Classical Electrodynamics |
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Page 454
... quantum values of bmin . For fast particles in all but the highest Z sub- stances ( Zze2 / hv ) is less than unity . Then the quantum value ( 13.98 ) will be used for min . With value ( 13.95 ) for the screening radius a , ( 13.98 ) ...
... quantum values of bmin . For fast particles in all but the highest Z sub- stances ( Zze2 / hv ) is less than unity . Then the quantum value ( 13.98 ) will be used for min . With value ( 13.95 ) for the screening radius a , ( 13.98 ) ...
Page 511
... quantum - mechanical formulas apply here as for the energy loss . The frequency spectrum of the quantum cross section extends up to a maximum frequency wax of the order of ( a ) @max Mv2 h ( 15.19 ) We note that this is approximately ...
... quantum - mechanical formulas apply here as for the energy loss . The frequency spectrum of the quantum cross section extends up to a maximum frequency wax of the order of ( a ) @max Mv2 h ( 15.19 ) We note that this is approximately ...
Page 549
John David Jackson. This has the obvious quantum interpretation that the radiation from a multipole of order ( 1 , m ) carries off mh units of a component of angular momentum per photon of energy ho . In further analogy with quantum ...
John David Jackson. This has the obvious quantum interpretation that the radiation from a multipole of order ( 1 , m ) carries off mh units of a component of angular momentum per photon of energy ho . In further analogy with quantum ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis 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 dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result 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