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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 604
... cross section , Osc ( 0 ) ≈ 3 12 г2 2 ( w - @p ) 2 + ( T ; / 2 ) 2 ( 17.66 ) This exhibits the typical Lorentz line shape with half - width given by г , and peak cross section , Osc ( wo ) = σπλο ( 1 ) 2 ( 17.67 ) At high frequencies ...
... cross section , Osc ( 0 ) ≈ 3 12 г2 2 ( w - @p ) 2 + ( T ; / 2 ) 2 ( 17.66 ) This exhibits the typical Lorentz line shape with half - width given by г , and peak cross section , Osc ( wo ) = σπλο ( 1 ) 2 ( 17.67 ) At high frequencies ...
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame 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 P₂ parallel perpendicular plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