Resolved Specific Ion Data Collections

Temperature Range
14.48 eV → 1.448 x 105 eV


Full Path
Download data
  • Spontaneous Emission: As+28(i) → As+28(j) + hv
  • Electron Impact Excitation: As+28(i) + e → As+28(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 329312.0 cm-1
2s1 2p2 4P0.5 592123.0 cm-1
2s1 2p2 4P1.5 784611.0 cm-1
2s1 2p2 4P2.5 906063.0 cm-1
2s1 2p2 2D1.5 1168580.0 cm-1
2s1 2p2 2P0.5 1257370.0 cm-1
2s1 2p2 2D2.5 1298540.0 cm-1
2s1 2p2 2S0.5 1610400.0 cm-1
2s1 2p2 2P1.5 1626410.0 cm-1
2p3 4S1.5 1896290.0 cm-1
2p3 2D1.5 2151340.0 cm-1
2p3 2D2.5 2240420.0 cm-1
2p3 2P0.5 2418330.0 cm-1
2p3 2P1.5 2651670.0 cm-1
2s2 3s1 2S0.5 13959500.0 cm-1
2s2 3p1 2P0.5 14201800.0 cm-1
2s2 3p1 2P1.5 14292200.0 cm-1
2s1 2p1 3s1 4P0.5 14434000.0 cm-1
2s1 2p1 3s1 4P1.5 14500800.0 cm-1
2s2 3d1 2D1.5 14514100.0 cm-1
2s2 3d1 2D2.5 14544300.0 cm-1
2s1 2p1 3s1 2P0.5 14576900.0 cm-1
2s1 2p1 3p1 4D0.5 14646200.0 cm-1
2s1 2p1 3p1 4D1.5 14707300.0 cm-1
2s1 2p1 3s1 4P2.5 14752400.0 cm-1
2s1 2p1 3p1 4S1.5 14780100.0 cm-1
2s1 2p1 3p1 4P0.5 14800200.0 cm-1
2s1 2p1 3p1 2P0.5 14824200.0 cm-1
2s1 2p1 3p1 4D2.5 14831100.0 cm-1
2s1 2p1 3s1 2P1.5 14840800.0 cm-1
2s1 2p1 3p1 2D1.5 14868900.0 cm-1
2s1 2p1 3d1 4F1.5 14942100.0 cm-1
2s1 2p1 3d1 4F2.5 14988300.0 cm-1
2s1 2p1 3p1 4P1.5 15020000.0 cm-1
2s1 2p1 3d1 4P2.5 15042700.0 cm-1
2s1 2p1 3p1 4P2.5 15042800.0 cm-1
2s1 2p1 3d1 4F3.5 15060700.0 cm-1
2s1 2p1 3d1 4D1.5 15064900.0 cm-1
2s1 2p1 3p1 4D3.5 15065000.0 cm-1
2s1 2p1 3d1 4D0.5 15069900.0 cm-1
2s1 2p1 3p1 2P1.5 15089800.0 cm-1
2s1 2p1 3s1 2P1.5 15115400.0 cm-1
2s1 2p1 3s1 2P0.5 15117300.0 cm-1
2s1 2p1 3d1 2D1.5 15144400.0 cm-1
2s1 2p1 3d1 2F2.5 15153000.0 cm-1
2s1 2p1 3p1 2D2.5 15154400.0 cm-1
2s1 2p1 3p1 2S0.5 15179200.0 cm-1
2s1 2p1 3d1 4F4.5 15276900.0 cm-1
2s1 2p1 3d1 4D3.5 15306300.0 cm-1
2s1 2p1 3d1 4D2.5 15309900.0 cm-1
2p2 3s1 4P0.5 15318500.0 cm-1
2s1 2p1 3d1 4P1.5 15320800.0 cm-1
2s1 2p1 3d1 4P0.5 15323300.0 cm-1
2s1 2p1 3p1 2P0.5 15365100.0 cm-1
2s1 2p1 3d1 2D2.5 15365100.0 cm-1
2s1 2p1 3p1 2D1.5 15369800.0 cm-1
2s1 2p1 3d1 2P1.5 15407400.0 cm-1
2s1 2p1 3p1 2D2.5 15433300.0 cm-1
2s1 2p1 3d1 2F3.5 15449400.0 cm-1
2s1 2p1 3p1 2P1.5 15455300.0 cm-1
2s1 2p1 3d1 2P0.5 15473500.0 cm-1
2s1 2p1 3p1 2S0.5 15506800.0 cm-1
2p2 3p1 4D0.5 15520000.0 cm-1
2p2 3s1 4P1.5 15548800.0 cm-1
2p2 3s1 2P0.5 15612500.0 cm-1
2p2 3s1 4P2.5 15632300.0 cm-1
2p2 3p1 4D1.5 15644900.0 cm-1
2s1 2p1 3d1 2F2.5 15666400.0 cm-1
2s1 2p1 3d1 2F3.5 15670700.0 cm-1
2s1 2p1 3d1 2D1.5 15676700.0 cm-1
2p2 3s1 2D1.5 15681000.0 cm-1
2s1 2p1 3d1 2D2.5 15712900.0 cm-1
