Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 1
... discussed in this article . Special attention is paid to the interaction of high energy hadrons and photons . Interactions of high energy electrons and neutrinos are briefly men- tioned . The common features of all these processes are ...
... discussed in this article . Special attention is paid to the interaction of high energy hadrons and photons . Interactions of high energy electrons and neutrinos are briefly men- tioned . The common features of all these processes are ...
Page 18
... discussed above do approximately exhaust the list of processes contributing to elastic scattering . From our discussion of the components of σTOT ( σel , σDT , σPROD ) it follows that the measure- ments of σror may be a good way of ...
... discussed above do approximately exhaust the list of processes contributing to elastic scattering . From our discussion of the components of σTOT ( σel , σDT , σPROD ) it follows that the measure- ments of σror may be a good way of ...
Page 27
... on QED ! These and other related problems have been discussed in a series of papers by Cheng and Wu [ 21 , 22 ] ( see also [ 30 ] , [ S4 ] ) . 4. Diffractive Dissociation and Diffractive Excitation Diffractive processes - a 27 27.
... on QED ! These and other related problems have been discussed in a series of papers by Cheng and Wu [ 21 , 22 ] ( see also [ 30 ] , [ S4 ] ) . 4. Diffractive Dissociation and Diffractive Excitation Diffractive processes - a 27 27.
Page 38
... with hadronic targets at high energy , a process which will be discussed later . Example 1 : The processes of QED : ( a ) Bremsstrahlung : the Feynman diagrams हु Z AND давно go over to AND where the dot means that complete 38.
... with hadronic targets at high energy , a process which will be discussed later . Example 1 : The processes of QED : ( a ) Bremsstrahlung : the Feynman diagrams हु Z AND давно go over to AND where the dot means that complete 38.
Page 50
... discussed above [ 37 ] had shown that when or ( YA ) is computed from ( 4.10 ) , the single scattering contribution is not the one given by the VMD model ( compare also footnote 1 ) . Now let us go back to photoproduction of vector ...
... discussed above [ 37 ] had shown that when or ( YA ) is computed from ( 4.10 ) , the single scattering contribution is not the one given by the VMD model ( compare also footnote 1 ) . Now let us go back to photoproduction of vector ...
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