Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 3
... 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 the target particles . For instance , in the ...
... 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 the target particles . For instance , in the ...
Page 49
... attenuation of the outgoing vector meson beam is different . So , in the last two expressions for M ( y → V ) our Mr → V ( q ) depend on the position of all the other nucleons . These formulae are now adapted to take care of ...
... attenuation of the outgoing vector meson beam is different . So , in the last two expressions for M ( y → V ) our Mr → V ( q ) depend on the position of all the other nucleons . These formulae are now adapted to take care of ...
Page 54
... 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 the incident beam of 54.
... 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 the incident beam of 54.
Page 55
Wiesław Czyż. 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 ...
Wiesław Czyż. 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 ...
Page 61
... 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 ) = 1⁄2 [ ( Ï | T ‹ 4 ) | 1 ) + ( 2 | T ...
... 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 ) = 1⁄2 [ ( Ï | T ‹ 4 ) | 1 ) + ( 2 | T ...
Common terms and phrases
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 |
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