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Page 151
... atomic electrons possess intrinsic magnetic moments which cannot be expressed in terms of a current density . These moments can give rise to dipole fields which vary appreciably on the atomic scale of dimensions . To treat these atomic ...
... atomic electrons possess intrinsic magnetic moments which cannot be expressed in terms of a current density . These moments can give rise to dipole fields which vary appreciably on the atomic scale of dimensions . To treat these atomic ...
Page 559
... atomic or nuclear transition the lowest nonvanishing multipole will generally be the only one of importance . The ratio of transition probabilities for successive orders of either electric or magnetic multipoles of the same frequency is ...
... atomic or nuclear transition the lowest nonvanishing multipole will generally be the only one of importance . The ratio of transition probabilities for successive orders of either electric or magnetic multipoles of the same frequency is ...
Page 638
... atoms , 451 f . effect of atomic screening on , 453 effect of nuclear size on , 454 mean square angle of , 456 multiple , 458 single , 458 total atomic cross section for , 455 Scattering of radiation , by conducting sphere , at long ...
... atoms , 451 f . effect of atomic screening on , 453 effect of nuclear size on , 454 mean square angle of , 456 multiple , 458 single , 458 total atomic cross section for , 455 Scattering of radiation , by conducting sphere , at long ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