flike_mcw06#s7.dat

Resolved Specific Ion Data Collections

Ion
S7+
Temperature Range
1.103 eV → 1.103 x 104 eV

ADF04

Filename
flike_mcw06#s7.dat
Full Path
adf04/copaw#f/flike_mcw06#s7.dat
Download data
  • Spontaneous Emission: S+7(i) → S+7(j) + hv
  • Electron Impact Excitation: S+7(i) + e → S+7(j) + e
2s2 2p5 2P1.5 0.0 cm-1
2s2 2p5 2P0.5 10702.0 cm-1
2s1 2p6 2S0.5 523780.0 cm-1
2s2 2p4 3s1 4P2.5 1546240.0 cm-1
2s2 2p4 3s1 4P1.5 1552100.0 cm-1
2s2 2p4 3s1 4P0.5 1555770.0 cm-1
2s2 2p4 3s1 2P1.5 1567600.0 cm-1
2s2 2p4 3s1 2P0.5 1574610.0 cm-1
2s2 2p4 3s1 2D2.5 1612710.0 cm-1
2s2 2p4 3s1 2D1.5 1612850.0 cm-1
2s2 2p4 3p1 4P2.5 1650470.0 cm-1
2s2 2p4 3p1 4P1.5 1652170.0 cm-1
2s2 2p4 3p1 4P0.5 1654900.0 cm-1
2s2 2p4 3p1 4D3.5 1664160.0 cm-1
2s2 2p4 3p1 4D2.5 1667250.0 cm-1
2s2 2p4 3p1 4D1.5 1670430.0 cm-1
2s2 2p4 3p1 4D0.5 1671940.0 cm-1
2s2 2p4 3p1 2D2.5 1676190.0 cm-1
2s2 2p4 3p1 2P0.5 1678320.0 cm-1
2s2 2p4 3p1 2D1.5 1680840.0 cm-1
2s2 2p4 3p1 2P1.5 1684510.0 cm-1
2s2 2p4 3p1 4S1.5 1685850.0 cm-1
2s2 2p4 3p1 2S0.5 1687650.0 cm-1
2s2 2p4 3s1 2S0.5 1695280.0 cm-1
2s2 2p4 3p1 2F2.5 1721700.0 cm-1
2s2 2p4 3p1 2F3.5 1723100.0 cm-1
2s2 2p4 3p1 2D1.5 1735900.0 cm-1
2s2 2p4 3p1 2D2.5 1736820.0 cm-1
2s2 2p4 3p1 2P1.5 1767130.0 cm-1
2s2 2p4 3p1 2P0.5 1771540.0 cm-1
2s2 2p4 3d1 4D3.5 1799950.0 cm-1
2s2 2p4 3d1 4D2.5 1800610.0 cm-1
2s2 2p4 3d1 4D1.5 1801770.0 cm-1
2s2 2p4 3d1 4D0.5 1802940.0 cm-1
2s2 2p4 3d1 4F4.5 1813040.0 cm-1
2s2 2p4 3p1 2P1.5 1814820.0 cm-1
2s2 2p4 3p1 2P0.5 1815810.0 cm-1
2s2 2p4 3d1 4F3.5 1816280.0 cm-1
2s2 2p4 3d1 4F2.5 1819430.0 cm-1
2s2 2p4 3d1 4P0.5 1819990.0 cm-1
2s2 2p4 3d1 4F1.5 1821300.0 cm-1
2s2 2p4 3d1 4P1.5 1822380.0 cm-1
2s2 2p4 3d1 2F3.5 1823470.0 cm-1
2s2 2p4 3d1 4P2.5 1825360.0 cm-1
2s2 2p4 3d1 2F2.5 1828280.0 cm-1
2s2 2p4 3d1 2P0.5 1829470.0 cm-1
2s2 2p4 3d1 2D1.5 1832510.0 cm-1
2s2 2p4 3d1 2D2.5 1837840.0 cm-1
2s2 2p4 3d1 2P1.5 1838180.0 cm-1
2s2 2p4 3d1 2G3.5 1868290.0 cm-1
2s2 2p4 3d1 2G4.5 1868580.0 cm-1
2s2 2p4 3d1 2S0.5 1879740.0 cm-1
2s2 2p4 3d1 2F2.5 1882450.0 cm-1
2s2 2p4 3d1 2F3.5 1883280.0 cm-1
2s2 2p4 3d1 2P1.5 1885300.0 cm-1
2s2 2p4 3d1 2D2.5 1887600.0 cm-1
2s2 2p4 3d1 2P0.5 1888710.0 cm-1
2s2 2p4 3d1 2D1.5 1890660.0 cm-1
2s2 2p4 3d1 2D2.5 1961140.0 cm-1
2s2 2p4 3d1 2D1.5 1961850.0 cm-1
2s1 2p5 3s1 4P2.5 2006670.0 cm-1
2s1 2p5 3s1 4P1.5 2012270.0 cm-1
2s1 2p5 3s1 4P0.5 2016130.0 cm-1
2s1 2p5 3s1 2P1.5 2038660.0 cm-1
2s1 2p5 3s1 2P0.5 2045260.0 cm-1
2s2 2p4 4s1 4P2.5 2077980.0 cm-1
