Resolved Specific Ion Data Collections

Temperature Range
1.103 eV → 1.103 x 104 eV


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  • Spontaneous Emission: Mg+7(i) → Mg+7(j) + hv
  • Electron Impact Excitation: Mg+7(i) + e → Mg+7(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 3302.0 cm-1
2s1 2p2 4P0.5 129885.0 cm-1
2s1 2p2 4P1.5 131026.0 cm-1
2s1 2p2 4P2.5 132705.0 cm-1
2s1 2p2 2D1.5 232274.0 cm-1
2s1 2p2 2D2.5 232307.0 cm-1
2s1 2p2 2S0.5 298282.0 cm-1
2s1 2p2 2P0.5 318721.0 cm-1
2s1 2p2 2P1.5 320723.0 cm-1
2p3 4S1.5 413610.0 cm-1
2p3 2D1.5 465745.0 cm-1
2p3 2D2.5 465818.0 cm-1
2p3 2P0.5 524652.0 cm-1
2p3 2P1.5 524841.0 cm-1
2s2 3s1 2S0.5 1208630.0 cm-1
2s2 3p1 2P0.5 1273570.0 cm-1
2s2 3p1 2P1.5 1274450.0 cm-1
2s2 3d1 2D1.5 1335740.0 cm-1
2s2 3d1 2D2.5 1335980.0 cm-1
2s1 2p1 3s1 4P0.5 1350350.0 cm-1
2s1 2p1 3s1 4P1.5 1351470.0 cm-1
2s1 2p1 3s1 4P2.5 1353400.0 cm-1
2s1 2p1 3s1 2P0.5 1383390.0 cm-1
2s1 2p1 3s1 2P1.5 1385570.0 cm-1
2s1 2p1 3p1 2P0.5 1407520.0 cm-1
2s1 2p1 3p1 2P1.5 1408550.0 cm-1
2s1 2p1 3p1 4D0.5 1410290.0 cm-1
2s1 2p1 3p1 4D1.5 1410830.0 cm-1
2s1 2p1 3p1 4D2.5 1411790.0 cm-1
2s1 2p1 3p1 4D3.5 1413490.0 cm-1
2s1 2p1 3p1 4S1.5 1423490.0 cm-1
2s1 2p1 3p1 4P0.5 1431030.0 cm-1
2s1 2p1 3p1 4P1.5 1431910.0 cm-1
2s1 2p1 3p1 4P2.5 1433010.0 cm-1
2s1 2p1 3p1 2D1.5 1441630.0 cm-1
2s1 2p1 3p1 2D2.5 1443620.0 cm-1
2s1 2p1 3p1 2S0.5 1463170.0 cm-1
2s1 2p1 3d1 4F1.5 1463960.0 cm-1
2s1 2p1 3d1 4F2.5 1464610.0 cm-1
2s1 2p1 3d1 4F3.5 1465540.0 cm-1
2s1 2p1 3d1 4F4.5 1466800.0 cm-1
2s1 2p1 3d1 4D0.5 1479550.0 cm-1
2s1 2p1 3d1 4D1.5 1479700.0 cm-1
2s1 2p1 3d1 4D2.5 1480010.0 cm-1
2s1 2p1 3d1 4D3.5 1480790.0 cm-1
2s1 2p1 3d1 2D1.5 1482620.0 cm-1
2s1 2p1 3d1 2D2.5 1482880.0 cm-1
2s1 2p1 3d1 4P2.5 1485810.0 cm-1
2s1 2p1 3d1 4P1.5 1486330.0 cm-1
2s1 2p1 3d1 4P0.5 1486680.0 cm-1
2s1 2p1 3s1 2P0.5 1493910.0 cm-1
2s1 2p1 3s1 2P1.5 1493980.0 cm-1
2s1 2p1 3d1 2F2.5 1513100.0 cm-1
2s1 2p1 3d1 2F3.5 1515040.0 cm-1
2s1 2p1 3d1 2P1.5 1520230.0 cm-1
2s1 2p1 3d1 2P0.5 1521330.0 cm-1
2s1 2p1 3p1 2P0.5 1557530.0 cm-1
2s1 2p1 3p1 2P1.5 1558090.0 cm-1
2s1 2p1 3p1 2D1.5 1558980.0 cm-1
2s1 2p1 3p1 2D2.5 1559150.0 cm-1
2s1 2p1 3p1 2S0.5 1572200.0 cm-1
2p2 3s1 4P0.5 1592610.0 cm-1
2p2 3s1 4P1.5 1593770.0 cm-1
2p2 3s1 4P2.5 1595640.0 cm-1
2s1 2p1 3d1 2F3.5 1611810.0 cm-1
2s1 2p1 3d1 2F2.5 1611840.0 cm-1
2s1 2p1 3d1 2D1.5 1622030.0 cm-1
2s1 2p1 3d1 2D2.5 1622370.0 cm-1
2p2 3s1 2P0.5 1628200.0 cm-1
2p2 3s1 2P1.5 1630310.0 cm-1
2s1 2p1 3d1 2P0.5 1632620.0 cm-1
