flike_mcw06#al4.dat

Resolved Specific Ion Data Collections

Ion
Al4+
Temperature Range
0.431 eV → 4308 eV

ADF04

Filename
flike_mcw06#al4.dat
Full Path
adf04/copaw#f/flike_mcw06#al4.dat
Download data
  • Spontaneous Emission: Al+4(i) → Al+4(j) + hv
  • Electron Impact Excitation: Al+4(i) + e → Al+4(j) + e
2s2 2p5 2P1.5 0.0 cm-1
2s2 2p5 2P0.5 3739.0 cm-1
2s1 2p6 2S0.5 380389.0 cm-1
2s2 2p4 3s1 4P2.5 734855.0 cm-1
2s2 2p4 3s1 4P1.5 736968.0 cm-1
2s2 2p4 3s1 4P0.5 738246.0 cm-1
2s2 2p4 3s1 2P1.5 748025.0 cm-1
2s2 2p4 3s1 2P0.5 750565.0 cm-1
2s2 2p4 3s1 2D2.5 781907.0 cm-1
2s2 2p4 3s1 2D1.5 781928.0 cm-1
2s2 2p4 3p1 4P2.5 800368.0 cm-1
2s2 2p4 3p1 4P1.5 801170.0 cm-1
2s2 2p4 3p1 4P0.5 801968.0 cm-1
2s2 2p4 3p1 4D3.5 808759.0 cm-1
2s2 2p4 3p1 4D2.5 810045.0 cm-1
2s2 2p4 3p1 4D1.5 811059.0 cm-1
2s2 2p4 3p1 4D0.5 811625.0 cm-1
2s2 2p4 3p1 2D2.5 815228.0 cm-1
2s2 2p4 3p1 2D1.5 817383.0 cm-1
2s2 2p4 3p1 2S0.5 819428.0 cm-1
2s2 2p4 3p1 4S1.5 820564.0 cm-1
2s2 2p4 3p1 2P1.5 822493.0 cm-1
2s2 2p4 3p1 2P0.5 822667.0 cm-1
2s2 2p4 3s1 2S0.5 843295.0 cm-1
2s2 2p4 3p1 2F2.5 850496.0 cm-1
2s2 2p4 3p1 2F3.5 850855.0 cm-1
2s2 2p4 3p1 2D1.5 859040.0 cm-1
2s2 2p4 3p1 2D2.5 859279.0 cm-1
2s2 2p4 3p1 2P1.5 875957.0 cm-1
2s2 2p4 3p1 2P0.5 877693.0 cm-1
2s2 2p4 3d1 4D3.5 893928.0 cm-1
2s2 2p4 3d1 4D2.5 894255.0 cm-1
2s2 2p4 3d1 4D1.5 894669.0 cm-1
2s2 2p4 3d1 4D0.5 895023.0 cm-1
2s2 2p4 3d1 4F4.5 900841.0 cm-1
2s2 2p4 3d1 4F3.5 902026.0 cm-1
2s2 2p4 3d1 4F2.5 903076.0 cm-1
2s2 2p4 3d1 4F1.5 903797.0 cm-1
2s2 2p4 3d1 4P0.5 904206.0 cm-1
2s2 2p4 3d1 4P1.5 904953.0 cm-1
2s2 2p4 3d1 2F3.5 905044.0 cm-1
2s2 2p4 3d1 4P2.5 906005.0 cm-1
2s2 2p4 3d1 2F2.5 906789.0 cm-1
2s2 2p4 3d1 2D1.5 909883.0 cm-1
2s2 2p4 3d1 2P0.5 910051.0 cm-1
2s2 2p4 3d1 2D2.5 910919.0 cm-1
2s2 2p4 3d1 2P1.5 912689.0 cm-1
2s2 2p4 3p1 2P1.5 917812.0 cm-1
2s2 2p4 3p1 2P0.5 917978.0 cm-1
2s2 2p4 3d1 2G3.5 940996.0 cm-1
2s2 2p4 3d1 2G4.5 941059.0 cm-1
2s2 2p4 3d1 2P1.5 946016.0 cm-1
2s2 2p4 3d1 2S0.5 946245.0 cm-1
2s2 2p4 3d1 2P0.5 946950.0 cm-1
2s2 2p4 3d1 2F2.5 948265.0 cm-1
2s2 2p4 3d1 2F3.5 948556.0 cm-1
2s2 2p4 3d1 2D2.5 948736.0 cm-1
2s2 2p4 3d1 2D1.5 949229.0 cm-1
2s2 2p4 4s1 4P2.5 983161.0 cm-1
2s2 2p4 4s1 4P1.5 984987.0 cm-1
2s2 2p4 4s1 4P0.5 986500.0 cm-1
2s2 2p4 4s1 2P1.5 987926.0 cm-1
2s2 2p4 4s1 2P0.5 990222.0 cm-1
2s2 2p4 4p1 4P2.5 1006910.0 cm-1
2s2 2p4 3d1 2D2.5 1007120.0 cm-1
2s2 2p4 3d1 2D1.5 1007220.0 cm-1
2s2 2p4 4p1 4P1.5 1007700.0 cm-1
2s2 2p4 4p1 4P0.5 1008680.0 cm-1
2s2 2p4 4p1 4D3.5 1009800.0 cm-1
2s2 2p4 4p1 4D2.5 1010830.0 cm-1
2s2 2p4 4p1 4D1.5 1012210.0 cm-1
2s2 2p4 4p1 2D2.5 1012900.0 cm-1
