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Page ix
... quantum - mechanical ex- pressions for energy loss , etc. , from the classical results . This approach , so fruitful in the hands of Niels Bohr and E. J. Williams , allows one to see clearly how and when quantum - mechanical effects ...
... quantum - mechanical ex- pressions for energy loss , etc. , from the classical results . This approach , so fruitful in the hands of Niels Bohr and E. J. Williams , allows one to see clearly how and when quantum - mechanical effects ...
Page 454
John David Jackson. We note that the ratio of the classical to quantum - mechanical angles Omin is Zze2 / hu in agreement with the ratio ( 13.42 ) of the classical and quantum values of bmin . For fast particles in all but the highest Z ...
John David Jackson. We note that the ratio of the classical to quantum - mechanical angles Omin is Zze2 / hu in agreement with the ratio ( 13.42 ) of the classical and quantum values of bmin . For fast particles in all but the highest Z ...
Page 579
... quantum - mechanical treatments would remove the difficulties . While there is still hope that this may eventually occur , the present quantum - mechanical discussions are beset with even elaborate troubles than the classical ones . It ...
... quantum - mechanical treatments would remove the difficulties . While there is still hope that this may eventually occur , the present quantum - mechanical discussions are beset with even elaborate troubles than the classical ones . It ...
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Common terms and phrases
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