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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 n > 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 n > 1 ] for all kinds of particles in all types ...
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... 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 ...
... 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 ...
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John David Jackson. 13.5 Energy Loss in an Electronic Plasma か The loss of energy by a nonrelativistic particle passing through a plasma can be treated in a manner similar to the density effect for a relativistic particle . As was ...
John David Jackson. 13.5 Energy Loss in an Electronic Plasma か The loss of energy by a nonrelativistic particle passing through a plasma can be treated in a manner similar to the density effect for a relativistic particle . As was ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