Interactions of High Energy Particles with Nuclei |
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Page 12
... is not an academic problem because there are experimental pro- jects under way ) . The geometry of the process is shown in figure 3 . 255 O A COMPONENTS ( b ) ( 0 ) O B COMPONENTS The profile describing the collision of two elements ...
... is not an academic problem because there are experimental pro- jects under way ) . The geometry of the process is shown in figure 3 . 255 O A COMPONENTS ( b ) ( 0 ) O B COMPONENTS The profile describing the collision of two elements ...
Page 14
Some special cases of formula ( 3.2 ) were also employed to describe hadron - hadron scattering in the high energy limit . For example , the limit when A and B become very large was considered [ 13 ] ( compare also [ 12 ] ) : lim M = A ...
Some special cases of formula ( 3.2 ) were also employed to describe hadron - hadron scattering in the high energy limit . For example , the limit when A and B become very large was considered [ 13 ] ( compare also [ 12 ] ) : lim M = A ...
Page 28
We shall describe diffractive production processes in very close analogy to diffractive dissociation phenomena which are well known in the case of systems where degeneracy exists . Let us start with an example taken from optics .
We shall describe diffractive production processes in very close analogy to diffractive dissociation phenomena which are well known in the case of systems where degeneracy exists . Let us start with an example taken from optics .
Page 34
In describing the regeneration process K - K , we drew heavily on the known structure of K and K , ° : they are superpositions of K ° and Ko , whose elastic scattering from nucleons is reason- ably well known . 4.1 .
In describing the regeneration process K - K , we drew heavily on the known structure of K and K , ° : they are superpositions of K ° and Ko , whose elastic scattering from nucleons is reason- ably well known . 4.1 .
Page 36
π Final state : n + π = + 12 ñ = d1 TM ” | ññ ) + d2 TM ” | μ ) . p = small admixture In the sense given earlier in these notes , for the purpose of describing elastic scattering we have approximately ( compare eq ( 4.4 ) ) The ...
π Final state : n + π = + 12 ñ = d1 TM ” | ññ ) + d2 TM ” | μ ) . p = small admixture In the sense given earlier in these notes , for the purpose of describing elastic scattering we have approximately ( compare eq ( 4.4 ) ) The ...
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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 |