flike_mcw06#p6.dat

Resolved Specific Ion Data Collections

Ion
P6+
Temperature Range
0.844 eV → 8444 eV

ADF04

Filename
flike_mcw06#p6.dat
Full Path
adf04/copaw#f/flike_mcw06#p6.dat
Download data
  • Spontaneous Emission: P+6(i) → P+6(j) + hv
  • Electron Impact Excitation: P+6(i) + e → P+6(j) + e
2s2 2p5 2P1.5 0.0 cm-1
2s2 2p5 2P0.5 7767.0 cm-1
2s1 2p6 2S0.5 475284.0 cm-1
2s2 2p4 3s1 4P2.5 1245300.0 cm-1
2s2 2p4 3s1 4P1.5 1249610.0 cm-1
2s2 2p4 3s1 4P0.5 1252260.0 cm-1
2s2 2p4 3s1 2P1.5 1263830.0 cm-1
2s2 2p4 3s1 2P0.5 1269000.0 cm-1
2s2 2p4 3s1 2D2.5 1305000.0 cm-1
2s2 2p4 3s1 2D1.5 1305080.0 cm-1
2s2 2p4 3p1 4P2.5 1336510.0 cm-1
2s2 2p4 3p1 4P1.5 1337890.0 cm-1
2s2 2p4 3p1 4P0.5 1339750.0 cm-1
2s2 2p4 3p1 4D3.5 1348480.0 cm-1
2s2 2p4 3p1 4D2.5 1350900.0 cm-1
2s2 2p4 3p1 4D1.5 1353090.0 cm-1
2s2 2p4 3p1 4D0.5 1354210.0 cm-1
2s2 2p4 3p1 2D2.5 1358450.0 cm-1
2s2 2p4 3p1 2P0.5 1361680.0 cm-1
2s2 2p4 3p1 2D1.5 1362380.0 cm-1
2s2 2p4 3p1 2P1.5 1365850.0 cm-1
2s2 2p4 3p1 4S1.5 1366800.0 cm-1
2s2 2p4 3p1 2S0.5 1368280.0 cm-1
2s2 2p4 3s1 2S0.5 1380440.0 cm-1
2s2 2p4 3p1 2F2.5 1400540.0 cm-1
2s2 2p4 3p1 2F3.5 1401480.0 cm-1
2s2 2p4 3p1 2D1.5 1412870.0 cm-1
2s2 2p4 3p1 2D2.5 1413490.0 cm-1
2s2 2p4 3p1 2P1.5 1439490.0 cm-1
2s2 2p4 3p1 2P0.5 1442860.0 cm-1
2s2 2p4 3d1 4D3.5 1467670.0 cm-1
2s2 2p4 3d1 4D2.5 1468220.0 cm-1
2s2 2p4 3d1 4D1.5 1469070.0 cm-1
2s2 2p4 3d1 4D0.5 1469880.0 cm-1
2s2 2p4 3d1 4F4.5 1478800.0 cm-1
2s2 2p4 3d1 4F3.5 1481220.0 cm-1
2s2 2p4 3d1 4F2.5 1483440.0 cm-1
2s2 2p4 3d1 4P0.5 1484500.0 cm-1
2s2 2p4 3d1 4F1.5 1484860.0 cm-1
2s2 2p4 3p1 2P1.5 1484990.0 cm-1
2s2 2p4 3p1 2P0.5 1485590.0 cm-1
2s2 2p4 3d1 4P1.5 1486150.0 cm-1
2s2 2p4 3d1 2F3.5 1486900.0 cm-1
2s2 2p4 3d1 4P2.5 1488360.0 cm-1
2s2 2p4 3d1 2F2.5 1490490.0 cm-1
2s2 2p4 3d1 2P0.5 1493030.0 cm-1
2s2 2p4 3d1 2D1.5 1494850.0 cm-1
2s2 2p4 3d1 2D2.5 1498320.0 cm-1
2s2 2p4 3d1 2P1.5 1499290.0 cm-1
2s2 2p4 3d1 2G3.5 1528690.0 cm-1
2s2 2p4 3d1 2G4.5 1528880.0 cm-1
2s2 2p4 3d1 2S0.5 1538060.0 cm-1
2s2 2p4 3d1 2F2.5 1540630.0 cm-1
2s2 2p4 3d1 2F3.5 1541170.0 cm-1
2s2 2p4 3d1 2P1.5 1541260.0 cm-1
2s2 2p4 3d1 2P0.5 1543590.0 cm-1
2s2 2p4 3d1 2D2.5 1543780.0 cm-1
2s2 2p4 3d1 2D1.5 1545750.0 cm-1
2s2 2p4 3d1 2D2.5 1612580.0 cm-1
2s2 2p4 3d1 2D1.5 1613000.0 cm-1
2s1 2p5 3s1 4P2.5 1662140.0 cm-1
2s1 2p5 3s1 4P1.5 1666180.0 cm-1
2s1 2p5 3s1 4P0.5 1668900.0 cm-1
2s2 2p4 4s1 4P2.5 1672490.0 cm-1
2s2 2p4 4s1 4P1.5 1675880.0 cm-1
2s2 2p4 4s1 4P0.5 1679300.0 cm-1
