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3 c We2/ W \ rua ' To transform this result to the (unprimed) laboratory frame we
need to know the transformation properties of the radiation cross section and the
frequency. The radiation cross section has the dimensions of (cross- sectional ...
The virtual quanta are scattered by the incident particle (the struck system in K')
according to the Thomson cross section (14.105) at low frequencies and the
Klein-Nishina formula (14.106) at photon energies ha>' *3 Mc2. Thus, in the
frame K', ...
We see that near the resonant frequency eo0 the absorption cross section has
the same Lorentz shape as the scattering cross section, but is larger by a factor F
</F. At high frequencies F< — »• MZT, so that the absorption cross section ...
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Introduction to Electrostatics
BoundaryValue Problems in Electrostatics I
Multipoles Electrostatics of Macroscopic Media
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