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
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 strong enough ...
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 strong enough ...
Page 4
The amplitude for the particle to scatter from k to k ' is : M ( k ' , k ) = - ≈ m 2π m 2π d3r exp ( -ik ' • r ) V ... The most complete analysis one can perform is presumably to employ the Watson multiple scattering theory , but we ...
The amplitude for the particle to scatter from k to k ' is : M ( k ' , k ) = - ≈ m 2π m 2π d3r exp ( -ik ' • r ) V ... The most complete analysis one can perform is presumably to employ the Watson multiple scattering theory , but we ...
Page 21
( b ) which is equivalent to our multiple scattering description ) . - 00 = From this expression ( 3.7 ) one can see that the interplay of xc ( b ) and § ( b ) is , in this optical limit , determined by the size and sign of an and a ,.
( b ) which is equivalent to our multiple scattering description ) . - 00 = From this expression ( 3.7 ) one can see that the interplay of xc ( b ) and § ( b ) is , in this optical limit , determined by the size and sign of an and a ,.
Page 24
Then the elastic scattering amplitude ( with the c.m. motion correction included ) reads M ( A ) = ik ( R2 + 2a ) exp ... ( R2 + 20 ) a3 ] 4A ( -1 ) +1 j ( R2 + 2a ) 2π 4j Many general features of the multiple scattering are included in 24.
Then the elastic scattering amplitude ( with the c.m. motion correction included ) reads M ( A ) = ik ( R2 + 2a ) exp ... ( R2 + 20 ) a3 ] 4A ( -1 ) +1 j ( R2 + 2a ) 2π 4j Many general features of the multiple scattering are included in 24.
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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 |