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Page 515
... cross section and the frequency . The radiation cross section has the dimensions of ( cross- sectional area ) · ( energy ) · ( frequency ) -1 . Since energy and frequency transform in the same way under Lorentz transformations , while ...
... cross section and the frequency . The radiation cross section has the dimensions of ( cross- sectional area ) · ( energy ) · ( frequency ) -1 . Since energy and frequency transform in the same way under Lorentz transformations , while ...
Page 525
... cross section ( 14.105 ) at low frequencies and the Klein - Nishina formula ( 14.106 ) at photon energies ho ' Mc2 . Thus , in the frame K ' , for frequencies small compared to Mc2 / h , the radiation cross section z ' ( w ) is given by ...
... cross section ( 14.105 ) at low frequencies and the Klein - Nishina formula ( 14.106 ) at photon energies ho ' Mc2 . Thus , in the frame K ' , for frequencies small compared to Mc2 / h , the radiation cross section z ' ( w ) is given by ...
Page 606
John David Jackson. We see that near the resonant frequency wo the absorption cross section has the same Lorentz shape as the scattering cross section , but is larger by a factor / г . At high frequencies I , → w2 , so that the ...
John David Jackson. We see that near the resonant frequency wo the absorption cross section has the same Lorentz shape as the scattering cross section , but is larger by a factor / г . At high frequencies I , → w2 , so that the ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain oscillations P₁ parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