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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 ħ ( 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 ħ ( 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 mħ units of z 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 mħ units of z component of angular momentum per photon of energy ho . In further analogy with quantum ...
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