Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 1
... photons . Interactions of high energy electrons and neutrinos are briefly men- tioned . The common features of all ... photon - nucleus interactions ; they are not well known in the case of neutrino reactions and very virtual photons ...
... photons . Interactions of high energy electrons and neutrinos are briefly men- tioned . The common features of all ... photon - nucleus interactions ; they are not well known in the case of neutrino reactions and very virtual photons ...
Page 2
... photons inter- acting with nucleons - where the strongly interacting vector mesons seem to dominate in the case of neutrino interactions - as was pointed out by Adler [ 7 ] -T - mesons should be important ) . In other words , in all the ...
... photons inter- acting with nucleons - where the strongly interacting vector mesons seem to dominate in the case of neutrino interactions - as was pointed out by Adler [ 7 ] -T - mesons should be important ) . In other words , in all the ...
Page 27
... PHOTON PHOTON POSITRON INITIAL ELECTRON - POSITRON WAVE FUNCTION Diffractive Scattering from the target FINAL ELECTRON - POSITRON WAVE FUNCTION the " relativistic wave functions " in an analogous way to that shown above in the case of ...
... PHOTON PHOTON POSITRON INITIAL ELECTRON - POSITRON WAVE FUNCTION Diffractive Scattering from the target FINAL ELECTRON - POSITRON WAVE FUNCTION the " relativistic wave functions " in an analogous way to that shown above in the case of ...
Page 30
... photon ) . We want to compute ( X ; | TX ; ) . We expand | X ; ) into a set of states | A ) whose scattering and absorption in the target we assume known : | { ; ) = Σdij | λ ; ) | Xi ) = Σcij | X ; ) 2 | Xi ) , | X ; ) form orthonormal ...
... photon ) . We want to compute ( X ; | TX ; ) . We expand | X ; ) into a set of states | A ) whose scattering and absorption in the target we assume known : | { ; ) = Σdij | λ ; ) | Xi ) = Σcij | X ; ) 2 | Xi ) , | X ; ) form orthonormal ...
Page 41
... photons exhibit shadowing . The total photo cross sections for complex nuclei vary approximately as A ° .9 in the few GeV energy range . It is very suggestive then to accept that photons have 41.
... photons exhibit shadowing . The total photo cross sections for complex nuclei vary approximately as A ° .9 in the few GeV energy range . It is very suggestive then to accept that photons have 41.
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 |
| Export Citation | BiBTeX EndNote RefMan |