## Interactions of High Energy Particles with Nuclei |

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Page 12

For the sake of simplicity let us take the wave functions of ( a ) and ( b ) in the form of products of

For the sake of simplicity let us take the wave functions of ( a ) and ( b ) in the form of products of

**single**particle wave functions . Let us assume also that all particles have the same**single**particle wave functions . Page 25

A geometrical picture of

A geometrical picture of

**single**- , double- , etc. scattering contributions is as follows : log | m |**Single**( positive ) Double ( negative ) Triple ( positive ) 42 ( ii ) With this picture it is easy to establish the existence of ... Page 26

In fact the ( m | | m ' ) contributions are indeed the most important but they always lead to a sharp diffractive minimum : log doel dA 2 DEUTERON TARGET

In fact the ( m | | m ' ) contributions are indeed the most important but they always lead to a sharp diffractive minimum : log doel dA 2 DEUTERON TARGET

**SINGLE**DOUBLE 12 A But ( m | S12 m ' ) # 0 in general ( also ( m | S12 S12 | m ... Page 38

This represents both

This represents both

**single**and double scattering of the n- system This represents both**single**and double scattering of the n- system . р - in which the diffractive elastic scattering occurs either before or after the fluctuation takes ... Page 43

When the VMD model does reproduce the correct total photon - nucleon cross section the contribution given above is just a

When the VMD model does reproduce the correct total photon - nucleon cross section the contribution given above is just a

**single**scattering contribution of the multiple scattering of vector mesons and is properly taken care of by the ...### What people are saying - Write a review

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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