Interactions of High Energy Particles with Nuclei |
From inside the book
Page 30
... not observed in scattering experiments . ( The process of KK , ' regeneration given below is an example where we know ni's however ! ) The situation changes when we accept that diffractive production processes are weak compared to.
... not observed in scattering experiments . ( The process of KK , ' regeneration given below is an example where we know ni's however ! ) The situation changes when we accept that diffractive production processes are weak compared to.
Page 44
All these parameters are obtained from a host of various experiments : y v2 / 41 from ete - storage rings where the following process is observed : e Suma v Oyn and nu ( not shown above 44.
All these parameters are obtained from a host of various experiments : y v2 / 41 from ete - storage rings where the following process is observed : e Suma v Oyn and nu ( not shown above 44.
Page 45
41 is well known from colliding beam experiments . So , it is unlikely that one should reduce it by a ... Nuclear target : One could test ( 4.8 ) directly against experimental data for nuclear targets if the energy were high enough .
41 is well known from colliding beam experiments . So , it is unlikely that one should reduce it by a ... Nuclear target : One could test ( 4.8 ) directly against experimental data for nuclear targets if the energy were high enough .
Page 47
As we saw in the example of our discussion of or ( Y , A ) , present experiments are not quite in this limit ( at several GeV I < R ) . Hence if we want to analyze the existing experimental data we have to keep the longitudinal momentum ...
As we saw in the example of our discussion of or ( Y , A ) , present experiments are not quite in this limit ( at several GeV I < R ) . Hence if we want to analyze the existing experimental data we have to keep the longitudinal momentum ...
Page 50
Recall that the experiments discussed above [ 37 ] had shown that when ot ( YA ) is computed from ( 4.10 ) , the single scattering contribution ... The formulae discussed above were applied to analyze a multitude of experimental data .
Recall that the experiments discussed above [ 37 ] had shown that when ot ( YA ) is computed from ( 4.10 ) , the single scattering contribution ... The formulae discussed above were applied to analyze a multitude of experimental data .
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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 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 |