Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 61
... initial beam , thus making this concern irrevelant . This example shows that one can easily explain the " anomalously " low absorption of diffrac- tively produced objects if one assumes that the initial ( one pion ) and the final ...
... initial beam , thus making this concern irrevelant . This example shows that one can easily explain the " anomalously " low absorption of diffrac- tively produced objects if one assumes that the initial ( one pion ) and the final ...
Page 63
... initial state of the incident particle and some other states one may reduce considerably the absorption of the initial state in nuclear matter . One can put it differently : the effect of allowing intermediate states to occur during the ...
... initial state of the incident particle and some other states one may reduce considerably the absorption of the initial state in nuclear matter . One can put it differently : the effect of allowing intermediate states to occur during the ...
Page 64
Wiesław Czyż. 11 ) NUCLEUS 12 ) 3π elastic scatting of the initial particle scattering of the final object with many different intermediate states This is , at the moment , the most commonly considered model of coherent diffractive ...
Wiesław Czyż. 11 ) NUCLEUS 12 ) 3π elastic scatting of the initial particle scattering of the final object with many different intermediate states This is , at the moment , the most commonly considered model of coherent diffractive ...
Page
... initial distribution is handled by the sponsor ; public distribution is by the National Technical Information Service ( Springfield , Va . 22161 ) in paper copy or microfiche form . Order NBS publications ( except NBSIR's and Biblio ...
... initial distribution is handled by the sponsor ; public distribution is by the National Technical Information Service ( Springfield , Va . 22161 ) in paper copy or microfiche form . Order NBS publications ( except NBSIR's and Biblio ...
Common terms and phrases
absorption additivity of phase anomalous magnetic moment ú approximately assume attenuation b+½s beam Bureau of Standards coherent diffractive production collision Compton scattering compute Coulomb interactions Czyż d³r db exp i▲·b deuteron diagonalization diffractive production processes diffractive scattering discussed double scattering elastic scattering amplitude electromagnetic equation example excited experiments factor Feynman diagrams formula four-momentum Glauber model hadrons Hence high energy limit incident particle incident wave inelastic shadowing Interactions of High invariant mass K mesons multiple scattering National Bureau neutrino neutrons ññ Note nuclear matter nuclear targets nuclei nucleon obtained optical theorem parameters phase shifts photon photoproduction of vector physical pion production amplitude profiles quantum numbers regeneration Řº shadowing effects single scattering spin strongly interacting target nucleus total cross section vector meson VMD model wave function γν Σ Σ