2s2 2p4 4s1 4P1.5 2082430.0 cm-1
2s2 2p4 4s1 4P0.5 2087100.0 cm-1
2s2 2p4 4s1 2P1.5 2088750.0 cm-1
2s2 2p4 4s1 2P0.5 2094590.0 cm-1
2s1 2p5 3p1 4S1.5 2104190.0 cm-1
2s1 2p5 3p1 4D3.5 2119590.0 cm-1
2s1 2p5 3p1 4D2.5 2121730.0 cm-1
2s2 2p4 4p1 4P2.5 2122880.0 cm-1
2s2 2p4 4p1 4P1.5 2124310.0 cm-1
2s1 2p5 3p1 4D1.5 2124560.0 cm-1
2s2 2p4 4p1 4D3.5 2124660.0 cm-1
2s2 2p4 4p1 2D2.5 2126710.0 cm-1
2s1 2p5 3p1 4D0.5 2126870.0 cm-1
2s2 2p4 4p1 4P0.5 2127370.0 cm-1
2s2 2p4 4p1 4D1.5 2131170.0 cm-1
2s1 2p5 3p1 2D2.5 2132890.0 cm-1
2s2 2p4 4p1 4D2.5 2132940.0 cm-1
2s2 2p4 4p1 4D0.5 2133550.0 cm-1
2s2 2p4 4p1 2S0.5 2133920.0 cm-1
2s2 2p4 4p1 2D1.5 2135840.0 cm-1
2s2 2p4 4p1 4S1.5 2136070.0 cm-1
2s1 2p5 3p1 2D1.5 2136570.0 cm-1
2s1 2p5 3p1 4P2.5 2137120.0 cm-1
2s1 2p5 3p1 4P1.5 2139000.0 cm-1
2s1 2p5 3p1 4P0.5 2140640.0 cm-1
2s1 2p5 3p1 2P1.5 2142210.0 cm-1
2s2 2p4 4p1 2P1.5 2142340.0 cm-1
2s2 2p4 4p1 2P0.5 2143200.0 cm-1
2s2 2p4 4s1 2D2.5 2143350.0 cm-1
2s1 2p5 3p1 2P0.5 2144350.0 cm-1
2s2 2p4 4s1 2D1.5 2145600.0 cm-1
2s2 2p4 4d1 4D3.5 2174970.0 cm-1
2s2 2p4 4d1 4D2.5 2175440.0 cm-1
2s2 2p4 4d1 4D1.5 2176480.0 cm-1
2s2 2p4 4d1 4D0.5 2177880.0 cm-1
2s2 2p4 4d1 4F4.5 2178120.0 cm-1
2s2 2p4 4d1 2F3.5 2180210.0 cm-1
2s2 2p4 4d1 4P0.5 2182130.0 cm-1
2s2 2p4 4d1 4F2.5 2183790.0 cm-1
2s2 2p4 4p1 2F2.5 2183840.0 cm-1
2s2 2p4 4d1 4P1.5 2184170.0 cm-1
2s2 2p4 4p1 2F3.5 2184350.0 cm-1
2s2 2p4 4d1 4F3.5 2185920.0 cm-1
2s1 2p5 3p1 2S0.5 2186140.0 cm-1
2s2 2p4 4d1 4F1.5 2187080.0 cm-1
2s2 2p4 4d1 4P2.5 2187780.0 cm-1
2s2 2p4 4p1 2D1.5 2188360.0 cm-1
2s2 2p4 4d1 2F2.5 2188830.0 cm-1
2s2 2p4 4p1 2D2.5 2188910.0 cm-1
2s2 2p4 4d1 2P0.5 2189830.0 cm-1
2s2 2p4 4d1 2P1.5 2191850.0 cm-1
2s2 2p4 4f1 4F4.5 2193340.0 cm-1
2s2 2p4 4f1 4F3.5 2193360.0 cm-1
2s2 2p4 4f1 4F2.5 2193720.0 cm-1
2s2 2p4 4p1 2P1.5 2193740.0 cm-1
2s2 2p4 4f1 4F1.5 2194520.0 cm-1
2s2 2p4 4f1 2F3.5 2195110.0 cm-1
2s2 2p4 4f1 2F2.5 2195670.0 cm-1
2s2 2p4 4d1 2D2.5 2196260.0 cm-1
2s2 2p4 4f1 4D0.5 2196480.0 cm-1
2s2 2p4 4f1 2D1.5 2197050.0 cm-1
2s2 2p4 4p1 2P0.5 2197340.0 cm-1
2s2 2p4 4f1 4G5.5 2197640.0 cm-1
2s2 2p4 4f1 2G4.5 2197740.0 cm-1
2s2 2p4 4d1 2D1.5 2198070.0 cm-1
2s2 2p4 4f1 4D1.5 2202220.0 cm-1
2s2 2p4 4f1 4D2.5 2202440.0 cm-1
2s2 2p4 4f1 4G4.5 2204000.0 cm-1
2s2 2p4 4f1 4D3.5 2204150.0 cm-1
2s2 2p4 4f1 4G3.5 2204340.0 cm-1
2s2 2p4 4f1 2D2.5 2204940.0 cm-1
2s1 2p5 3s1 2P0.5 2206710.0 cm-1
2s1 2p5 3s1 2P1.5 2206770.0 cm-1
2s2 2p4 4f1 4G2.5 2207030.0 cm-1
2s2 2p4 4f1 2G3.5 2207070.0 cm-1
