Interactions of High Energy Particles with Nuclei |
From inside the book
Results 1-5 of 8
Page 1
... and diffractive excitation , ( 5 ) Diffractive production of hadrons in hadron - nucleon collisions , ( 6 ) Shadowing effects in inelastic electron - nucleus scattering , ( 7 ) Shadowing effects in neutrino reactions on nuclei .
... and diffractive excitation , ( 5 ) Diffractive production of hadrons in hadron - nucleon collisions , ( 6 ) Shadowing effects in inelastic electron - nucleus scattering , ( 7 ) Shadowing effects in neutrino reactions on nuclei .
Page 18
O O O O They are the source of the so - called 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 ...
O O O O They are the source of the so - called 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 ...
Page 28
... Compton scattering , etc. in hadron physics ; all kinds of elastic hadron - hadron scattering do ( experiments seem to indicate that the = f ( ) differential cross sections depend weakly DA ? on energy ) inelastic processes : 7 - sp ...
... Compton scattering , etc. in hadron physics ; all kinds of elastic hadron - hadron scattering do ( experiments seem to indicate that the = f ( ) differential cross sections depend weakly DA ? on energy ) inelastic processes : 7 - sp ...
Page 29
Let us compute the elastic and inelastic scattering amplitudes . Since the transmitted wave is y = n , V , the wave which goes into scattering and production is ry - 4 = n ,, = ley + Aineinge , But Vy = n , Yn - nzYnyez ; hence 1 λο1 ...
Let us compute the elastic and inelastic scattering amplitudes . Since the transmitted wave is y = n , V , the wave which goes into scattering and production is ry - 4 = n ,, = ley + Aineinge , But Vy = n , Yn - nzYnyez ; hence 1 λο1 ...
Page 31
... zero zero = ( 1-7 ; 8 ; teji ( 1-7 ; ) - Eji ( 1 - ni ) . In this approximation ( Til T | 1i ) = 1 - mi = 2 Hence the absorption parameters ni are determined by elastic scattering of real particles . The inelastic amplitude ( il T | ...
... zero zero = ( 1-7 ; 8 ; teji ( 1-7 ; ) - Eji ( 1 - ni ) . In this approximation ( Til T | 1i ) = 1 - mi = 2 Hence the absorption parameters ni are determined by elastic scattering of real particles . The inelastic amplitude ( il T | ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Common terms and phrases
absorption additivity analysis approximately assume attenuation beam Bureau of Standards charge coherent collision complete components compute consider contribution corrections Coulomb Coulomb interactions coupling cross section db exp depend describe deuteron diffractive production processes discussed effects elastic scattering elastic scattering amplitude equation example excited existence exp ia.b 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 National Bureau Note nuclear nuclear targets nuclei nucleon numbers objects obtained parameters phase shifts photon photoproduction physical position possible present problem profiles regeneration shadowing single Standards step strong structure technical vector meson wave function