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

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**complete**and consistent system of physical measurement ; coordinates that system with measurement systems of other nations ; and furnishes essential services leading to accurate and uniform physical measurements throughout the Nation's ... Page 4

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**complete**analysis one can perform is presumably to employ the Watson multiple scattering theory , but we shall not present it here . In fact it is amazing that ( 2.1 ) works so well . Even in the conceptually simplest cases of rela ... Page 20

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**complete**amplitude by adding and subtracting a Coulomb point charge amplitude : M = ik = 00 db bJ , ( Ab ) [ 1 − exp ( ix . ” ( b ) ) ] + ik [ * db bJo ( Ab ) exp [ ix . ” ( b ) + ix . ( b ) ] · Mc ( P ) + ik 5 00 0 db bJo ( Ab ) [ exp ... Page 38

... with hadronic targets at high energy , a process which will be discussed later . Example 1 : The processes of QED : ( a ) Bremsstrahlung : the Feynman diagrams हु Z AND давно go over to AND where the dot means that

... with hadronic targets at high energy , a process which will be discussed later . Example 1 : The processes of QED : ( a ) Bremsstrahlung : the Feynman diagrams हु Z AND давно go over to AND where the dot means that

**complete**38. Page 39

Wiesław Czyż. go over to AND where the dot means that

Wiesław Czyż. go over to AND where the dot means that

**complete**( to all orders ) elastic scattering amplitudes are to be inserted and the vertices are given by di ; coefficients analogous to the ones in eqs ( 4.5 ) , ( 4.6 ) , and ( 4.7 ) ...### 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