Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Page 3
... attenuation of a wave penetrating a medium . One can also use some arguments based on approximate solutions of the wave equation of the incident particle interacting through potentials with the target particles . For instance , in the ...
... attenuation of a wave penetrating a medium . One can also use some arguments based on approximate solutions of the wave equation of the incident particle interacting through potentials with the target particles . For instance , in the ...
Page 49
... attenuation of the outgoing vector meson beam is different . So , in the last two expressions for M ( y → V ) our Mr → V ( q ) depend on the position of all the other nucleons . These formulae are now adapted to take care of ...
... attenuation of the outgoing vector meson beam is different . So , in the last two expressions for M ( y → V ) our Mr → V ( q ) depend on the position of all the other nucleons . These formulae are now adapted to take care of ...
Page 54
... of vector mesons on nuclear targets we can easily remedy this situation . So , the only change we should introduce into the formulae given for vector meson photoproduction is an attenuation of the incident beam of 54.
... of vector mesons on nuclear targets we can easily remedy this situation . So , the only change we should introduce into the formulae given for vector meson photoproduction is an attenuation of the incident beam of 54.
Page 55
Wiesław Czyż. meson photoproduction is an attenuation of the incident beam of hadrons ( the incident photons were not attenuated due to the weakness of electromagnetic interactions ) . Let us make this extension explicitly and obtain the ...
Wiesław Czyż. meson photoproduction is an attenuation of the incident beam of hadrons ( the incident photons were not attenuated due to the weakness of electromagnetic interactions ) . Let us make this extension explicitly and obtain the ...
Page 61
... attenuation of the outgoing object ( compare the discussion of experimental results given previously ) . Then the elastic scattering amplitude of | 1 ) ( = | ) ) is totally determined M ( 1 → 1 ) = 1⁄2 [ ( Ï | T ‹ 4 ) | 1 ) + ( 2 | T ...
... attenuation of the outgoing object ( compare the discussion of experimental results given previously ) . Then the elastic scattering amplitude of | 1 ) ( = | ) ) is totally determined M ( 1 → 1 ) = 1⁄2 [ ( Ï | T ‹ 4 ) | 1 ) + ( 2 | T ...
Common terms and phrases
absorption additivity of phase anomalous magnetic moment ú approximately assume attenuation b+½s beam Bureau of Standards coherent diffractive production collision Compton scattering compute Coulomb interactions Czyż d³r db exp i▲·b deuteron diagonalization diffractive production processes diffractive scattering discussed double scattering elastic scattering amplitude electromagnetic equation example excited experiments factor Feynman diagrams formula four-momentum Glauber model hadrons Hence high energy limit incident particle incident wave inelastic shadowing Interactions of High invariant mass K mesons multiple scattering National Bureau neutrino neutrons ññ Note nuclear matter nuclear targets nuclei nucleon obtained optical theorem parameters phase shifts photon photoproduction of vector physical pion production amplitude profiles quantum numbers regeneration Řº shadowing effects single scattering spin strongly interacting target nucleus total cross section vector meson VMD model wave function γν Σ Σ