Interactions of High Energy Particles with Nuclei |
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Page 12
For the sake of simplicity let us take the wave functions of ( a ) and ( b ) in the form of products of single particle wave functions . Let us assume also that all particles have the same single particle wave functions .
For the sake of simplicity let us take the wave functions of ( a ) and ( b ) in the form of products of single particle wave functions . Let us assume also that all particles have the same single particle wave functions .
Page 25
A geometrical picture of single- , double- , etc. scattering contributions is as follows : log / ml Single ( positive ) Double ( negative ) Triple ( positive ) A2 ( ii ) With this picture it is easy to establish the existence of ...
A geometrical picture of single- , double- , etc. scattering contributions is as follows : log / ml Single ( positive ) Double ( negative ) Triple ( positive ) A2 ( ii ) With this picture it is easy to establish the existence of ...
Page 26
... the ( mmm ' ) contributions are indeed the most important but they always lead to a sharp diffractive minimum : DEUTERON TARGET doel log SINGLE 2 DA DOUBLE 10 But ( m | S12 | m ' ) # 0 in general ( also ( m | S12S12 | m ' ) + 0 ) .
... the ( mmm ' ) contributions are indeed the most important but they always lead to a sharp diffractive minimum : DEUTERON TARGET doel log SINGLE 2 DA DOUBLE 10 But ( m | S12 | m ' ) # 0 in general ( also ( m | S12S12 | m ' ) + 0 ) .
Page 38
This represents both single and double scattering of the n- a system This represents both single and double scattering of the n - t system . T - р P in which the diffractive elastic scattering occurs either before or after the ...
This represents both single and double scattering of the n- a system This represents both single and double scattering of the n - t system . T - р P in which the diffractive elastic scattering occurs either before or after the ...
Page 43
When the VMD model does reproduce the correct total photon - nucleon cross section the contribution given above is just a single scattering contribution of the multiple scattering of vector mesons and is properly taken care of by the ...
When the VMD model does reproduce the correct total photon - nucleon cross section the contribution given above is just a single scattering contribution of the multiple scattering of vector mesons and is properly taken care of by the ...
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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 |