Classical Electrodynamics |
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Page 515
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'(o') in the system K' is 16 Zoe? (#. ) () (o: 2) '(a)') c + --| – || |-| ln I ...
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'(o') in the system K' is 16 Zoe? (#. ) () (o: 2) '(a)') c + --| – || |-| ln I ...
Page 525
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, in the frame K
", ...
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, in the frame K
", ...
Page 604
In the neighborhood of the resonance the cross section can be approximated by
do(a), e.') ~ 9. 7.2 T2 d() 16" (o – or 4 (T/2)* where Zo = (cloo) is the wavelength (
divided by 2m) at resonance, T = woot is the radiative decay constant, and T, c T
...
In the neighborhood of the resonance the cross section can be approximated by
do(a), e.') ~ 9. 7.2 T2 d() 16" (o – or 4 (T/2)* where Zo = (cloo) is the wavelength (
divided by 2m) at resonance, T = woot is the radiative decay constant, and T, c T
...
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Contents
Introduction to Electrostatics | 1 |
References and suggested reading | 23 |
Multipoles Electrostatics of Macroscopic Media | 98 |
Copyright | |
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