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Page 456
... Scattering and the Angular Distribution of Multiple Scattering Rutherford scattering is confined to very small angles even for a point Coulomb field , and for fast particles Omax is small compared to unity . Thus there is a very large ...
... Scattering and the Angular Distribution of Multiple Scattering Rutherford scattering is confined to very small angles even for a point Coulomb field , and for fast particles Omax is small compared to unity . Thus there is a very large ...
Page 458
... scattering distribution for the projected angle of scattering is PM ( 0 ' ) d0 ' = 1 0/2 exp do ' 2 ( 13.112 ) where both positive and negative values of e ' are considered . The small- angle Rutherford formula ( 13.92 ) can be ...
... scattering distribution for the projected angle of scattering is PM ( 0 ' ) d0 ' = 1 0/2 exp do ' 2 ( 13.112 ) where both positive and negative values of e ' are considered . The small- angle Rutherford formula ( 13.92 ) can be ...
Page 459
... scattering distributions of projected angle . In the region of plural scattering ( a ~ 2-3 ) the dotted curve indicates the smooth transition from the small - angle multiple scattering ( approximately Gaussian in shape ) to the wide ...
... scattering distributions of projected angle . In the region of plural scattering ( a ~ 2-3 ) the dotted curve indicates the smooth transition from the small - angle multiple scattering ( approximately Gaussian in shape ) to the wide ...
Contents
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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