Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 1-5 of 8
Page 1
... inelastic electron - nucleus scattering , ( 7 ) Shadowing effects in neutrino reactions on nuclei . Key words : Diffractive production ; diffractive scattering ; Glauber model ; hadronic components of photons ; high energy scattering ...
... inelastic electron - nucleus scattering , ( 7 ) Shadowing effects in neutrino reactions on nuclei . Key words : Diffractive production ; diffractive scattering ; Glauber model ; hadronic components of photons ; high energy scattering ...
Page 18
... inelastic screening ( or inelastic shadowing ) phenomenon [ 47 ] . In order to include them we have to ascribe some kind of structure to the incident particle . Earlier in these notes we gave some examples of such cases . To analyze ...
... inelastic screening ( or inelastic shadowing ) phenomenon [ 47 ] . In order to include them we have to ascribe some kind of structure to the incident particle . Earlier in these notes we gave some examples of such cases . To analyze ...
Page 28
... inelastic processes : ( experiments seem to indicate that the differential cross sections depend weakly on energy ) γρ π - 3π T → 5π p → n + T on nucleons or nuclei . K¬Kπ , KËT etc. The nucleon and nuclear targets supplement each ...
... inelastic processes : ( experiments seem to indicate that the differential cross sections depend weakly on energy ) γρ π - 3π T → 5π p → n + T on nucleons or nuclei . K¬Kπ , KËT etc. The nucleon and nuclear targets supplement each ...
Page 29
... inelastic scattering amplitudes . Since the transmitted wave is = n , the wave which goes into scattering and production is ¥ n− ❤ = Ny ¥ y = λel ¥ n + λinel ¥ nxe ; But hence V1 = ny ¥ n - n2 ¥ nxez ; λel = ny2 , λinel = ―nzny ...
... inelastic scattering amplitudes . Since the transmitted wave is = n , the wave which goes into scattering and production is ¥ n− ❤ = Ny ¥ y = λel ¥ n + λinel ¥ nxe ; But hence V1 = ny ¥ n - n2 ¥ nxez ; λel = ny2 , λinel = ―nzny ...
Page 31
... inelastic amplitude ( X ; | T | X ; ) = ( 1 - ni ) € ¡ ¡ — ( 1 — nj ) Eij ( 4.4 ) is proportional to the difference between the absorption of the produced particle and the absorption of the incident particle . One still faces the ...
... inelastic amplitude ( X ; | T | X ; ) = ( 1 - ni ) € ¡ ¡ — ( 1 — nj ) Eij ( 4.4 ) is proportional to the difference between the absorption of the produced particle and the absorption of the incident particle . One still faces the ...
Common terms and phrases
absorption additivity of phase anomalous magnetic moment ú approximately assume attenuation beam Bureau of Standards coherent diffractive production collision Compton scattering compute Coulomb interactions Czyż d³r db bJo 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 Απ γν ΦΩ