2s1 2p1 3d1 2P0.5 15716200.0 cm-1
2p2 3p1 2S0.5 15735600.0 cm-1
2s1 2p1 3d1 2P1.5 15745300.0 cm-1
2p2 3p1 4P1.5 15774900.0 cm-1
2p2 3d1 4F1.5 15812400.0 cm-1
2p2 3p1 4D2.5 15827700.0 cm-1
2p2 3p1 4P2.5 15851700.0 cm-1
2p2 3p1 4P0.5 15867700.0 cm-1
2p2 3d1 2F2.5 15876600.0 cm-1
2p2 3p1 2D1.5 15894300.0 cm-1
2p2 3p1 4D3.5 15928200.0 cm-1
2p2 3s1 2D2.5 15945800.0 cm-1
2p2 3p1 4S1.5 15953000.0 cm-1
2p2 3p1 2P1.5 15978800.0 cm-1
2p2 3s1 2P1.5 15982800.0 cm-1
2p2 3p1 2F2.5 16008300.0 cm-1
2p2 3d1 2P1.5 16039600.0 cm-1
2p2 3d1 4F2.5 16048900.0 cm-1
2p2 3d1 4D0.5 16051200.0 cm-1
2p2 3d1 4F3.5 16060200.0 cm-1
2p2 3p1 2P0.5 16072500.0 cm-1
2p2 3d1 4D3.5 16106500.0 cm-1
2p2 3d1 4P2.5 16117800.0 cm-1
2p2 3d1 4D1.5 16118900.0 cm-1
2p2 3d1 4F4.5 16136000.0 cm-1
2p2 3d1 4D2.5 16183000.0 cm-1
2p2 3d1 4P1.5 16199900.0 cm-1
2p2 3s1 2S0.5 16200000.0 cm-1
2p2 3p1 2D1.5 16208200.0 cm-1
2p2 3d1 4P0.5 16224100.0 cm-1
2p2 3p1 2D2.5 16227300.0 cm-1
2p2 3p1 2D2.5 16236500.0 cm-1
2p2 3p1 2F3.5 16241600.0 cm-1
2p2 3d1 2G3.5 16241700.0 cm-1
2p2 3d1 2D2.5 16256100.0 cm-1
2p2 3p1 2P0.5 16256900.0 cm-1
2p2 3d1 2P0.5 16259900.0 cm-1
2p2 3d1 2D1.5 16264500.0 cm-1
2p2 3p1 2P1.5 16410100.0 cm-1
2p2 3d1 2F3.5 16434600.0 cm-1
2p2 3d1 2G4.5 16455300.0 cm-1
2p2 3p1 2P0.5 16470900.0 cm-1
2p2 3d1 2D1.5 16475900.0 cm-1
2p2 3d1 2D2.5 16480600.0 cm-1
2p2 3d1 2P0.5 16485200.0 cm-1
2p2 3d1 2F3.5 16515100.0 cm-1
2p2 3p1 2P1.5 16538600.0 cm-1
2p2 3d1 2S0.5 16560100.0 cm-1
2p2 3d1 2P1.5 16587100.0 cm-1
2p2 3d1 2F2.5 16597200.0 cm-1
2p2 3d1 2D2.5 16762600.0 cm-1
2p2 3d1 2D1.5 16766700.0 cm-1
2s2 4s1 2S0.5 18906400.0 cm-1
2s2 4p1 2P0.5 19007200.0 cm-1
2s2 4p1 2P1.5 19044100.0 cm-1
2s2 4d1 2D1.5 19126500.0 cm-1
2s2 4d1 2D2.5 19138700.0 cm-1
2s2 4f1 2F2.5 19187800.0 cm-1
2s2 4f1 2F3.5 19193700.0 cm-1
2s1 2p1 4s1 4P0.5 19370200.0 cm-1
2s1 2p1 4s1 4P1.5 19432800.0 cm-1
2s1 2p1 4s1 2P0.5 19458300.0 cm-1
2s1 2p1 4p1 4D0.5 19459500.0 cm-1
2s1 2p1 4p1 4D1.5 19506200.0 cm-1
2s1 2p1 4p1 4S1.5 19524400.0 cm-1
2s1 2p1 4p1 4P0.5 19551300.0 cm-1
2s1 2p1 4p1 4D2.5 19571100.0 cm-1
2s1 2p1 4p1 2P0.5 19573300.0 cm-1
2s1 2p1 4d1 4F1.5 19575900.0 cm-1
2s1 2p1 4p1 2D1.5 19583300.0 cm-1
2s1 2p1 4d1 4P2.5 19598100.0 cm-1
2s1 2p1 4d1 4F2.5 19639800.0 cm-1
2s1 2p1 4f1 4G2.5 19641300.0 cm-1
2s1 2p1 4f1 4D3.5 19647900.0 cm-1
2s1 2p1 4d1 4D1.5 19653800.0 cm-1
2s1 2p1 4d1 4D0.5 19658100.0 cm-1
2s1 2p1 4d1 4F3.5 19660100.0 cm-1
2s1 2p1 4d1 2D1.5 19679000.0 cm-1
2s1 2p1 4d1 2F2.5 19682400.0 cm-1
2s1 2p1 4s1 4P2.5 19693900.0 cm-1
2s1 2p1 4f1 4F1.5 19705700.0 cm-1
2s1 2p1 4f1 4G3.5 19707000.0 cm-1
2s1 2p1 4f1 4D2.5 19709400.0 cm-1
