Abstract
Cross-section formulas for large-angle (e,e) and for coincidence (e,2e) scattering of fast electrons from gaseous and solid targets are derived. It is shown that the momentum and spin-density distribution of the bound electrons can be obtained from single (e,e) scattering of polarized electrons. It is also shown that the electronic spin- and energy-dependent momentum-density distribution can be obtained from (e,2e) scattering of polarized electrons. An (e,2e) experiment with unpolarized electrons gives the energy-dependent momentum distribution. A comparison is made with related methods, like Compton scattering, and the feasibility of the suggested experiments is discussed.