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 analysis approximately assume attenuation beam coherent collision complete components compute consider contribution corrections Coulomb Coulomb interactions coupling cross section db exp db exp i▲·b depend describe deuteron diffractive production processes discussed effects elastic scattering elastic scattering amplitude equation example excited existence experimental experiments expression fact factor field final formula forward given gives Glauber ground hadrons Hence high energy limit important incident particle inelastic initial Institute interactions introduce magnetic mass measurement momentum transfer multiple scattering Note nuclear nuclear targets nuclei nucleon numbers objects obtained parameters phase shifts photon photoproduction physical position possible problem profiles regeneration shadowing single Standards step strong structure technical vector meson wave function weak