Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 1
... discussed in this article . Special attention is paid to the interaction of high energy hadrons and photons . Interactions of high energy electrons and neutrinos are briefly men- tioned . The common features of all these processes are ...
... discussed in this article . Special attention is paid to the interaction of high energy hadrons and photons . Interactions of high energy electrons and neutrinos are briefly men- tioned . The common features of all these processes are ...
Page 18
... discussed above do approximately exhaust the list of processes contributing to elastic scattering . From our discussion of the components of σTOT ( σel , σDT , σPROD ) it follows that the measure- ments of σror may be a good way of ...
... discussed above do approximately exhaust the list of processes contributing to elastic scattering . From our discussion of the components of σTOT ( σel , σDT , σPROD ) it follows that the measure- ments of σror may be a good way of ...
Page 27
... on QED ! These and other related problems have been discussed in a series of papers by Cheng and Wu [ 21 , 22 ] ( see also [ 30 ] , [ S4 ] ) . 4. Diffractive Dissociation and Diffractive Excitation Diffractive processes - a 27 27.
... on QED ! These and other related problems have been discussed in a series of papers by Cheng and Wu [ 21 , 22 ] ( see also [ 30 ] , [ S4 ] ) . 4. Diffractive Dissociation and Diffractive Excitation Diffractive processes - a 27 27.
Page 38
... with hadronic targets at high energy , a process which will be discussed later . Example 1 : The processes of QED : ( a ) Bremsstrahlung : the Feynman diagrams हु Z AND давно go over to AND where the dot means that complete 38.
... with hadronic targets at high energy , a process which will be discussed later . Example 1 : The processes of QED : ( a ) Bremsstrahlung : the Feynman diagrams हु Z AND давно go over to AND where the dot means that complete 38.
Page 50
... discussed above [ 37 ] had shown that when or ( YA ) is computed from ( 4.10 ) , the single scattering contribution is not the one given by the VMD model ( compare also footnote 1 ) . Now let us go back to photoproduction of vector ...
... discussed above [ 37 ] had shown that when or ( YA ) is computed from ( 4.10 ) , the single scattering contribution is not the one given by the VMD model ( compare also footnote 1 ) . Now let us go back to photoproduction of vector ...
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
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 |