Resolved Specific Ion Data Collections

Temperature Range
1.396 eV → 1.396 x 104 eV


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  • Spontaneous Emission: Al+8(i) → Al+8(j) + hv
  • Electron Impact Excitation: Al+8(i) + e → Al+8(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 4894.3 cm-1
2s1 2p2 4P0.5 145270.0 cm-1
2s1 2p2 4P1.5 146993.0 cm-1
2s1 2p2 4P2.5 149462.0 cm-1
2s1 2p2 2D1.5 259726.0 cm-1
2s1 2p2 2D2.5 259759.0 cm-1
2s1 2p2 2S0.5 332713.0 cm-1
2s1 2p2 2P0.5 354078.0 cm-1
2s1 2p2 2P1.5 356954.0 cm-1
2p3 4S1.5 460930.0 cm-1
2p3 2D1.5 520078.0 cm-1
2p3 2D2.5 520144.0 cm-1
2p3 2P0.5 585185.0 cm-1
2p3 2P1.5 585536.0 cm-1
2s2 3s1 2S0.5 1499140.0 cm-1
2s2 3p1 2P0.5 1572100.0 cm-1
2s2 3p1 2P1.5 1573420.0 cm-1
2s2 3d1 2D1.5 1642370.0 cm-1
2s2 3d1 2D2.5 1642750.0 cm-1
2s1 2p1 3s1 4P0.5 1655700.0 cm-1
2s1 2p1 3s1 4P1.5 1657340.0 cm-1
2s1 2p1 3s1 4P2.5 1660220.0 cm-1
2s1 2p1 3s1 2P0.5 1692740.0 cm-1
2s1 2p1 3s1 2P1.5 1695970.0 cm-1
2s1 2p1 3p1 2P0.5 1720340.0 cm-1
2s1 2p1 3p1 2P1.5 1721890.0 cm-1
2s1 2p1 3p1 4D0.5 1723610.0 cm-1
2s1 2p1 3p1 4D1.5 1724330.0 cm-1
2s1 2p1 3p1 4D2.5 1725580.0 cm-1
2s1 2p1 3p1 4D3.5 1728100.0 cm-1
2s1 2p1 3p1 4S1.5 1738740.0 cm-1
2s1 2p1 3p1 4P0.5 1746960.0 cm-1
2s1 2p1 3p1 4P1.5 1748320.0 cm-1
2s1 2p1 3p1 4P2.5 1749900.0 cm-1
2s1 2p1 3p1 2D1.5 1758750.0 cm-1
2s1 2p1 3p1 2D2.5 1761710.0 cm-1
2s1 2p1 3d1 4F1.5 1783250.0 cm-1
2s1 2p1 3p1 2S0.5 1783340.0 cm-1
2s1 2p1 3d1 4F2.5 1784220.0 cm-1
2s1 2p1 3d1 4F3.5 1785610.0 cm-1
2s1 2p1 3d1 4F4.5 1787500.0 cm-1
2s1 2p1 3d1 4D0.5 1801560.0 cm-1
2s1 2p1 3d1 4D1.5 1801740.0 cm-1
2s1 2p1 3d1 4D2.5 1802130.0 cm-1
2s1 2p1 3d1 4D3.5 1803460.0 cm-1
2s1 2p1 3d1 2D1.5 1804930.0 cm-1
2s1 2p1 3d1 2D2.5 1805300.0 cm-1
2s1 2p1 3d1 4P2.5 1808870.0 cm-1
2s1 2p1 3d1 4P1.5 1809540.0 cm-1
2s1 2p1 3d1 4P0.5 1810010.0 cm-1
2s1 2p1 3s1 2P0.5 1813950.0 cm-1
2s1 2p1 3s1 2P1.5 1814080.0 cm-1
2s1 2p1 3d1 2F2.5 1839900.0 cm-1
2s1 2p1 3d1 2F3.5 1842790.0 cm-1
2s1 2p1 3d1 2P1.5 1848000.0 cm-1
2s1 2p1 3d1 2P0.5 1849640.0 cm-1
2s1 2p1 3p1 2P0.5 1885350.0 cm-1
2s1 2p1 3p1 2P1.5 1886170.0 cm-1
2s1 2p1 3p1 2D1.5 1887410.0 cm-1
2s1 2p1 3p1 2D2.5 1887620.0 cm-1
2s1 2p1 3p1 2S0.5 1903880.0 cm-1
2p2 3s1 4P0.5 1923870.0 cm-1
2p2 3s1 4P1.5 1925580.0 cm-1
2p2 3s1 4P2.5 1928320.0 cm-1
2s1 2p1 3d1 2F3.5 1947940.0 cm-1
2s1 2p1 3d1 2F2.5 1948000.0 cm-1
2s1 2p1 3d1 2D1.5 1958290.0 cm-1
2s1 2p1 3d1 2D2.5 1958800.0 cm-1
2p2 3s1 2P0.5 1964110.0 cm-1
2p2 3s1 2P1.5 1967170.0 cm-1
2s1 2p1 3d1 2P0.5 1971150.0 cm-1
2s1 2p1 3d1 2P1.5 1971620.0 cm-1
2p2 3p1 2S0.5 1973650.0 cm-1
