## Interactions of High Energy Particles with Nuclei |

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( kv ) ) = 10 , kv )1 O E - Ev 7 Then the

( kv ) ) = 10 , kv )1 O E - Ev 7 Then the

**photoproduction**of V ( on a hadronic target ) has the forward amplitude Ykv | H ' | ky ) M ( 7 -- V ) = ( 0 , kv | tv 10 , kv ) E , -Ev Similarly , the elastic scattering of a high energy photon ... Page 45

e Suma v Oyn and nu ( not shown above ) from the A dependence of V

e Suma v Oyn and nu ( not shown above ) from the A dependence of V

**photoproduction**, nun was also extracted from Compton scattering and leptonic decays . From the table above one can also see that the p meson contribution is more ... Page 46

**Photoproduction**of Vector Bosons The breakdown of VMD which one sees from the results of Caldwell et al . [ 37 ] does not eliminate the possibility that the previously worked out relations between M ( 9 - p ) and M ( + p ) are good ... Page 49

They are being used in all standard analyses of

They are being used in all standard analyses of

**photoproduction**of vector bosons on nuclei [ S3 ] . Let us also quote , for the sake of completeness ( without giving derivation ) , the amplitude for elastic scattering of photons from a ... Page 50

Now let us go back to

Now let us go back to

**photoproduction**of vector mesons . The formulae discussed above were applied to analyze a multitude of experimental data . The first suggestion that one can obtain some important information on the properties of V ...### What people are saying - Write a review

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absorption additivity analysis approximately assume attenuation beam Bureau of Standards charge coherent collision complete components compute consider contribution corrections Coulomb Coulomb interactions coupling cross section db exp depend describe deuteron diffractive production processes discussed effects elastic scattering elastic scattering amplitude equation example excited existence exp ia.b 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 National Bureau Note nuclear nuclear targets nuclei nucleon numbers objects obtained parameters phase shifts photon photoproduction physical position possible present problem profiles regeneration shadowing single Standards step strong structure technical vector meson wave function