Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
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Page 15
... structure ( e.g. , diffractive minima ) of the high energy hadron - hadron collisions . The very recent measurements of p - p elastic collisions confirm the existence of such a structure ( CERN - Serpukhov experiment ) . In the form ...
... structure ( e.g. , diffractive minima ) of the high energy hadron - hadron collisions . The very recent measurements of p - p elastic collisions confirm the existence of such a structure ( CERN - Serpukhov experiment ) . In the form ...
Page 18
... structure to the incident particle . Earlier in these notes we gave some examples of such cases . To analyze this problem in more detail , one has to link it with diffractive production processes and we shall postpone such a discussion ...
... structure to the incident particle . Earlier in these notes we gave some examples of such cases . To analyze this problem in more detail , one has to link it with diffractive production processes and we shall postpone such a discussion ...
Page 34
... ( structure of K , and KL , fK ° n , SK ° n , SK ° p , SK ° p amplitudes ) we obtained a very important piece of information about the target nuclei : the neutron distribution . This is so because neutrons are more effective in ...
... ( structure of K , and KL , fK ° n , SK ° n , SK ° p , SK ° p amplitudes ) we obtained a very important piece of information about the target nuclei : the neutron distribution . This is so because neutrons are more effective in ...
Page 43
... structure constant ) : ( kv H'ky ) E , -Ev ν πα 848 γν m 1020 MeV ) . Then But M ( v → y ) = ΣM ( v → V ) V Υπα γν Υπα M ( y → V ) = M ( V → V ) γν 4 Note that restricting the high energy photon - nucleus interaction to only vector ...
... structure constant ) : ( kv H'ky ) E , -Ev ν πα 848 γν m 1020 MeV ) . Then But M ( v → y ) = ΣM ( v → V ) V Υπα γν Υπα M ( y → V ) = M ( V → V ) γν 4 Note that restricting the high energy photon - nucleus interaction to only vector ...
Page 53
... structure constant . ) ( iii ) The results of this analysis check beautifully with the results obtained from po photo- production on larger nuclei ( whose cross sections , incidentally , do depend sensitively on 7 , as we have already ...
... structure constant . ) ( iii ) The results of this analysis check beautifully with the results obtained from po photo- production on larger nuclei ( whose cross sections , incidentally , do depend sensitively on 7 , as we have already ...
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