2s1 2p1 4f1 4G4.5 19711900.0 cm-1
2s1 2p1 4f1 2D2.5 19716900.0 cm-1
2s1 2p1 4f1 2G3.5 19719700.0 cm-1
2s1 2p1 4s1 2P1.5 19719900.0 cm-1
2s1 2p1 4p1 4P1.5 19797100.0 cm-1
2s1 2p1 4p1 4P2.5 19802500.0 cm-1
2s1 2p1 4p1 4D3.5 19818800.0 cm-1
2s1 2p1 4p1 2P1.5 19830400.0 cm-1
2s1 2p1 4p1 2D2.5 19850100.0 cm-1
2s1 2p1 4p1 2S0.5 19862800.0 cm-1
2s1 2p1 4d1 4F4.5 19903400.0 cm-1
2s1 2p1 4d1 4D3.5 19909400.0 cm-1
2s1 2p1 4d1 4D2.5 19910400.0 cm-1
2s1 2p1 4d1 4P1.5 19914600.0 cm-1
2s1 2p1 4d1 4P0.5 19915900.0 cm-1
2s1 2p1 4d1 2D2.5 19932100.0 cm-1
2s1 2p1 4d1 2P1.5 19944800.0 cm-1
2s1 2p1 4d1 2F3.5 19956200.0 cm-1
2s1 2p1 4f1 4F3.5 19965600.0 cm-1
2s1 2p1 4d1 2P0.5 19966100.0 cm-1
2s1 2p1 4f1 4F2.5 19968000.0 cm-1
2s1 2p1 4f1 4F4.5 19968200.0 cm-1
2s1 2p1 4f1 4D1.5 19973300.0 cm-1
2s1 2p1 4f1 2F3.5 19974600.0 cm-1
2s1 2p1 4f1 4G5.5 19975400.0 cm-1
2s1 2p1 4f1 4D0.5 19977500.0 cm-1
2s1 2p1 4f1 2G4.5 19979500.0 cm-1
2s1 2p1 4f1 2F2.5 19980900.0 cm-1
2s1 2p1 4f1 2D1.5 19989200.0 cm-1
2s1 2p1 4s1 2P0.5 20041200.0 cm-1
2s1 2p1 4s1 2P1.5 20044700.0 cm-1
2s1 2p1 4p1 2D1.5 20140900.0 cm-1
2s1 2p1 4p1 2P0.5 20141200.0 cm-1
2s1 2p1 4p1 2D2.5 20169700.0 cm-1
2s1 2p1 4p1 2P1.5 20179600.0 cm-1
2s1 2p1 4p1 2S0.5 20183100.0 cm-1
2s1 2p1 4d1 2D1.5 20255900.0 cm-1
2s1 2p1 4d1 2F2.5 20258400.0 cm-1
2s1 2p1 4d1 2F3.5 20262300.0 cm-1
2s1 2p1 4d1 2P0.5 20270700.0 cm-1
2s1 2p1 4d1 2D2.5 20270900.0 cm-1
2s1 2p1 4d1 2P1.5 20284100.0 cm-1
2s1 2p1 4f1 2F2.5 20303900.0 cm-1
2s1 2p1 4f1 2F3.5 20309700.0 cm-1
2s1 2p1 4f1 2G3.5 20316800.0 cm-1
2s1 2p1 4f1 2G4.5 20322000.0 cm-1
2s1 2p1 4f1 2D1.5 20324000.0 cm-1
2s1 2p1 4f1 2D2.5 20329500.0 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 = 1.37655
         2S = 1.25290
         2P = 1.17630
         3S = 1.57395
         3P = 1.37749
         3D = 1.48971
         4S = 1.50774
         4P = 1.38913
         4D = 1.53902
         4F = 1.60791

 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 2678.9781 Rydbergs (36450.176029 eV)

 A fine energy mesh of 0.000001 Z**2 Rydbergs (0.010667104 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (10.667104 eV) was used
 from the last threshold up to 0.840341 Z**2 Rydbergs (8964 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (10.667104 eV) was used
 from first threshold up to 0.840341 Z**2 Rydbergs (8964 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:        27/07/12

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

 Date:  Wed May 29 11:06:32 2013


  • Guiyun Liang
  • Nigel Badnell
  • Processes
  • States
  • Comments
  • Origins

Data Classes