This pseudopotential was carried over into the dynamical calculation as the potential holding the single electron to the effective Li + center.
The atomic wavefunctions were obtained by solving the time‐independent Schrödinger equation for a single valence electron in the field of the nucleus plus an exponential inner charge cloud. The rectilinear path impact parameter method was used, and cross sections for populating the various channels were determined over the energy range 0.4–400 keV. Coupled‐state calculations have been performed for the collision processes Li + + Li (2s)→ Li + + Li (nl),→ Li (nl)+ Li +, in which 1, 3, 4, or 6 of the states 2 s, 2 p 0, 2 p 1, 3 s, 3 p 0, 3 p 1 were included on each nuclear center as traveling‐wave atomic orbitals.
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