Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 47
... momentum transfer different from zero : mv2 A [ [ ༤ 2 ய Then the graphical description of figure 38 is not valid any more . One has to allow the amplitude Mnucleon ( Y → V ) to oscillate with the function eis 11 . This factor partly ...
... momentum transfer different from zero : mv2 A [ [ ༤ 2 ய Then the graphical description of figure 38 is not valid any more . One has to allow the amplitude Mnucleon ( Y → V ) to oscillate with the function eis 11 . This factor partly ...
Page 48
... momentum transfer vector . As long as there is only one scattering center this phase factor is irrelevant , but when there are more scattering centers we obtain M ( q ) = Σeiar¡Mj ( q ) , which is the formula used here . 6 The argument ...
... momentum transfer vector . As long as there is only one scattering center this phase factor is irrelevant , but when there are more scattering centers we obtain M ( q ) = Σeiar¡Mj ( q ) , which is the formula used here . 6 The argument ...
Page 54
... momentum transfer for the case of vector meson production ( the formula for elastic photon scattering was also given with- out derivation ) . 3. The Vector Meson Dominance model was briefly discussed and some recent experiments which ...
... momentum transfer for the case of vector meson production ( the formula for elastic photon scattering was also given with- out derivation ) . 3. The Vector Meson Dominance model was briefly discussed and some recent experiments which ...
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