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This sets a lower limit on impact parameters equal to ( 15.17 ) , even for relativistic motion . With ( 15.11 ) , ( 15.12 ) , and these revised impact parameters , the radiation cross section x'w ' ) in the system K ' is 16 Ze ?
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 ho ' > Mc . Thus ...
We see that near the resonant frequency w , the absorption cross section has the same Lorentz shape as the scattering cross section , but is larger by a factor T // . At high frequencies T , → wot , so that the absorption cross section ...
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Introduction to Electrostatics
BoundaryValue Problems in Electrostatics I
TimeVarying Fields Maxwells Equations Con
4 other sections not shown