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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 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 effects ...
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 effects ...
Page 527
... bremsstrahlung spectrum with number of photons per unit energy range given by N ( hw ) = e2 1 ahc \ hol LB In - + ß β ― 2 ( 15.67 ) It sometimes bears the name " inner bremsstrahlung " to distinguish it from bremsstrahlung emitted by ...
... bremsstrahlung spectrum with number of photons per unit energy range given by N ( hw ) = e2 1 ahc \ hol LB In - + ß β ― 2 ( 15.67 ) It sometimes bears the name " inner bremsstrahlung " to distinguish it from bremsstrahlung emitted by ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 modes momentum multipole nonrelativistic obtain oscillations P₁ parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