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B+H (s.1)} (11.45) mic m*C r dr where L = m(r,x v) is the electron's orbital angular
momentum. This interaction energy gives the anomalous Zeeman effect correctly,
but has a spin-orbit interaction which is twice too large. The error in (11.45) can ...
We will begin by considering the simple problem of energy transfer to a free
electron by a fast heavy particle. Then the effects of a binding force on the
electron are explored, and the classical Bohr formula for energy loss is obtained.
For simplicity we will consider the so-called Lorentz gas, which consists of N fixed
ions of charge Ze per unit volume and NZ free electrons per unit volume.
Furthermore electron-electron interactions will be ignored. The approximation of
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Introduction to Electrostatics
BoundaryValue Problems in Electrostatics I
BoundaryValue Problems in Electrostatics II
16 other sections not shown