2s2 2p4 4s1 2S0.5 2223510.0 cm-1
2s2 2p4 4d1 2G3.5 2236550.0 cm-1
2s2 2p4 4d1 2G4.5 2236670.0 cm-1
2s2 2p4 4d1 2F2.5 2241410.0 cm-1
2s2 2p4 4d1 2F3.5 2241750.0 cm-1
2s2 2p4 4d1 2P1.5 2242160.0 cm-1
2s2 2p4 4d1 2D2.5 2243210.0 cm-1
2s2 2p4 4d1 2P0.5 2243210.0 cm-1
2s2 2p4 4d1 2S0.5 2244330.0 cm-1
2s2 2p4 4d1 2D1.5 2244420.0 cm-1
2s2 2p4 4f1 2P0.5 2252520.0 cm-1
2s2 2p4 4f1 2P1.5 2252580.0 cm-1
2s1 2p5 3d1 4P0.5 2254690.0 cm-1
2s2 2p4 4f1 2D2.5 2254930.0 cm-1
2s2 2p4 4f1 2D1.5 2255080.0 cm-1
2s2 2p4 4f1 2H4.5 2255940.0 cm-1
2s2 2p4 4f1 2H5.5 2255990.0 cm-1
2s1 2p5 3d1 4P1.5 2256310.0 cm-1
2s2 2p4 4f1 2F3.5 2257450.0 cm-1
2s2 2p4 4f1 2F2.5 2257560.0 cm-1
2s2 2p4 4f1 2G4.5 2258540.0 cm-1
2s2 2p4 4f1 2G3.5 2258580.0 cm-1
2s1 2p5 3d1 4P2.5 2259180.0 cm-1
2s1 2p5 3d1 4F4.5 2264380.0 cm-1
2s1 2p5 3d1 4F3.5 2266670.0 cm-1
2s1 2p5 3d1 4F2.5 2269120.0 cm-1
2s2 2p4 4p1 2P0.5 2270840.0 cm-1
2s2 2p4 4p1 2P1.5 2270880.0 cm-1
2s1 2p5 3d1 4F1.5 2271400.0 cm-1
2s1 2p5 3d1 4D3.5 2278410.0 cm-1
2s1 2p5 3d1 4D2.5 2281620.0 cm-1
2s1 2p5 3d1 4D0.5 2281800.0 cm-1
2s1 2p5 3d1 4D1.5 2282130.0 cm-1
2s1 2p5 3d1 2F3.5 2282620.0 cm-1
2s1 2p5 3d1 2F2.5 2285010.0 cm-1
2s1 2p5 3d1 2D1.5 2290770.0 cm-1
2s1 2p5 3d1 2D2.5 2291350.0 cm-1
2s1 2p5 3d1 2P0.5 2304510.0 cm-1
2s1 2p5 3p1 2D1.5 2308370.0 cm-1
2s1 2p5 3d1 2P1.5 2309400.0 cm-1
2s1 2p5 3p1 2D2.5 2309850.0 cm-1
2s1 2p5 3p1 2P0.5 2316520.0 cm-1
2s1 2p5 3p1 2P1.5 2317230.0 cm-1
2s2 2p4 4d1 2D2.5 2323840.0 cm-1
2s2 2p4 4d1 2D1.5 2324170.0 cm-1
2s1 2p5 3p1 2S0.5 2337090.0 cm-1
2s2 2p4 4f1 2F2.5 2339710.0 cm-1
2s2 2p4 4f1 2F3.5 2339750.0 cm-1
2s1 2p5 3d1 2F2.5 2452370.0 cm-1
2s1 2p5 3d1 2F3.5 2452590.0 cm-1
2s1 2p5 3d1 2P1.5 2459700.0 cm-1
2s1 2p5 3d1 2P0.5 2460090.0 cm-1
2s1 2p5 3d1 2D1.5 2462180.0 cm-1
2s1 2p5 3d1 2D2.5 2462340.0 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 = 1.4405
         2S = 1.1886
         2P = 1.1332
         3S = 1.1053
         3P = 1.0575
         3D = 1.0776
         4S = 1.1187
         4P = 1.0655
         4D = 1.0777
         4F = 1.0670

 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 (0.0333347 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (0.666694 eV) was used
 from the last threshold up to 1.473240 Z**2 Rydbergs (982.2 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (0.666694 eV) was used
 from first threshold up to 1.473240 Z**2 Rydbergs (982.2 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
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