## Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |

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Page 49

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**positions**z , the 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 ... Page 65

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**position**of these physical states propagating through the nuclear matter , a superposition in which both these states are equally important . Now let us go back and close our discussion of the coherent diffractive production by pions of ...### Common terms and phrases

absorption additivity of phase anomalous magnetic moment Ãº 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