lilike_cpb02#li0.dat

• Spontaneous Emission: Li⁺⁰(i) → Li⁺⁰(j) + hv
• Electron Impact Excitation: Li⁺⁰(i) + e → Li⁺⁰(j) + e

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        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

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Dependents

• ADF04 cpb02_ls#li0.dat

Contributors

• Connor Ballance
• Don Griffin
• James Colgan