2s2 2p4 4s1 2P1.5 1680600.0 cm-1
2s2 2p4 4s1 2P0.5 1684940.0 cm-1
2s1 2p5 3s1 2P1.5 1690630.0 cm-1
2s1 2p5 3s1 2P0.5 1695480.0 cm-1
2s2 2p4 4p1 4P2.5 1711380.0 cm-1
2s2 2p4 4p1 4D3.5 1711660.0 cm-1
2s2 2p4 4p1 4P1.5 1712660.0 cm-1
2s2 2p4 4p1 2D2.5 1713570.0 cm-1
2s2 2p4 4p1 4P0.5 1714970.0 cm-1
2s2 2p4 4p1 4D1.5 1716700.0 cm-1
2s2 2p4 4p1 4D2.5 1717970.0 cm-1
2s2 2p4 4p1 4D0.5 1718260.0 cm-1
2s2 2p4 4p1 2S0.5 1719460.0 cm-1
2s2 2p4 4p1 2D1.5 1720330.0 cm-1
2s2 2p4 4p1 4S1.5 1720780.0 cm-1
2s2 2p4 4p1 2P1.5 1727820.0 cm-1
2s2 2p4 4p1 2P0.5 1728460.0 cm-1
2s2 2p4 4s1 2D2.5 1728560.0 cm-1
2s2 2p4 4s1 2D1.5 1728590.0 cm-1
2s1 2p5 3p1 4S1.5 1748770.0 cm-1
2s2 2p4 4d1 4D3.5 1753840.0 cm-1
2s2 2p4 4d1 4D2.5 1754390.0 cm-1
2s2 2p4 4d1 4D1.5 1755310.0 cm-1
2s2 2p4 4d1 4D0.5 1756380.0 cm-1
2s2 2p4 4d1 4F4.5 1758140.0 cm-1
2s2 2p4 4d1 4F3.5 1759740.0 cm-1
2s2 2p4 4d1 4P0.5 1760580.0 cm-1
2s2 2p4 4d1 4F2.5 1761940.0 cm-1
2s2 2p4 4d1 4P1.5 1761980.0 cm-1
2s2 2p4 4d1 2F3.5 1762880.0 cm-1
2s2 2p4 4d1 4P2.5 1763800.0 cm-1
2s2 2p4 4d1 4F1.5 1764320.0 cm-1
2s2 2p4 4p1 2F2.5 1764950.0 cm-1
2s1 2p5 3p1 4D3.5 1765130.0 cm-1
2s2 2p4 4p1 2F3.5 1765290.0 cm-1
2s2 2p4 4d1 2F2.5 1765410.0 cm-1
2s2 2p4 4d1 2P0.5 1766540.0 cm-1
2s1 2p5 3p1 4D2.5 1766680.0 cm-1
2s2 2p4 4d1 2D1.5 1766810.0 cm-1
2s1 2p5 3p1 4D1.5 1767930.0 cm-1
2s2 2p4 4d1 2D2.5 1768430.0 cm-1
2s2 2p4 4p1 2D1.5 1768950.0 cm-1
2s2 2p4 4p1 2D2.5 1769200.0 cm-1
2s1 2p5 3p1 4D0.5 1769400.0 cm-1
2s2 2p4 4f1 4F4.5 1771200.0 cm-1
2s2 2p4 4f1 4F3.5 1771220.0 cm-1
2s2 2p4 4d1 2P1.5 1771290.0 cm-1
2s2 2p4 4f1 4F2.5 1771430.0 cm-1
2s2 2p4 4f1 4F1.5 1772000.0 cm-1
2s2 2p4 4f1 2F3.5 1772010.0 cm-1
2s2 2p4 4f1 2F2.5 1772500.0 cm-1
2s2 2p4 4f1 4D0.5 1773300.0 cm-1
2s2 2p4 4f1 4G5.5 1773550.0 cm-1
2s2 2p4 4f1 2D1.5 1773600.0 cm-1
2s2 2p4 4f1 2G4.5 1773630.0 cm-1
2s1 2p5 3p1 4P2.5 1776700.0 cm-1
2s2 2p4 4p1 2P1.5 1776950.0 cm-1
2s2 2p4 4f1 4D1.5 1777460.0 cm-1
2s2 2p4 4f1 4D2.5 1777600.0 cm-1
2s2 2p4 4f1 4G4.5 1778320.0 cm-1
2s2 2p4 4f1 4G3.5 1778440.0 cm-1
2s1 2p5 3p1 4P1.5 1778640.0 cm-1
2s2 2p4 4f1 4D3.5 1778870.0 cm-1
2s2 2p4 4f1 2D2.5 1779130.0 cm-1
2s2 2p4 4p1 2P0.5 1779320.0 cm-1
2s1 2p5 3p1 4P0.5 1779340.0 cm-1
2s1 2p5 3p1 2D2.5 1780520.0 cm-1
2s2 2p4 4f1 2G3.5 1780640.0 cm-1
2s2 2p4 4f1 4G2.5 1780650.0 cm-1
2s1 2p5 3p1 2P1.5 1780810.0 cm-1
2s1 2p5 3p1 2P0.5 1783840.0 cm-1
2s1 2p5 3p1 2D1.5 1784720.0 cm-1
2s2 2p4 4s1 2S0.5 1803100.0 cm-1
2s2 2p4 4d1 2G3.5 1810750.0 cm-1
2s2 2p4 4d1 2G4.5 1810830.0 cm-1
