Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 1
... effects in 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 ...
... effects in 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 ...
Page 2
... effects . So , the crucial point in our discussion is an understanding of a multiple scattering process of strongly interacting particles inside of nuclear matter ( or more generally : just a multiple scattering process with forces ...
... effects . So , the crucial point in our discussion is an understanding of a multiple scattering process of strongly interacting particles inside of nuclear matter ( or more generally : just a multiple scattering process with forces ...
Page 18
... effects which the model allows for ) and then found a definite dis- crepancy with experimentally measured Tor - it would very strongly suggest the existence of inelastic shadowing phenomena described above . In fact such an analysis has ...
... effects which the model allows for ) and then found a definite dis- crepancy with experimentally measured Tor - it would very strongly suggest the existence of inelastic shadowing phenomena described above . In fact such an analysis has ...
Page 19
... effects produced by the average Coulomb potential produced by the whole nucleus [ 15 ] which produces almost identical results [ 16 , 17 ] . We shall assume that , in the high energy limit , the total phase shift is the sum of the ...
... effects produced by the average Coulomb potential produced by the whole nucleus [ 15 ] which produces almost identical results [ 16 , 17 ] . We shall assume that , in the high energy limit , the total phase shift is the sum of the ...
Page 26
... effect in more detail . The ground state deuteron wave function is : Pm ( r ) = ( 4π ) -1 / 2-1 [ u ( r ) + 8-1 / 2 S12W ( r ) Jx1.m where u ( r ) and w ( r ) are the radial S and D functions and Sız = [ 3 ( ơi • r ) ( • r ) −ơi ...
... effect in more detail . The ground state deuteron wave function is : Pm ( r ) = ( 4π ) -1 / 2-1 [ u ( r ) + 8-1 / 2 S12W ( r ) Jx1.m where u ( r ) and w ( r ) are the radial S and D functions and Sız = [ 3 ( ơi • r ) ( • r ) −ơi ...
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