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Slow projectiles nonlinear theory

In practice, one uses the Kohn-Sham scheme that consists in solving self-consistently the following one-electron equations [16]  [Pg.232]

The electronic density n(r) is obtained from the sum over occupied states  [Pg.232]

This sum includes a contribution originating from the occupied bound states and another one coming from the integration over the continuum up to [Pg.232]

One can also extract from this calculation the scattering phase shifts S/ for the conduction band. In this respect, a number of physical quantities can be expressed in terms of the phase shifts at the Fermi level which obey, [Pg.233]

At low velocities the stopping power can be written in terms of the transport cross-section at the Fermi level [34]  [Pg.233]


See other pages where Slow projectiles nonlinear theory is mentioned: [Pg.223]    [Pg.232]    [Pg.223]    [Pg.232]    [Pg.232]    [Pg.233]   


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