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... quantum- mechanical energy loss will correspond to much smaller energy transfers than given by ( 13.2 ) for b < Ax . Thus Ax ~ h / p is a quantum analog of the minimum impact parameter ( 13.6 ) . In the collision of two particles each ...
... quantum- mechanical energy loss will correspond to much smaller energy transfers than given by ( 13.2 ) for b < Ax . Thus Ax ~ h / p is a quantum analog of the minimum impact parameter ( 13.6 ) . In the collision of two particles each ...
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... quantum - mechanical energy - loss formulas are obtained from clas- sical ones by the replacement [ see ( 13.43 ) ] , ze2 B1 = mBc = B. hv ( 13.48 ) we expect that the quantum - mechanical formula for energy - loss per unit distance due ...
... quantum - mechanical energy - loss formulas are obtained from clas- sical ones by the replacement [ see ( 13.43 ) ] , ze2 B1 = mBc = B. hv ( 13.48 ) we expect that the quantum - mechanical formula for energy - loss per unit distance due ...
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... quantum - mechanical formulas apply here as for the energy loss . The frequency spectrum of the quantum cross section extends up to a maximum frequency wax of the order of ( a ) @max Mv2 h ( 15.19 ) We note that this is approximately ...
... quantum - mechanical formulas apply here as for the energy loss . The frequency spectrum of the quantum cross section extends up to a maximum frequency wax of the order of ( a ) @max Mv2 h ( 15.19 ) We note that this is approximately ...
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