Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 45
... strong dependence on the invariant mass of a virtual photon ) . One can also get the correct answer when one accepts that there is a contribution from a Compton - like process ( not given by the VMD model ! ) which does not show any ...
... strong dependence on the invariant mass of a virtual photon ) . One can also get the correct answer when one accepts that there is a contribution from a Compton - like process ( not given by the VMD model ! ) which does not show any ...
Page 62
... strong coupling " description of diffractive production which , in contrast to the " one step " description , is not a perturbative approach : ( i ) In the " strong coupling " model there is an internal relation between elastic and ...
... strong coupling " description of diffractive production which , in contrast to the " one step " description , is not a perturbative approach : ( i ) In the " strong coupling " model there is an internal relation between elastic and ...
Page 63
... strong coupling between | 1 ) and 2 ) . Then , let us take the case where | 1 ) scatters only elastically ( hence we forbid the inter- mediate states | 2 ) ) . Then the attenuation of the incident wave is ( ii ) eik z ( 1 − ( 1 | T | 1 ) ...
... strong coupling between | 1 ) and 2 ) . Then , let us take the case where | 1 ) scatters only elastically ( hence we forbid the inter- mediate states | 2 ) ) . Then the attenuation of the incident wave is ( ii ) eik z ( 1 − ( 1 | T | 1 ) ...
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