flike_mcw06#si5.dat

Resolved Specific Ion Data Collections

Ion
Si5+
Temperature Range
0.620 eV → 6204 eV

ADF04

Filename
flike_mcw06#si5.dat
Full Path
adf04/copaw#f/flike_mcw06#si5.dat
Download data
  • Spontaneous Emission: Si+5(i) → Si+5(j) + hv
  • Electron Impact Excitation: Si+5(i) + e → Si+5(j) + e
2s2 2p5 2P1.5 0.0 cm-1
2s2 2p5 2P0.5 5481.0 cm-1
2s1 2p6 2S0.5 427523.0 cm-1
2s2 2p4 3s1 4P2.5 974850.0 cm-1
2s2 2p4 3s1 4P1.5 977923.0 cm-1
2s2 2p4 3s1 4P0.5 979790.0 cm-1
2s2 2p4 3s1 2P1.5 990674.0 cm-1
2s2 2p4 3s1 2P0.5 994365.0 cm-1
2s2 2p4 3s1 2D2.5 1028110.0 cm-1
2s2 2p4 3s1 2D1.5 1028150.0 cm-1
2s2 2p4 3p1 4P2.5 1053170.0 cm-1
2s2 2p4 3p1 4P1.5 1054250.0 cm-1
2s2 2p4 3p1 4P0.5 1055480.0 cm-1
2s2 2p4 3p1 4D3.5 1063380.0 cm-1
2s2 2p4 3p1 4D2.5 1065180.0 cm-1
2s2 2p4 3p1 4D1.5 1066680.0 cm-1
2s2 2p4 3p1 4D0.5 1067490.0 cm-1
2s2 2p4 3p1 2D2.5 1071530.0 cm-1
2s2 2p4 3p1 2D1.5 1074550.0 cm-1
2s2 2p4 3p1 2P0.5 1075500.0 cm-1
2s2 2p4 3p1 4S1.5 1078040.0 cm-1
2s2 2p4 3p1 2P1.5 1079040.0 cm-1
2s2 2p4 3p1 2S0.5 1079950.0 cm-1
2s2 2p4 3s1 2S0.5 1096490.0 cm-1
2s2 2p4 3p1 2F2.5 1110190.0 cm-1
2s2 2p4 3p1 2F3.5 1110790.0 cm-1
2s2 2p4 3p1 2D1.5 1120640.0 cm-1
2s2 2p4 3p1 2D2.5 1121030.0 cm-1
2s2 2p4 3p1 2P1.5 1142490.0 cm-1
2s2 2p4 3p1 2P0.5 1144970.0 cm-1
2s2 2p4 3d1 4D3.5 1165750.0 cm-1
2s2 2p4 3d1 4D2.5 1166180.0 cm-1
2s2 2p4 3d1 4D1.5 1166790.0 cm-1
2s2 2p4 3d1 4D0.5 1167330.0 cm-1
2s2 2p4 3d1 4F4.5 1174810.0 cm-1
2s2 2p4 3d1 4F3.5 1176540.0 cm-1
2s2 2p4 3d1 4F2.5 1178080.0 cm-1
2s2 2p4 3d1 4F1.5 1179110.0 cm-1
2s2 2p4 3d1 4P0.5 1179310.0 cm-1
2s2 2p4 3d1 4P1.5 1180440.0 cm-1
2s2 2p4 3d1 2F3.5 1180840.0 cm-1
2s2 2p4 3d1 4P2.5 1182000.0 cm-1
2s2 2p4 3d1 2F2.5 1183420.0 cm-1
2s2 2p4 3p1 2P1.5 1186050.0 cm-1
2s2 2p4 3p1 2P0.5 1186390.0 cm-1
2s2 2p4 3d1 2P0.5 1186650.0 cm-1
2s2 2p4 3d1 2D1.5 1187390.0 cm-1
2s2 2p4 3d1 2D2.5 1189430.0 cm-1
2s2 2p4 3d1 2P1.5 1190880.0 cm-1
2s2 2p4 3d1 2G3.5 1219690.0 cm-1
2s2 2p4 3d1 2G4.5 1219800.0 cm-1