2s1 2p1 3d1 2P1.5 1632920.0 cm-1
2p2 3p1 2S0.5 1636110.0 cm-1
2p2 3p1 4D0.5 1646240.0 cm-1
2p2 3p1 4D1.5 1646950.0 cm-1
2p2 3s1 2D1.5 1647650.0 cm-1
2p2 3s1 2D2.5 1647680.0 cm-1
2p2 3p1 4D2.5 1648130.0 cm-1
2p2 3p1 4D3.5 1649790.0 cm-1
2s2 4s1 2S0.5 1653110.0 cm-1
2p2 3p1 4P0.5 1654800.0 cm-1
2p2 3p1 4P1.5 1655390.0 cm-1
2p2 3p1 4P2.5 1656480.0 cm-1
2p2 3p1 2D1.5 1664580.0 cm-1
2p2 3p1 2D2.5 1666670.0 cm-1
2s2 4p1 2P0.5 1677410.0 cm-1
2s2 4p1 2P1.5 1677740.0 cm-1
2p2 3p1 2P1.5 1680810.0 cm-1
2p2 3p1 2P0.5 1680990.0 cm-1
2p2 3p1 4S1.5 1685610.0 cm-1
2p2 3d1 4F1.5 1694370.0 cm-1
2p2 3d1 4F2.5 1695010.0 cm-1
2p2 3d1 4F3.5 1695930.0 cm-1
2p2 3d1 4F4.5 1697150.0 cm-1
2s2 4d1 2D1.5 1697770.0 cm-1
2s2 4d1 2D2.5 1697870.0 cm-1
2p2 3p1 2F2.5 1701640.0 cm-1
2p2 3p1 2F3.5 1702260.0 cm-1
2p2 3d1 4D0.5 1706410.0 cm-1
2p2 3d1 4D1.5 1706540.0 cm-1
2p2 3d1 4D2.5 1707190.0 cm-1
2p2 3d1 4D3.5 1707660.0 cm-1
2p2 3d1 2P1.5 1708380.0 cm-1
2p2 3d1 2P0.5 1710220.0 cm-1
2s2 4f1 2F2.5 1712660.0 cm-1
2p2 3d1 2F2.5 1712680.0 cm-1
2s2 4f1 2F3.5 1712770.0 cm-1
2p2 3d1 2F3.5 1714900.0 cm-1
2p2 3d1 4P2.5 1723150.0 cm-1
2p2 3d1 4P1.5 1723910.0 cm-1
2p2 3d1 4P0.5 1724340.0 cm-1
2p2 3p1 2D2.5 1726570.0 cm-1
2p2 3p1 2D1.5 1726650.0 cm-1
2p2 3s1 2S0.5 1739200.0 cm-1
2p2 3p1 2P0.5 1739720.0 cm-1
2p2 3p1 2P1.5 1741010.0 cm-1
2p2 3d1 2G3.5 1749780.0 cm-1
2p2 3d1 2D1.5 1749950.0 cm-1
2p2 3d1 2G4.5 1750020.0 cm-1
2p2 3d1 2D2.5 1750070.0 cm-1
2p2 3d1 2D1.5 1765140.0 cm-1
2p2 3d1 2D2.5 1765730.0 cm-1
2p2 3d1 2F3.5 1766800.0 cm-1
2p2 3d1 2F2.5 1767560.0 cm-1
2p2 3d1 2P0.5 1781500.0 cm-1
2p2 3d1 2P1.5 1782310.0 cm-1
2p2 3d1 2S0.5 1790130.0 cm-1
2s1 2p1 4s1 4P0.5 1793010.0 cm-1
2s1 2p1 4s1 4P1.5 1794060.0 cm-1
2s1 2p1 4s1 4P2.5 1795940.0 cm-1
2p2 3p1 2P0.5 1803420.0 cm-1
2p2 3p1 2P1.5 1804120.0 cm-1
2s1 2p1 4s1 2P0.5 1807310.0 cm-1
2s1 2p1 4s1 2P1.5 1809070.0 cm-1
2s1 2p1 4p1 4D0.5 1816400.0 cm-1
2s1 2p1 4p1 4D1.5 1817030.0 cm-1
2s1 2p1 4p1 4D2.5 1818060.0 cm-1
2s1 2p1 4p1 4D3.5 1819580.0 cm-1
2s1 2p1 4p1 2P0.5 1820400.0 cm-1
2s1 2p1 4p1 2P1.5 1820610.0 cm-1
2s1 2p1 4p1 4S1.5 1822130.0 cm-1
2s1 2p1 4p1 4P0.5 1824050.0 cm-1
2s1 2p1 4p1 4P1.5 1825070.0 cm-1
2s1 2p1 4p1 4P2.5 1825730.0 cm-1
2s1 2p1 4p1 2D1.5 1830890.0 cm-1
2s1 2p1 4p1 2D2.5 1832670.0 cm-1
2s1 2p1 4d1 4F1.5 1835890.0 cm-1
2s1 2p1 4d1 4F2.5 1836470.0 cm-1
2s1 2p1 4d1 4F3.5 1837350.0 cm-1
2s1 2p1 4d1 4F4.5 1838650.0 cm-1
2s1 2p1 4p1 2S0.5 1840810.0 cm-1
2s1 2p1 4d1 4D1.5 1841710.0 cm-1
2s1 2p1 4d1 4D2.5 1841710.0 cm-1
