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Page 505
... bremsstrahlung ( braking radiation ) because it was first observed when high- energy electrons were stopped in a thick metallic target . For nonrelativistic particles the loss of energy by radiation is negligible compared with the ...
... bremsstrahlung ( braking radiation ) because it was first observed when high- energy electrons were stopped in a thick metallic target . For nonrelativistic particles the loss of energy by radiation is negligible compared with the ...
Page 513
... bremsstrahlung spectrum . The radiation cross section ( w ) depends on the properties of the particles involved in the collision as Z24 / M2 ... Bremsstrahlung , Virtual Quanta , Radiative Beta Processes Relativistic bremsstrahlung,
... bremsstrahlung spectrum . The radiation cross section ( w ) depends on the properties of the particles involved in the collision as Z24 / M2 ... Bremsstrahlung , Virtual Quanta , Radiative Beta Processes Relativistic bremsstrahlung,
Page 525
John David Jackson. 15.6 Bremsstrahlung as the Scattering of Virtual Quanta The emission of bremsstrahlung in a ... bremsstrahlung cross section in complete agreement with the Bethe - Heitler formulas ( Weizsäcker , 1934 ) . ∞ The ...
John David Jackson. 15.6 Bremsstrahlung as the Scattering of Virtual Quanta The emission of bremsstrahlung in a ... bremsstrahlung cross section in complete agreement with the Bethe - Heitler formulas ( Weizsäcker , 1934 ) . ∞ The ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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 coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ 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