2s2 2p4 3d1 2S0.5 1226990.0 cm-1
2s2 2p4 3d1 2P1.5 1228190.0 cm-1
2s2 2p4 3d1 2F2.5 1229340.0 cm-1
2s2 2p4 3d1 2P0.5 1229690.0 cm-1
2s2 2p4 3d1 2F3.5 1229690.0 cm-1
2s2 2p4 3d1 2D2.5 1230860.0 cm-1
2s2 2p4 3d1 2D1.5 1232000.0 cm-1
2s2 2p4 3d1 2D2.5 1294680.0 cm-1
2s2 2p4 3d1 2D1.5 1294910.0 cm-1
2s2 2p4 4s1 4P2.5 1307290.0 cm-1
2s2 2p4 4s1 4P1.5 1309830.0 cm-1
2s2 2p4 4s1 4P0.5 1312140.0 cm-1
2s2 2p4 4s1 2P1.5 1313520.0 cm-1
2s2 2p4 4s1 2P0.5 1316740.0 cm-1
2s2 2p4 4p1 4P2.5 1332880.0 cm-1
2s2 2p4 4p1 4P1.5 1334390.0 cm-1
2s2 2p4 4p1 4P0.5 1335860.0 cm-1
2s2 2p4 4p1 4D3.5 1340040.0 cm-1
2s2 2p4 4p1 4D2.5 1341300.0 cm-1
2s2 2p4 4p1 4D1.5 1343380.0 cm-1
2s2 2p4 4p1 2D2.5 1344150.0 cm-1
2s2 2p4 4p1 4D0.5 1344510.0 cm-1
2s2 2p4 4p1 2S0.5 1345720.0 cm-1
2s2 2p4 4p1 4S1.5 1346270.0 cm-1
2s2 2p4 4p1 2D1.5 1346560.0 cm-1
2s2 2p4 4p1 2P1.5 1353670.0 cm-1
2s2 2p4 4p1 2P0.5 1354540.0 cm-1
2s2 2p4 4s1 2D2.5 1357190.0 cm-1
2s2 2p4 4s1 2D1.5 1357210.0 cm-1
2s1 2p5 3s1 4P2.5 1358250.0 cm-1
2s1 2p5 3s1 4P1.5 1361000.0 cm-1
2s1 2p5 3s1 4P0.5 1362660.0 cm-1
2s1 2p5 3s1 2P1.5 1371200.0 cm-1
2s1 2p5 3s1 2P0.5 1373870.0 cm-1
2s2 2p4 4d1 4D3.5 1376990.0 cm-1
2s2 2p4 4d1 4D2.5 1377300.0 cm-1
2s2 2p4 4d1 4D1.5 1377900.0 cm-1
2s2 2p4 4d1 4D0.5 1378630.0 cm-1
2s2 2p4 4d1 4F4.5 1379580.0 cm-1
2s2 2p4 4d1 4F3.5 1380850.0 cm-1
2s2 2p4 4d1 4P0.5 1381740.0 cm-1
2s2 2p4 4d1 4F2.5 1382570.0 cm-1
2s2 2p4 4d1 4P1.5 1382790.0 cm-1
2s2 2p4 4d1 2F3.5 1383630.0 cm-1
2s2 2p4 4d1 4F1.5 1384130.0 cm-1
2s2 2p4 4d1 4P2.5 1384580.0 cm-1
2s2 2p4 4d1 2F2.5 1385410.0 cm-1
2s2 2p4 4d1 2P0.5 1386910.0 cm-1
2s2 2p4 4d1 2D1.5 1387640.0 cm-1
2s2 2p4 4p1 2F2.5 1387780.0 cm-1
2s2 2p4 4p1 2F3.5 1387990.0 cm-1
2s2 2p4 4d1 2D2.5 1389520.0 cm-1
2s2 2p4 4f1 4F4.5 1389570.0 cm-1
2s2 2p4 4f1 4F3.5 1389600.0 cm-1
2s2 2p4 4f1 4F2.5 1389740.0 cm-1
2s2 2p4 4f1 2F3.5 1390030.0 cm-1
2s2 2p4 4f1 4F1.5 1390160.0 cm-1
2s2 2p4 4f1 2F2.5 1390430.0 cm-1
2s2 2p4 4d1 2P1.5 1391000.0 cm-1
