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Page 102
... quantum numbers of total angular momentum J and its projection M along the z axis , as well as others which we will denote by a general index a . A given nuclear state has associated with it a quantum - mechanical charge density * PJM ...
... quantum numbers of total angular momentum J and its projection M along the z axis , as well as others which we will denote by a general index a . A given nuclear state has associated with it a quantum - mechanical charge density * PJM ...
Page 439
... quantum- mechanical modifications cause a breakdown of the classical result . The important quantum effects are ( 1 ) discreteness of the possible energy transfers , and ( 2 ) limitations due to the wave nature of the particles and the ...
... quantum- mechanical modifications cause a breakdown of the classical result . The important quantum effects are ( 1 ) discreteness of the possible energy transfers , and ( 2 ) limitations due to the wave nature of the particles and the ...
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 ) ...
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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