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

### From inside the book

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**approximately**exhaust the list of processes contributing to elastic scattering . From our discussion of the components of σTOT ( σel , σDT , σPROD ) it follows that the measure- ments of σror may be a good way of finding out whether the ... Page 21

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**approximately**the same as Re M without xe ! This is true for 208 Pb . In general one gets all kinds of intermediate situations . In any case , the influence of the Coulomb interaction is very important " everywhere " as the figure below ... Page 36

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**approximately**( compare eq ( 4.4 ) ) The production amplitude is : p≈p , + p≈π + р . Msi = ( p | T | p ) d1o d1⁄2 TM ” + ( ññ | Т | ññ ) d1⁄2o d ̧ TM ” . Suppose the target is a nucleon , then ( p | Tp ) is taken to be the proton ... Page 41

... fact that , at high energy , photons exhibit shadowing . The total photo cross sections for complex nuclei vary

... fact that , at high energy , photons exhibit shadowing . The total photo cross sections for complex nuclei vary

**approximately**as A ° .9 in the few GeV energy range . It is very suggestive then to accept that photons have 41. Page 45

... a purely electromagnetic interaction to obtain a contribution ~ A . It could come from a heavy vector boson whose 1≈ 2w My2 << R is still short because its rest mass is large . Conclusion : The VMD model is only

... a purely electromagnetic interaction to obtain a contribution ~ A . It could come from a heavy vector boson whose 1≈ 2w My2 << R is still short because its rest mass is large . Conclusion : The VMD model is only

**approximately**correct . 45.### 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