2s2 2p4 4p1 4D0.5 1012930.0 cm-1
2s2 2p4 4p1 2S0.5 1014300.0 cm-1
2s2 2p4 4p1 2D1.5 1014560.0 cm-1
2s2 2p4 4p1 4S1.5 1014700.0 cm-1
2s2 2p4 4p1 2P1.5 1021920.0 cm-1
2s2 2p4 4p1 2P0.5 1022390.0 cm-1
2s2 2p4 4s1 2D2.5 1027330.0 cm-1
2s2 2p4 4s1 2D1.5 1027340.0 cm-1
2s2 2p4 4d1 4D3.5 1040380.0 cm-1
2s2 2p4 4d1 4D2.5 1040610.0 cm-1
2s2 2p4 4d1 4D1.5 1041040.0 cm-1
2s2 2p4 4d1 4D0.5 1041530.0 cm-1
2s2 2p4 4d1 4F4.5 1042360.0 cm-1
2s2 2p4 4d1 4F3.5 1043260.0 cm-1
2s2 2p4 4d1 4P0.5 1043970.0 cm-1
2s2 2p4 4d1 4F2.5 1044440.0 cm-1
2s2 2p4 4d1 4P1.5 1044680.0 cm-1
2s2 2p4 4d1 2F3.5 1045150.0 cm-1
2s2 2p4 4d1 4F1.5 1045480.0 cm-1
2s2 2p4 4d1 4P2.5 1045900.0 cm-1
2s2 2p4 4d1 2F2.5 1046440.0 cm-1
2s2 2p4 4d1 2P0.5 1047960.0 cm-1
2s2 2p4 4d1 2P1.5 1048380.0 cm-1
2s2 2p4 4f1 4F4.5 1049260.0 cm-1
2s2 2p4 4f1 4F3.5 1049280.0 cm-1
2s2 2p4 4f1 4F2.5 1049380.0 cm-1
2s2 2p4 4f1 2F3.5 1049490.0 cm-1
2s2 2p4 4d1 2D2.5 1049580.0 cm-1
2s2 2p4 4f1 4F1.5 1049680.0 cm-1
2s2 2p4 4f1 2F2.5 1049800.0 cm-1
2s2 2p4 4f1 4G5.5 1050230.0 cm-1
2s2 2p4 4f1 2G4.5 1050260.0 cm-1
2s2 2p4 4f1 4D0.5 1050350.0 cm-1
2s2 2p4 4f1 2D1.5 1050430.0 cm-1
2s2 2p4 4d1 2D1.5 1050740.0 cm-1
2s2 2p4 4p1 2F2.5 1052220.0 cm-1
2s2 2p4 4f1 4D1.5 1052280.0 cm-1
2s2 2p4 4f1 4D2.5 1052360.0 cm-1
2s2 2p4 4p1 2F3.5 1052360.0 cm-1
2s2 2p4 4f1 4G4.5 1052530.0 cm-1
2s2 2p4 4f1 4G3.5 1052580.0 cm-1
2s2 2p4 4f1 4D3.5 1052920.0 cm-1
2s2 2p4 4f1 2D2.5 1052970.0 cm-1
2s2 2p4 4f1 2G3.5 1053770.0 cm-1
2s2 2p4 4f1 4G2.5 1053780.0 cm-1
2s2 2p4 4p1 2D1.5 1054860.0 cm-1
2s2 2p4 4p1 2D2.5 1054980.0 cm-1
2s2 2p4 4p1 2P1.5 1056190.0 cm-1
2s2 2p4 4p1 2P0.5 1057160.0 cm-1
2s1 2p5 3s1 4P2.5 1072930.0 cm-1
2s1 2p5 3s1 4P1.5 1074980.0 cm-1
2s1 2p5 3s1 4P0.5 1076280.0 cm-1
2s2 2p4 4d1 2G3.5 1084280.0 cm-1
2s2 2p4 4d1 2G4.5 1084300.0 cm-1
2s2 2p4 4d1 2S0.5 1084470.0 cm-1
2s2 2p4 4d1 2P1.5 1086690.0 cm-1
2s2 2p4 4d1 2F2.5 1086940.0 cm-1
2s2 2p4 4d1 2F3.5 1087020.0 cm-1
2s2 2p4 4d1 2P0.5 1087050.0 cm-1
2s2 2p4 4d1 2D2.5 1087490.0 cm-1
2s2 2p4 4d1 2D1.5 1087750.0 cm-1
2s2 2p4 4f1 2P0.5 1091260.0 cm-1
2s2 2p4 4f1 2P1.5 1091270.0 cm-1
2s2 2p4 4s1 2S0.5 1091590.0 cm-1
2s2 2p4 4f1 2D2.5 1092220.0 cm-1
2s2 2p4 4f1 2D1.5 1092220.0 cm-1
2s2 2p4 4f1 2H4.5 1092250.0 cm-1
2s2 2p4 4f1 2H5.5 1092260.0 cm-1
2s2 2p4 4f1 2F2.5 1093170.0 cm-1
2s2 2p4 4f1 2F3.5 1093170.0 cm-1
2s2 2p4 4f1 2G3.5 1093470.0 cm-1
2s2 2p4 4f1 2G4.5 1093480.0 cm-1
2s1 2p5 3s1 2P1.5 1095200.0 cm-1
2s1 2p5 3s1 2P0.5 1097360.0 cm-1
2s2 2p4 4p1 2P1.5 1116830.0 cm-1
2s2 2p4 4p1 2P0.5 1117060.0 cm-1
2s1 2p5 3p1 4S1.5 1131760.0 cm-1
2s1 2p5 3p1 4D3.5 1141750.0 cm-1
