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Page 474
... relativistic radiation patterns , regardless of the vectorial relation between ẞ and B. The total power radiated can ... relativistic peaking at forward angles is present . In the relativistic limit ( y > 1 ) , the angular dP dn 919 ...
... relativistic radiation patterns , regardless of the vectorial relation between ẞ and B. The total power radiated can ... relativistic peaking at forward angles is present . In the relativistic limit ( y > 1 ) , the angular dP dn 919 ...
Page 632
... relativistic , 394 f . Kirchhoff diffraction , see Diffraction Kirchhoff's integral representation , 188 use of , in diffraction , 280 vector equivalent of , 283 Klein - Nishina formula , 490 Lagrangian , for relativistic charge par ...
... relativistic , 394 f . Kirchhoff diffraction , see Diffraction Kirchhoff's integral representation , 188 use of , in diffraction , 280 vector equivalent of , 283 Klein - Nishina formula , 490 Lagrangian , for relativistic charge par ...
Page 637
... Relativistic notation , 377 Relativistic transformation , and Thomas precession , 367 from CM system to laboratory , 400 f . of acceleration , 388 of charge and current densities , 378 of coordinates , 357 of electromagnetic fields ...
... Relativistic notation , 377 Relativistic transformation , and Thomas precession , 367 from CM system to laboratory , 400 f . of acceleration , 388 of charge and current densities , 378 of coordinates , 357 of electromagnetic fields ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