Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 53
... photon cross sections . ) From the above description and the inspection of the data shown in ref [ 40 ] one sees that there are several points which bring about uncertainties in such an analysis . These uncertainties arise because one ...
... photon cross sections . ) From the above description and the inspection of the data shown in ref [ 40 ] one sees that there are several points which bring about uncertainties in such an analysis . These uncertainties arise because one ...
Page 54
... photon interactions with hadronic targets ( which include nuclei ) . 1. We considered the high energy limit of elastic scattering of photons by nucleons and nuclei . We discussed the evidence for the existence , in the physical high ...
... photon interactions with hadronic targets ( which include nuclei ) . 1. We considered the high energy limit of elastic scattering of photons by nucleons and nuclei . We discussed the evidence for the existence , in the physical high ...
Page 55
... photons were not attenuated due to the weakness of electromagnetic interactions ) . Let us make this extension explicitly and obtain the so - called " one step " model for diffractive production of hadrons in hadron- nucleus collisions ...
... photons were not attenuated due to the weakness of electromagnetic interactions ) . Let us make this extension explicitly and obtain the so - called " one step " model for diffractive production of hadrons in hadron- nucleus collisions ...
Page 59
... the composition of | KL ) = 1 / √2 ( | Ko ) + | Řo ) ) and | K . ) = 1 / √2 ( | Ko ) — | Ko ) ) which is nonperturbative , hence fundamentally different from the y— V structure of the photon . In fact , accepting the 59.
... the composition of | KL ) = 1 / √2 ( | Ko ) + | Řo ) ) and | K . ) = 1 / √2 ( | Ko ) — | Ko ) ) which is nonperturbative , hence fundamentally different from the y— V structure of the photon . In fact , accepting the 59.
Page 60
Wiesław Czyż. structure of the photon . In fact , accepting the fact that Ko and Ão scatter only elastically from the nucleus we get the formula which is correct : M ( KL → K . ) = ik 2π d2b exp ( i △ b ) { exp [ −1⁄2oà ° ' T ( b ) ...
Wiesław Czyż. structure of the photon . In fact , accepting the fact that Ko and Ão scatter only elastically from the nucleus we get the formula which is correct : M ( KL → K . ) = ik 2π d2b exp ( i △ b ) { exp [ −1⁄2oà ° ' T ( b ) ...
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