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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 x ' ( w ' ) is given ...
... 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 x ' ( w ' ) is given ...
Page 606
... 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 absorption cross section approaches the constant Thomson value ( we have again ignored WT ...
... 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 absorption cross section approaches the constant Thomson value ( we have again ignored WT ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