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Page 477
... spectrum thus contains frequencies up to a maximum w , ~ ( At ) −1 . Wo for arbitrary motion it plays the role of a fundamental frequency of motion . Equation ( 14.50 ) shows that a relativistic particle emits a broad spectrum of ...
... spectrum thus contains frequencies up to a maximum w , ~ ( At ) −1 . Wo for arbitrary motion it plays the role of a fundamental frequency of motion . Equation ( 14.50 ) shows that a relativistic particle emits a broad spectrum of ...
Page 525
... spectrum of virtual quanta I ( w ' ) is given by ( 15.54 ) with q = Ze . The minimum impact parameter is ħ / Mv , so that the frequency spectrum extends up to ' ~ yMc2 / h . The virtual quanta are scattered by the incident particle ...
... spectrum of virtual quanta I ( w ' ) is given by ( 15.54 ) with q = Ze . The minimum impact parameter is ħ / Mv , so that the frequency spectrum extends up to ' ~ yMc2 / h . The virtual quanta are scattered by the incident particle ...
Page 528
... spectrum of energies up to some maximum . Then the radiation spectrum ( 15.66 ) must be averaged over the energy distribution of the beta particles . Furthermore , a quantum- mechanical treatment leads to modifications near the upper ...
... spectrum of energies up to some maximum . Then the radiation spectrum ( 15.66 ) must be averaged over the energy distribution of the beta particles . Furthermore , a quantum- mechanical treatment leads to modifications near the upper ...
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