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