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Page 443
John David Jackson. 13.4 Density Effect in Collision Energy Loss For particles which are not too relativistic the observed energy loss is given accurately by ( 13.44 ) [ or by ( 13.36 ) if ʼn > 1 ] for all kinds of particles in all types ...
John David Jackson. 13.4 Density Effect in Collision Energy Loss For particles which are not too relativistic the observed energy loss is given accurately by ( 13.44 ) [ or by ( 13.36 ) if ʼn > 1 ] for all kinds of particles in all types ...
Page 448
... energy loss no longer depends on the details of atomic structure through ( w ) ( 13.38 ) , but only on the number of electrons per unit volume through w ,. Two substances having very different atomic struc- tures will produce the same ...
... energy loss no longer depends on the details of atomic structure through ( w ) ( 13.38 ) , but only on the number of electrons per unit volume through w ,. Two substances having very different atomic struc- tures will produce the same ...
Page 449
... Energy loss , including the density effect . The dotted curve is the total energy loss without density correction . The solid curves have the density effect incorporated , the upper one being the total energy loss and the lower one the ...
... Energy loss , including the density effect . The dotted curve is the total energy loss without density correction . The solid curves have the density effect incorporated , the upper one being the total energy loss and the lower one the ...
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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