Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 1-5 of 23
Page 15
... cross section ( from the optical theorem ) which is energy independent . So , it seems to be difficult to reconcile this model with the recent evidence for the increase of the total hadron - proton cross sections at very high energies ...
... cross section ( from the optical theorem ) which is energy independent . So , it seems to be difficult to reconcile this model with the recent evidence for the increase of the total hadron - proton cross sections at very high energies ...
Page 17
... cross section at the impact parameter b≈ ( l + 1⁄2 ) / k with all nucleons frozen at the positions $ 1 , SA . .. • So , in our model there are three different contributions . OEL ONLY NUCLEONS APPEAR бот NEW PARTICLES ARE PRODUCED ...
... cross section at the impact parameter b≈ ( l + 1⁄2 ) / k with all nucleons frozen at the positions $ 1 , SA . .. • So , in our model there are three different contributions . OEL ONLY NUCLEONS APPEAR бот NEW PARTICLES ARE PRODUCED ...
Page 18
... cross section is ~ 10 of elastic cross section ) . ( In fact this is one of the very important questions to be answered by the very high energy experiments of the future : how much cross section goes into diffractive production ...
... cross section is ~ 10 of elastic cross section ) . ( In fact this is one of the very important questions to be answered by the very high energy experiments of the future : how much cross section goes into diffractive production ...
Page 19
... cross section is doel do = | Im M2 + | Re M 2 . ( 3.6 ) ( b ) ( which is , as a rule , ( b ) because this is the The amplitude ( 3.6 ) has some simple properties which show that the Coulomb interaction may help us in learning about the ...
... cross section is doel do = | Im M2 + | Re M 2 . ( 3.6 ) ( b ) ( which is , as a rule , ( b ) because this is the The amplitude ( 3.6 ) has some simple properties which show that the Coulomb interaction may help us in learning about the ...
Page 21
... cross section for scattering on either neutron or proton . ( Incidentally , one can define an optical potential ... cross sections . For an ap = -0.33 , σn = 0 , = 38.9 mb ( these parameters are resonable for ~ 20 GeV protons ) , one ...
... cross section for scattering on either neutron or proton . ( Incidentally , one can define an optical potential ... cross sections . For an ap = -0.33 , σn = 0 , = 38.9 mb ( these parameters are resonable for ~ 20 GeV protons ) , one ...
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