Interactions of High Energy Particles with Nuclei |
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Page 1
The common features of all these processes are emphasized throughout the article : The multiple scattering and shadowing processes inside of the target nuclei . An effort is made to develop a unified way of treating nuclear interactions ...
The common features of all these processes are emphasized throughout the article : The multiple scattering and shadowing processes inside of the target nuclei . An effort is made to develop a unified way of treating nuclear interactions ...
Page 2
In other words , in all the processes we are going to discuss , strongly interacting particles appear ( as real or virtual particles ) which may produce shadowing effects . So , the crucial point in our discussion is an understanding of ...
In other words , in all the processes we are going to discuss , strongly interacting particles appear ( as real or virtual particles ) which may produce shadowing effects . So , the crucial point in our discussion is an understanding of ...
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 41
Example 3 : Photoprocesses and vector meson dominance : It is now a well established fact that , at high energy , photons exhibit shadowing . The total photo cross sections for complex nuclei vary approximately as A0.9 in the few GeV ...
Example 3 : Photoprocesses and vector meson dominance : It is now a well established fact that , at high energy , photons exhibit shadowing . The total photo cross sections for complex nuclei vary approximately as A0.9 in the few GeV ...
Page 42
R ( R = nuclear radius ) we shall have shadowing fully developed . We can see , therefore , that full shadowing occurs at high enough energies . At low photon energies | E , -En | is large ...
R ( R = nuclear radius ) we shall have shadowing fully developed . We can see , therefore , that full shadowing occurs at high enough energies . At low photon energies | E , -En | is large ...
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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
Bibliographic information
| Title | Interactions of High Energy Particles with Nuclei Volume 139 of NBS monograph |
| Author | Wiesław Czyż |
| Publisher | National Bureau of Standards, 1975 |
| Original from | the University of Michigan |
| Digitized | 21 Nov 2007 |
| Length | 69 pages |
| Export Citation | BiBTeX EndNote RefMan |