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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 ...
Page 450
John David Jackson. 13.5 Energy Loss in an Electronic Plasma -1 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 -1 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 |
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