Interactions of High Energy Particles with Nuclei |
From inside the book
Page 3
One can use , e.g. , an optical description of attenuation of a wave penetrating a medium . One can also use some arguments based on approximate solutions of the wave equation of the incident particle interacting through potentials with ...
One can use , e.g. , an optical description of attenuation of a wave penetrating a medium . One can also use some arguments based on approximate solutions of the wave equation of the incident particle interacting through potentials with ...
Page 49
Note that for nucleons at different positions z , the attenuation of the outgoing vector meson beam is different . So , in the last two expressions for M ( 9V ) our My ( q ) depend on the position of all the other nucleons .
Note that for nucleons at different positions z , the attenuation of the outgoing vector meson beam is different . So , in the last two expressions for M ( 9V ) our My ( q ) depend on the position of all the other nucleons .
Page 54
... with our experience in photoproduction of vector mesons on nuclear targets we can easily remedy this situation . So , the only change we should introduce into the formulae given for vector meson photoproduction is an attenuation of ...
... with our experience in photoproduction of vector mesons on nuclear targets we can easily remedy this situation . So , the only change we should introduce into the formulae given for vector meson photoproduction is an attenuation of ...
Page 55
meson photoproduction is an attenuation of the incident beam of hadrons ( the incident photons were not attenuated due to the weakness of electromagnetic interactions ) . Let us make this extension explicitly and obtain the so - called ...
meson photoproduction is an attenuation of the incident beam of hadrons ( the incident photons were not attenuated due to the weakness of electromagnetic interactions ) . Let us make this extension explicitly and obtain the so - called ...
Page 61
The formula ( 5.7 ) contains the correct attenuation of the outgoing object ( compare the discussion of experimental results given previously ) . Then the elastic scattering amplitude of ( 1 ) ( = | * ) ) is totally determined M ( 1-1 ) ...
The formula ( 5.7 ) contains the correct attenuation of the outgoing object ( compare the discussion of experimental results given previously ) . Then the elastic scattering amplitude of ( 1 ) ( = | * ) ) is totally determined M ( 1-1 ) ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Common terms and phrases
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 hadrons Hence high energy limit important incident particle inelastic initial Institute interactions introduce magnetic mass materials measurement momentum transfer multiple scattering National Bureau Note nuclear nuclear targets nuclei nucleon numbers objects obtained parameters phase shifts photon photoproduction physical position possible problem profiles 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 |