Resolved Specific Ion Data Collections

Temperature Range
0.086 eV → 8.617 eV


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  • Spontaneous Emission: Li+0(i) → Li+0(j) + hv
  • Electron Impact Excitation: Li+0(i) + e → Li+0(j) + e
1s2 2s1 2S0.5 0.0 cm-1
1s2 2p1 2P2.5 14850.0 cm-1
1s2 3s1 2S0.5 26890.0 cm-1
1s2 3p1 2P2.5 30626.0 cm-1
1s2 3d1 2D4.5 30893.0 cm-1
1s2 4s1 2S0.5 34643.0 cm-1
1s2 4p1 2P2.5 36112.0 cm-1
1s2 4d1 2D4.5 36228.0 cm-1
1s2 4f1 2F6.5 36229.0 cm-1

        For more information see: D. C. Griffin, D. M. Mitnik, J. Colgan,
        and M. S. Pindzola, Phys. Rev. A 64 032718 (2001)

        From a 55-state R-matrix with pseudo-state (RMPS) calculation

        The 1s and 2s orbitals were determined from a Hartree-Fock (HF)
        calculation on 1s22s.  The 2p, 3s, 3p, 3d, 4s, 4p, 4d, and 4f
        orbitals were determined from a frozen-core HF calculation on
        1s2nl.  In addition, we generated 1s2nl pseudo states for:
        ns with n=6 to 15, np with n=6 to 14, nd with n=6 to 13, nf with
        n=6 to 12, and ng with n=6 to 12 using Laguerre orbitals.  These
        were used to represent the target continuum as well as the highly
        excited Rydberg states.

        For the RMPS calculation with exchange, all partial LSPI partial
        waves from L = 0 to L = 9 were included.  This was then extended
        to higher L values by adding to it the results of a no-exchange
        9-state R-matrix calculation from L=10 to L=60 with top up.  The
        size of the continuum basis for these calculations was 36 and the
        size of the R-matrix box was 77.3 au.

        Donald C. Griffin                 December, 18 2001




  • Connor Ballance
  • Don Griffin
  • James Colgan
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