2s2 2p4 4d1 2S0.5 1813130.0 cm-1
2s2 2p4 4d1 2F2.5 1814910.0 cm-1
2s2 2p4 4d1 2F3.5 1815130.0 cm-1
2s2 2p4 4d1 2P1.5 1815440.0 cm-1
2s2 2p4 4d1 2D2.5 1816380.0 cm-1
2s2 2p4 4d1 2P0.5 1816530.0 cm-1
2s2 2p4 4d1 2D1.5 1817230.0 cm-1
2s2 2p4 4f1 2P0.5 1823840.0 cm-1
2s2 2p4 4f1 2P1.5 1823870.0 cm-1
2s2 2p4 4f1 2D2.5 1825740.0 cm-1
2s2 2p4 4f1 2D1.5 1825770.0 cm-1
2s2 2p4 4f1 2H4.5 1826120.0 cm-1
2s2 2p4 4f1 2H5.5 1826150.0 cm-1
2s1 2p5 3p1 2S0.5 1826350.0 cm-1
2s2 2p4 4f1 2F3.5 1827600.0 cm-1
2s2 2p4 4f1 2F2.5 1827610.0 cm-1
2s2 2p4 4f1 2G3.5 1828300.0 cm-1
2s2 2p4 4f1 2G4.5 1828330.0 cm-1
2s2 2p4 4p1 2P1.5 1840720.0 cm-1
2s2 2p4 4p1 2P0.5 1841450.0 cm-1
2s1 2p5 3s1 2P0.5 1847410.0 cm-1
2s1 2p5 3s1 2P1.5 1847840.0 cm-1
2s1 2p5 3d1 4P0.5 1881250.0 cm-1
2s1 2p5 3d1 4P1.5 1882410.0 cm-1
2s1 2p5 3d1 4P2.5 1884500.0 cm-1
2s1 2p5 3d1 4F4.5 1887680.0 cm-1
2s1 2p5 3d1 4F3.5 1889590.0 cm-1
2s2 2p4 4d1 2D2.5 1889700.0 cm-1
2s2 2p4 4d1 2D1.5 1889900.0 cm-1
2s1 2p5 3d1 4F2.5 1891500.0 cm-1
2s1 2p5 3d1 4F1.5 1893180.0 cm-1
2s1 2p5 3d1 4D3.5 1899720.0 cm-1
2s1 2p5 3d1 2F3.5 1902050.0 cm-1
2s1 2p5 3d1 4D2.5 1902230.0 cm-1
2s1 2p5 3d1 4D0.5 1902560.0 cm-1
2s1 2p5 3d1 4D1.5 1902680.0 cm-1
2s2 2p4 4f1 2F2.5 1902680.0 cm-1
2s2 2p4 4f1 2F3.5 1903700.0 cm-1
2s1 2p5 3d1 2F2.5 1904940.0 cm-1
2s1 2p5 3d1 2D1.5 1909920.0 cm-1
2s1 2p5 3d1 2D2.5 1910000.0 cm-1
2s1 2p5 3d1 2P0.5 1921290.0 cm-1
2s1 2p5 3d1 2P1.5 1924740.0 cm-1
2s1 2p5 3p1 2D1.5 1936820.0 cm-1
2s1 2p5 3p1 2D2.5 1937810.0 cm-1
2s1 2p5 3p1 2P0.5 1943310.0 cm-1
2s1 2p5 3p1 2P1.5 1943800.0 cm-1
2s1 2p5 3p1 2S0.5 1960400.0 cm-1
2s1 2p5 3d1 2F2.5 2061590.0 cm-1
2s1 2p5 3d1 2F3.5 2061720.0 cm-1
2s1 2p5 3d1 2P1.5 2067020.0 cm-1
2s1 2p5 3d1 2P0.5 2067260.0 cm-1
2s1 2p5 3d1 2D1.5 2069880.0 cm-1
2s1 2p5 3d1 2D2.5 2069990.0 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 = 1.4453
         2S = 1.1849
         2P = 1.1309
         3S = 1.0999
         3P = 1.0528
         3D = 1.0689
         4S = 1.1127
         4P = 1.0600
         4D = 1.0686
         4F = 1.0543

 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 (0.0244908 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (0.489816 eV) was used
 from the last threshold up to 1.628571 Z**2 Rydbergs (797.7 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (0.489816 eV) was used
 from first threshold up to 1.628571 Z**2 Rydbergs (797.7 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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