2s2 2p4 4f1 4G5.5 1391080.0 cm-1
2s2 2p4 4f1 4D0.5 1391110.0 cm-1
2s2 2p4 4p1 2D1.5 1391110.0 cm-1
2s2 2p4 4f1 2G4.5 1391130.0 cm-1
2s2 2p4 4p1 2D2.5 1391260.0 cm-1
2s2 2p4 4f1 2D1.5 1391290.0 cm-1
2s2 2p4 4f1 4D1.5 1393990.0 cm-1
2s2 2p4 4f1 4D2.5 1394060.0 cm-1
2s2 2p4 4f1 4G4.5 1394450.0 cm-1
2s2 2p4 4f1 4G3.5 1394520.0 cm-1
2s2 2p4 4f1 4D3.5 1394960.0 cm-1
2s2 2p4 4f1 2D2.5 1395070.0 cm-1
2s2 2p4 4f1 2G3.5 1396180.0 cm-1
2s2 2p4 4f1 4G2.5 1396200.0 cm-1
2s2 2p4 4p1 2P1.5 1402690.0 cm-1
2s2 2p4 4p1 2P0.5 1404750.0 cm-1
2s2 2p4 4s1 2S0.5 1423810.0 cm-1
2s1 2p5 3p1 4S1.5 1424720.0 cm-1
2s2 2p4 4d1 2G3.5 1426710.0 cm-1
2s2 2p4 4d1 2G4.5 1426760.0 cm-1
2s2 2p4 4d1 2F2.5 1430130.0 cm-1
2s2 2p4 4d1 2P1.5 1430170.0 cm-1
2s2 2p4 4d1 2F3.5 1430260.0 cm-1
2s2 2p4 4d1 2P0.5 1430780.0 cm-1
2s2 2p4 4d1 2D2.5 1430920.0 cm-1
2s2 2p4 4d1 2D1.5 1431400.0 cm-1
2s2 2p4 4d1 2S0.5 1432280.0 cm-1
2s2 2p4 4f1 2P0.5 1436720.0 cm-1
2s2 2p4 4f1 2P1.5 1436740.0 cm-1
2s1 2p5 3p1 4D3.5 1436900.0 cm-1
2s2 2p4 4f1 2D2.5 1438100.0 cm-1
2s2 2p4 4f1 2D1.5 1438120.0 cm-1
2s2 2p4 4f1 2H4.5 1438250.0 cm-1
2s2 2p4 4f1 2H5.5 1438270.0 cm-1
2s1 2p5 3p1 4D2.5 1438310.0 cm-1
2s2 2p4 4f1 2F3.5 1439470.0 cm-1
2s2 2p4 4f1 2F2.5 1439470.0 cm-1
2s1 2p5 3p1 4D1.5 1439740.0 cm-1
2s2 2p4 4f1 2G3.5 1439930.0 cm-1
2s2 2p4 4f1 2G4.5 1439950.0 cm-1
2s1 2p5 3p1 4D0.5 1440810.0 cm-1
2s1 2p5 3p1 4P2.5 1447190.0 cm-1
2s1 2p5 3p1 2D2.5 1448940.0 cm-1
2s1 2p5 3p1 4P1.5 1448960.0 cm-1
2s1 2p5 3p1 4P0.5 1449620.0 cm-1
2s1 2p5 3p1 2D1.5 1450540.0 cm-1
2s1 2p5 3p1 2P1.5 1453100.0 cm-1
2s1 2p5 3p1 2P0.5 1453640.0 cm-1
2s2 2p4 4p1 2P1.5 1459280.0 cm-1
2s2 2p4 4p1 2P0.5 1459400.0 cm-1
2s1 2p5 3p1 2S0.5 1490100.0 cm-1
2s2 2p4 4d1 2D2.5 1498050.0 cm-1
2s2 2p4 4d1 2D1.5 1498180.0 cm-1
2s2 2p4 4f1 2F2.5 1507850.0 cm-1
2s2 2p4 4f1 2F3.5 1507860.0 cm-1
2s1 2p5 3s1 2P1.5 1516570.0 cm-1
2s1 2p5 3s1 2P0.5 1516710.0 cm-1
2s1 2p5 3d1 4P0.5 1538740.0 cm-1
2s1 2p5 3d1 4P1.5 1539560.0 cm-1
