p1 4D2.5 14677200.0 cm-1
2s1 2p1 4p1 2P0.5 14679800.0 cm-1
2s1 2p1 4p1 2D1.5 14690200.0 cm-1
2s1 2p1 4d1 4F1.5 14693800.0 cm-1
2s1 2p1 4d1 4P2.5 14705300.0 cm-1
2s1 2p1 4s1 4P2.5 14713400.0 cm-1
2s1 2p1 4s1 2P1.5 14736500.0 cm-1
2s1 2p1 4d1 4F2.5 14739200.0 cm-1
2s1 2p1 4f1 4G2.5 14747100.0 cm-1
2s1 2p1 4d1 4D1.5 14748400.0 cm-1
2s1 2p1 4d1 4F3.5 14749400.0 cm-1
2s1 2p1 4f1 4D3.5 14751100.0 cm-1
2s1 2p1 4d1 4D0.5 14752000.0 cm-1
2s1 2p1 4d1 2D1.5 14767600.0 cm-1
2s1 2p1 4d1 2F2.5 14774800.0 cm-1
2s1 2p1 4f1 4F1.5 14789500.0 cm-1
2s1 2p1 4f1 4G3.5 14791100.0 cm-1
2s1 2p1 4f1 2F2.5 14792200.0 cm-1
2s1 2p1 4f1 4G4.5 14793300.0 cm-1
2s1 2p1 4f1 2D2.5 14798500.0 cm-1
2s1 2p1 4f1 2G3.5 14800500.0 cm-1
2s1 2p1 4p1 4P1.5 14801600.0 cm-1
2s1 2p1 4p1 4P2.5 14806200.0 cm-1
2s1 2p1 4p1 4D3.5 14809700.0 cm-1
2s1 2p1 4p1 2P1.5 14820000.0 cm-1
2s1 2p1 4p1 2D2.5 14837800.0 cm-1
2s1 2p1 4p1 2S0.5 14849700.0 cm-1
2s1 2p1 4d1 4F4.5 14878600.0 cm-1
2s1 2p1 4d1 4D3.5 14885800.0 cm-1
2s1 2p1 4d1 4D2.5 14888300.0 cm-1
2s1 2p1 4d1 4P1.5 14891700.0 cm-1
2s1 2p1 4d1 4P0.5 14892900.0 cm-1
2s1 2p1 4d1 2D2.5 14904100.0 cm-1
2s1 2p1 4d1 2P1.5 14915900.0 cm-1
2s1 2p1 4d1 2F3.5 14926500.0 cm-1
2s1 2p1 4f1 4F3.5 14931800.0 cm-1
2s1 2p1 4f1 4F4.5 14933000.0 cm-1
2s1 2p1 4d1 2P0.5 14933700.0 cm-1
2s1 2p1 4f1 4F2.5 14934100.0 cm-1
2s1 2p1 4f1 2F3.5 14938000.0 cm-1
2s1 2p1 4f1 4G5.5 14938500.0 cm-1
2s1 2p1 4f1 4D1.5 14938600.0 cm-1
2s1 2p1 4f1 4D0.5 14942100.0 cm-1
2s1 2p1 4f1 2G4.5 14942900.0 cm-1
2s1 2p1 4f1 4D2.5 14943400.0 cm-1
2s1 2p1 4f1 2D1.5 14950400.0 cm-1
2s1 2p1 4s1 2P0.5 15030600.0 cm-1
2s1 2p1 4s1 2P1.5 15033000.0 cm-1
2s1 2p1 4p1 2D1.5 15114600.0 cm-1
2s1 2p1 4p1 2P0.5 15115700.0 cm-1
2s1 2p1 4p1 2D2.5 15130400.0 cm-1
2s1 2p1 4p1 2P1.5 15137500.0 cm-1
2s1 2p1 4p1 2S0.5 15146600.0 cm-1
2s1 2p1 4d1 2D1.5 15203400.0 cm-1
2s1 2p1 4d1 2F2.5 15204800.0 cm-1
2s1 2p1 4d1 2F3.5 15206200.0 cm-1
2s1 2p1 4d1 2D2.5 15212100.0 cm-1
2s1 2p1 4d1 2P0.5 15218700.0 cm-1
2s1 2p1 4d1 2P1.5 15225600.0 cm-1
2s1 2p1 4f1 2F2.5 15240700.0 cm-1
2s1 2p1 4f1 2F3.5 15244000.0 cm-1
2s1 2p1 4f1 2G3.5 15252200.0 cm-1
2s1 2p1 4f1 2G4.5 15255200.0 cm-1
2s1 2p1 4f1 2D1.5 15259000.0 cm-1
2s1 2p1 4f1 2D2.5 15262000.0 cm-1
U+24        29        25      18610000.(  )

        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 = 1.37797
         2S = 1.25223
         2P = 1.17570
         3S = 1.57796
         3P = 1.37542
         3D = 1.48796
         4S = 1.50475
         4P = 1.38649
         4D = 1.53824
         4F = 1.59381

 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 2017.0345 Rydbergs (27443.771407 eV)

 A fine energy mesh of 0.000002 Z**2 Rydbergs (0.015674112 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (7.837056 eV) was used
 from the last threshold up to 0.850192 Z**2 Rydbergs (6663 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (7.837056 eV) was used
 from first threshold up to 0.850192 Z**2 Rydbergs (6663 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:        26/06/12

 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 23:16:11 2013


  • Guiyun Liang
  • Nigel Badnell
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