2p2 3p1 4D0.5 1984210.0 cm-1
2p2 3p1 4D1.5 1985270.0 cm-1
2p2 3s1 2D2.5 1985950.0 cm-1
2p2 3s1 2D1.5 1985960.0 cm-1
2p2 3p1 4D2.5 1987030.0 cm-1
2p2 3p1 4D3.5 1989490.0 cm-1
2p2 3p1 4P0.5 1994360.0 cm-1
2p2 3p1 4P1.5 1995160.0 cm-1
2p2 3p1 4P2.5 1996730.0 cm-1
2p2 3p1 2D1.5 2005020.0 cm-1
2p2 3p1 2D2.5 2008170.0 cm-1
2p2 3p1 2P1.5 2023130.0 cm-1
2p2 3p1 2P0.5 2023480.0 cm-1
2p2 3p1 4S1.5 2028410.0 cm-1
2p2 3d1 4F1.5 2038790.0 cm-1
2p2 3d1 4F2.5 2039740.0 cm-1
2p2 3d1 4F3.5 2041120.0 cm-1
2p2 3d1 4F4.5 2042950.0 cm-1
2s2 4s1 2S0.5 2046060.0 cm-1
2p2 3p1 2F2.5 2047910.0 cm-1
2p2 3p1 2F3.5 2048930.0 cm-1
2p2 3d1 4D0.5 2052570.0 cm-1
2p2 3d1 4D1.5 2052660.0 cm-1
2p2 3d1 4D2.5 2053750.0 cm-1
2p2 3d1 4D3.5 2054450.0 cm-1
2p2 3d1 2P1.5 2055010.0 cm-1
2p2 3d1 2P0.5 2057650.0 cm-1
2p2 3d1 2F2.5 2059720.0 cm-1
2p2 3d1 2F3.5 2063050.0 cm-1
2p2 3d1 4P2.5 2071770.0 cm-1
2p2 3d1 4P1.5 2072890.0 cm-1
2p2 3d1 4P0.5 2073510.0 cm-1
2p2 3p1 2D2.5 2074240.0 cm-1
2p2 3p1 2D1.5 2074280.0 cm-1
2s2 4p1 2P0.5 2074360.0 cm-1
2s2 4p1 2P1.5 2074940.0 cm-1
2p2 3s1 2S0.5 2087050.0 cm-1
2p2 3p1 2P0.5 2089940.0 cm-1
2p2 3p1 2P1.5 2091880.0 cm-1
2s2 4d1 2D1.5 2097910.0 cm-1
2s2 4d1 2D2.5 2098000.0 cm-1
2p2 3d1 2G3.5 2101230.0 cm-1
2p2 3d1 2G4.5 2101610.0 cm-1
2p2 3d1 2D1.5 2103370.0 cm-1
2p2 3d1 2D2.5 2103480.0 cm-1
2s2 4f1 2F2.5 2112980.0 cm-1
2s2 4f1 2F3.5 2113040.0 cm-1
2p2 3d1 2D1.5 2118640.0 cm-1
2p2 3d1 2D2.5 2119800.0 cm-1
2p2 3d1 2F3.5 2122130.0 cm-1
2p2 3d1 2F2.5 2123170.0 cm-1
2p2 3d1 2P0.5 2137080.0 cm-1
2p2 3d1 2P1.5 2138320.0 cm-1
2p2 3d1 2S0.5 2146430.0 cm-1
2p2 3p1 2P0.5 2159750.0 cm-1
2p2 3p1 2P1.5 2160290.0 cm-1
2s1 2p1 4s1 4P0.5 2201620.0 cm-1
2s1 2p1 4s1 4P1.5 2203160.0 cm-1
2s1 2p1 4s1 4P2.5 2205980.0 cm-1
2p2 3d1 2D2.5 2214710.0 cm-1
2p2 3d1 2D1.5 2215210.0 cm-1
2s1 2p1 4s1 2P0.5 2216030.0 cm-1
2s1 2p1 4s1 2P1.5 2219220.0 cm-1
2s1 2p1 4p1 4D0.5 2228060.0 cm-1
2s1 2p1 4p1 4D1.5 2229030.0 cm-1
2s1 2p1 4p1 4D2.5 2230580.0 cm-1
2s1 2p1 4p1 2P0.5 2232630.0 cm-1
2s1 2p1 4p1 4D3.5 2232880.0 cm-1
2s1 2p1 4p1 2P1.5 2232990.0 cm-1
2s1 2p1 4p1 4S1.5 2235380.0 cm-1
2s1 2p1 4p1 4P0.5 2237120.0 cm-1
2s1 2p1 4p1 4P1.5 2238810.0 cm-1
2s1 2p1 4p1 4P2.5 2239660.0 cm-1
2s1 2p1 4p1 2D1.5 2244590.0 cm-1
2s1 2p1 4p1 2D2.5 2247200.0 cm-1
2s1 2p1 4d1 4F1.5 2250510.0 cm-1
2s1 2p1 4d1 4F2.5 2251360.0 cm-1
2s1 2p1 4d1 4F3.5 2252650.0 cm-1
2s1 2p1 4d1 4F4.5 2254670.0 cm-1
2s1 2p1 4p1 2S0.5 2256060.0 cm-1
2s1 2p1 4d1 4D2.5 2257230.0 cm-1
2s1 2p1 4d1 4D1.5 2257350.0 cm-1
2s1 2p1 4d1 4D0.5 2257410.0 cm-1
2s1 2p1 4d1 4D3.5 2259390.0 cm-1