2s1 2p5 3d1 4P2.5 1541050.0 cm-1
2s1 2p5 3d1 4F4.5 1543380.0 cm-1
2s1 2p5 3d1 4F3.5 1544810.0 cm-1
2s1 2p5 3d1 4F2.5 1546190.0 cm-1
2s1 2p5 3d1 4F1.5 1547380.0 cm-1
2s1 2p5 3d1 2F3.5 1552880.0 cm-1
2s1 2p5 3d1 4D2.5 1554810.0 cm-1
2s1 2p5 3d1 4D3.5 1554980.0 cm-1
2s1 2p5 3d1 4D0.5 1555150.0 cm-1
2s1 2p5 3d1 4D1.5 1555180.0 cm-1
2s1 2p5 3d1 2F2.5 1556300.0 cm-1
2s1 2p5 3d1 2D2.5 1560610.0 cm-1
2s1 2p5 3d1 2D1.5 1560700.0 cm-1
2s1 2p5 3d1 2P0.5 1569180.0 cm-1
2s1 2p5 3d1 2P1.5 1571570.0 cm-1
2s1 2p5 3p1 2D1.5 1595920.0 cm-1
2s1 2p5 3p1 2D2.5 1596560.0 cm-1
2s1 2p5 3p1 2P0.5 1601460.0 cm-1
2s1 2p5 3p1 2P1.5 1601770.0 cm-1
2s1 2p5 3p1 2S0.5 1615210.0 cm-1
2s1 2p5 3d1 2F2.5 1702220.0 cm-1
2s1 2p5 3d1 2F3.5 1702310.0 cm-1
2s1 2p5 3d1 2P1.5 1705910.0 cm-1
2s1 2p5 3d1 2P0.5 1706050.0 cm-1
2s1 2p5 3d1 2D1.5 1708890.0 cm-1
2s1 2p5 3d1 2D2.5 1708960.0 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 = 1.4506
         2S = 1.1805
         2P = 1.1282
         3S = 1.0931
         3P = 1.0473
         3D = 1.0577
         4S = 1.1052
         4P = 1.0535
         4D = 1.0569
         4F = 1.0391

 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 0.000050 Z**2 Rydbergs (0.0170075 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (0.34015 eV) was used
 from the last threshold up to 1.856534 Z**2 Rydbergs (631.5 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (0.34015 eV) was used
 from first threshold up to 1.856534 Z**2 Rydbergs (631.5 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

------------------------------------------------------------------------
 Update: Martin O'Mullane, 04-11-2010
         Update ionisation potential from NIST database.

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

Dependents

Contributors

  • Mike Witthoeft
  • Allan Whiteford
  • Nigel Badnell
  • Martin O'Mullane
  • Processes
  • States
  • Comments
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