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For ka > 1 , the second form in (9.109) can be used to obtain an asymptotic
expression, T~ 1 - 2ka sin (ika - -} \ 4/ + (9.110) which exhibits the small
oscillations explicitly. These approximate expressions (9.109) and (9.110) for 7"
give the ...
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 l/e(w) can be readily calculated and
substituted into (13.70). Then the integral over da> can be performed in the same
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Introduction to Electrostatics
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