## Interactions of High Energy Particles with Nuclei |

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Page 9

Scattering of a

Scattering of a

**charged**vector meson in a static field ( we shall quote the results , for more details see refs . [ 9 , 10 ] ) . Let us allow for our vector particle to have an arbitrary magnetic moment and define the magnetic moment ... Page 10

In order to make the condition ( 2.7 ) more plausible , let us consider a

In order to make the condition ( 2.7 ) more plausible , let us consider a

**charged**particle with spin S and magnetic moment M given by ( 2.7 ) moving in an almost uniform magnetic field B. This particle follows a circular trajectory with ... Page 15

If we accept that the densities of hadronic matter are the same as

If we accept that the densities of hadronic matter are the same as

**charge**densities , F ( a ) , F ( b ) are the F**charge**form factors of the colliding hadrons . This formula was used successfully to : ( i ) reproduce the proton**charge**... Page 18

... corrections to be discussed ( although they are , in principle , included in the algorithm presented above ) are : ( i ) the Coulomb corrections which play an important role in elastic scattering from nuclei of

... corrections to be discussed ( although they are , in principle , included in the algorithm presented above ) are : ( i ) the Coulomb corrections which play an important role in elastic scattering from nuclei of

**charged**hadrons , and ... Page 19

This last expression is the Coulomb phase shift produced by a point

This last expression is the Coulomb phase shift produced by a point

**charge**. ... But we do know the analytic expression for the Coulomb scattering amplitude of point - like**charges**: > M. ( P ) = ik = | db exp 19.### What people are saying - Write a review

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