2s1 2p1 4d1 4D0.5 1841720.0 cm-1
2s1 2p1 4d1 4D3.5 1842990.0 cm-1
2s1 2p1 4d1 2D1.5 1844000.0 cm-1
2s1 2p1 4d1 4P2.5 1844020.0 cm-1
2s1 2p1 4d1 4P1.5 1844840.0 cm-1
2s1 2p1 4d1 2D2.5 1844920.0 cm-1
2s1 2p1 4d1 4P0.5 1845070.0 cm-1
2p2 3d1 2D2.5 1850210.0 cm-1
2p2 3d1 2D1.5 1850560.0 cm-1
2s1 2p1 4f1 4F2.5 1851510.0 cm-1
2s1 2p1 4f1 4F3.5 1851550.0 cm-1
2s1 2p1 4f1 4F1.5 1852080.0 cm-1
2s1 2p1 4f1 4F4.5 1852160.0 cm-1
2s1 2p1 4f1 4G2.5 1852720.0 cm-1
2s1 2p1 4f1 4G3.5 1853370.0 cm-1
2s1 2p1 4f1 2G3.5 1854030.0 cm-1
2s1 2p1 4f1 4G4.5 1854340.0 cm-1
2s1 2p1 4f1 4G5.5 1854840.0 cm-1
2s1 2p1 4f1 2F2.5 1855050.0 cm-1
2s1 2p1 4d1 2F2.5 1855110.0 cm-1
2s1 2p1 4f1 4D3.5 1855750.0 cm-1
2s1 2p1 4f1 2G4.5 1856350.0 cm-1
2s1 2p1 4f1 2F3.5 1856630.0 cm-1
2s1 2p1 4d1 2F3.5 1856820.0 cm-1
2s1 2p1 4f1 4D2.5 1856820.0 cm-1
2s1 2p1 4f1 4D1.5 1857270.0 cm-1
2s1 2p1 4d1 2P1.5 1857460.0 cm-1
2s1 2p1 4f1 4D0.5 1857530.0 cm-1
2s1 2p1 4d1 2P0.5 1858530.0 cm-1
2s1 2p1 4f1 2D2.5 1860820.0 cm-1
2s1 2p1 4f1 2D1.5 1861770.0 cm-1
2s1 2p1 4s1 2P0.5 1934540.0 cm-1
2s1 2p1 4s1 2P1.5 1934620.0 cm-1
2s1 2p1 4p1 2D1.5 1958170.0 cm-1
2s1 2p1 4p1 2D2.5 1958350.0 cm-1
2s1 2p1 4p1 2P0.5 1959830.0 cm-1
2s1 2p1 4p1 2P1.5 1960100.0 cm-1
2s1 2p1 4p1 2S0.5 1964800.0 cm-1
2s1 2p1 4d1 2F3.5 1979130.0 cm-1
2s1 2p1 4d1 2F2.5 1979140.0 cm-1
2s1 2p1 4d1 2D1.5 1980250.0 cm-1
2s1 2p1 4d1 2D2.5 1980370.0 cm-1
2s1 2p1 4d1 2P0.5 1985430.0 cm-1
2s1 2p1 4d1 2P1.5 1985540.0 cm-1
2s1 2p1 4f1 2F2.5 1988460.0 cm-1
2s1 2p1 4f1 2F3.5 1988500.0 cm-1
2s1 2p1 4f1 2G3.5 1992630.0 cm-1
2s1 2p1 4f1 2G4.5 1992680.0 cm-1
2s1 2p1 4f1 2D1.5 1996430.0 cm-1
2s1 2p1 4f1 2D2.5 1996460.0 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 = 1.39554
         2S = 1.24527
         2P = 1.17189
         3S = 1.62232
         3P = 1.35422
         3D = 1.46091
         4S = 1.38464
         4P = 1.31611
         4D = 1.53481
         4F = 0.57992

 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 220.8441 Rydbergs (3004.804825 eV)

 A fine energy mesh of 0.000005 Z**2 Rydbergs (0.00333347 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 1.196771 Z**2 Rydbergs (797.88 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 1.196771 Z**2 Rydbergs (797.88 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:        23/05/12

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

 Date:  Tue May 28 20:45:13 2013


  • Guiyun Liang
  • Nigel Badnell
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