Deformation des Thomas-Fermischen Atommodells durch nicht-kugelsymmetrische Potentialfelder
The conditions will be deduced for the exact solution of the Thomas-Fermi-equation for an atom or ion, which is deformed by non-spherical fields. A numerical method for the solution of the associated integral equation will be shown. Explicite calculations have been performed for the polarizability of some ions and for the energy required to bring an electron by steps from inside the model to infinity.