2s1 2p1 4d1 2D1.5 2259970.0 cm-1
2s1 2p1 4d1 4P2.5 2260380.0 cm-1
2s1 2p1 4d1 2D2.5 2261430.0 cm-1
2s1 2p1 4d1 4P1.5 2261560.0 cm-1
2s1 2p1 4d1 4P0.5 2261870.0 cm-1
2s1 2p1 4f1 4F2.5 2268100.0 cm-1
2s1 2p1 4f1 4F3.5 2268210.0 cm-1
2s1 2p1 4f1 4F1.5 2268870.0 cm-1
2s1 2p1 4f1 4F4.5 2269170.0 cm-1
2s1 2p1 4f1 4G2.5 2269800.0 cm-1
2s1 2p1 4f1 4G3.5 2270570.0 cm-1
2s1 2p1 4f1 2G3.5 2271240.0 cm-1
2s1 2p1 4f1 2F2.5 2271720.0 cm-1
2s1 2p1 4d1 2F2.5 2272370.0 cm-1
2s1 2p1 4f1 4G4.5 2272430.0 cm-1
2s1 2p1 4f1 4G5.5 2273190.0 cm-1
2s1 2p1 4f1 2F3.5 2273590.0 cm-1
2s1 2p1 4f1 4D3.5 2274590.0 cm-1
2s1 2p1 4d1 2F3.5 2274880.0 cm-1
2s1 2p1 4f1 4D2.5 2274900.0 cm-1
2s1 2p1 4f1 2G4.5 2274960.0 cm-1
2s1 2p1 4d1 2P1.5 2275180.0 cm-1
2s1 2p1 4f1 4D1.5 2275590.0 cm-1
2s1 2p1 4f1 4D0.5 2275980.0 cm-1
2s1 2p1 4d1 2P0.5 2276730.0 cm-1
2s1 2p1 4f1 2D2.5 2277450.0 cm-1
2s1 2p1 4f1 2D1.5 2278710.0 cm-1
2s1 2p1 4s1 2P0.5 2357520.0 cm-1
2s1 2p1 4s1 2P1.5 2357620.0 cm-1
2s1 2p1 4p1 2D1.5 2384450.0 cm-1
2s1 2p1 4p1 2D2.5 2384740.0 cm-1
2s1 2p1 4p1 2P0.5 2386240.0 cm-1
2s1 2p1 4p1 2P1.5 2386670.0 cm-1
2s1 2p1 4p1 2S0.5 2391930.0 cm-1
2s1 2p1 4d1 2F3.5 2408440.0 cm-1
2s1 2p1 4d1 2F2.5 2408460.0 cm-1
2s1 2p1 4d1 2D1.5 2409610.0 cm-1
2s1 2p1 4d1 2D2.5 2409800.0 cm-1
2s1 2p1 4d1 2P0.5 2415410.0 cm-1
2s1 2p1 4d1 2P1.5 2415570.0 cm-1
2s1 2p1 4f1 2F2.5 2419090.0 cm-1
2s1 2p1 4f1 2F3.5 2419160.0 cm-1
2s1 2p1 4f1 2G3.5 2423700.0 cm-1
2s1 2p1 4f1 2G4.5 2423770.0 cm-1
2s1 2p1 4f1 2D1.5 2427440.0 cm-1
2s1 2p1 4f1 2D2.5 2427490.0 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 = 1.39331
         2S = 1.24606
         2P = 1.17194
         3S = 1.61707
         3P = 1.35664
         3D = 1.46554
         4S = 1.44070
         4P = 1.35498
         4D = 1.51784
         4F = 1.12328

 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 276.5179 Rydbergs (3762.302547 eV)

 A fine energy mesh of 0.000010 Z**2 Rydbergs (0.00870784 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (0.870784 eV) was used
 from the last threshold up to 1.183072 Z**2 Rydbergs (1030.2 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (0.870784 eV) was used
 from first threshold up to 1.183072 Z**2 Rydbergs (1030.2 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

      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:        13/05/12

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

 Produced by: Guiyun Liang
 Date:        28/05/2013



  • Guiyun Liang
  • Nigel Badnell
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