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most. +*H*). +:[1-(*#")||1-(**)]"co,. q249. where E' is given by (12.31). To obtain E,
we merely interchange ms and m, and change 0' into T – 6' (cos 0' → —cos 0').
The relation between angles 6' and 62 can be obtained from the expression ...
The Fermi expression (13.70) bears little resemblance to our previous results for
energy loss, such as (13.35). But under conditions where polarization effects are
unimportant it yields the same results as before. For example, for nonrelativistic ...
where we have used the dipole moment expression (13.19). Assuming that the
second term is small, the imaginary part of 1/e(a) can be readily calculated and
substituted into (13.70). Then the integral over do can be performed in the same ...
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Introduction to Electrostatics
BoundaryValue Problems in Electrostatics I
BoundaryValue Problems in Electrostatics II
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