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

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**Hadrons**- Scattering . I. Title . II . Series : United States . National Bureau of Standards . Monograph 139 . QC100.U556 No. 139 [ QC794.8.H5 ] [ 539.7'6 ] 389'.08s 74/13725 National Bureau of Standards Monograph 139 Nat . Bur . Stand ... Page 1

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**hadrons**or exhibit some**hadronic**components in such interactions . This article is divided into seven sections : ( 1 ) Introduction , ( 2 ) Description of multiple scat- tering , ( 3 ) Elastic scattering of**hadrons**from nuclei , ( 4 ) ... Page 10

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**Hadrons**from Nuclei Let us go back for a moment to scattering of incident particles whose internal structure one can neglect ( in particular the internal quantum numbers can be neglected ) . Let us start with just one scatterer : TARGET ... Page 14

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**hadron**-**hadron**scattering in the high energy limit . For example , the limit when A and B become very large was ...**hadrons**are very small ) we can write [ d ° s { a } d ° s « b > p { a } ( s { 0 } ) y ( b − s ) +8 ( a ) p ( b ) ... Page 15

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**hadrons**. This formula was used successfully to : ( i ) reproduce the proton charge form factors from elastic scattering**hadron**-**hadron**cross sections . ( ii ) predict diffractive structure ( e.g. , diffractive minima ) of the high energy ...### Common terms and phrases

absorption additivity of phase anomalous magnetic moment Ãº approximately assume attenuation beam Bureau of Standards coherent diffractive production collision Compton scattering compute Coulomb interactions Czyż d³r db bJo 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 Απ γν ΦΩ