2s1 2p5 3p1 4D2.5 1142790.0 cm-1
2s1 2p5 3p1 4D1.5 1143790.0 cm-1
2s1 2p5 3p1 4D0.5 1144510.0 cm-1
2s2 2p4 4d1 2D2.5 1147860.0 cm-1
2s2 2p4 4d1 2D1.5 1147950.0 cm-1
2s1 2p5 3p1 4P2.5 1150040.0 cm-1
2s1 2p5 3p1 2D2.5 1151220.0 cm-1
2s1 2p5 3p1 4P1.5 1151240.0 cm-1
2s1 2p5 3p1 4P0.5 1151700.0 cm-1
2s1 2p5 3p1 2D1.5 1152540.0 cm-1
2s1 2p5 3p1 2P1.5 1154460.0 cm-1
2s2 2p4 4f1 2F2.5 1154660.0 cm-1
2s2 2p4 4f1 2F3.5 1154670.0 cm-1
2s1 2p5 3p1 2P0.5 1155050.0 cm-1
2s1 2p5 3p1 2S0.5 1187610.0 cm-1
2s1 2p5 3s1 2P1.5 1219740.0 cm-1
2s1 2p5 3s1 2P0.5 1219850.0 cm-1
2s1 2p5 3d1 4P0.5 1226750.0 cm-1
2s1 2p5 3d1 4P1.5 1227320.0 cm-1
2s1 2p5 3d1 4P2.5 1228340.0 cm-1
2s1 2p5 3d1 4F4.5 1230020.0 cm-1
2s1 2p5 3d1 4F3.5 1231030.0 cm-1
2s1 2p5 3d1 4F2.5 1231990.0 cm-1
2s1 2p5 3d1 4F1.5 1232800.0 cm-1
2s1 2p5 3d1 2F3.5 1236800.0 cm-1
2s1 2p5 3d1 4D3.5 1238400.0 cm-1
2s1 2p5 3d1 4D2.5 1238430.0 cm-1
2s1 2p5 3d1 4D1.5 1238790.0 cm-1
2s1 2p5 3d1 4D0.5 1238790.0 cm-1
2s1 2p5 3d1 2F2.5 1239060.0 cm-1
2s1 2p5 3d1 2D2.5 1242440.0 cm-1
2s1 2p5 3d1 2D1.5 1242560.0 cm-1
2s1 2p5 3d1 2P0.5 1248060.0 cm-1
2s1 2p5 3d1 2P1.5 1249670.0 cm-1
2s1 2p5 3p1 2D1.5 1286110.0 cm-1
2s1 2p5 3p1 2D2.5 1286480.0 cm-1
2s1 2p5 3p1 2P0.5 1290640.0 cm-1
2s1 2p5 3p1 2P1.5 1290820.0 cm-1
2s1 2p5 3p1 2S0.5 1301140.0 cm-1
2s1 2p5 3d1 2F2.5 1373730.0 cm-1
2s1 2p5 3d1 2F3.5 1373770.0 cm-1
2s1 2p5 3d1 2P1.5 1375910.0 cm-1
2s1 2p5 3d1 2P0.5 1375980.0 cm-1
2s1 2p5 3d1 2D1.5 1378760.0 cm-1
2s1 2p5 3d1 2D2.5 1378800.0 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
    AUTOSTRUCTURE.

     Calculation details
     +++++++++++++++++++

 The following scaling parameters on bound orbitals were used:

         1S = 1.4568
         2S = 1.1754
         2P = 1.1249
         3S = 1.0844
         3P = 1.0404
         3D = 1.0430
         4S = 1.0957
         4P = 1.0454
         4D = 1.0415
         4F = 1.0187

 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 0.000100 Z**2 Rydbergs (0.0217696 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (0.217696 eV) was used
 from the last threshold up to 2.225581 Z**2 Rydbergs (484.5 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (0.217696 eV) was used
 from first threshold up to 2.225581 Z**2 Rydbergs (484.5 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

 See:
      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

------------------------------------------------------------------------

Contributors

  • Mike Witthoeft
  • Allan Whiteford
  • Nigel Badnell
  • Processes
  • States
  • Comments
  • Origins

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