## Interactions of High Energy Particles with Nuclei |

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[ S3 , S4 , S5 ] ) ' is a good

[ S3 , S4 , S5 ] ) ' is a good

**example**of the role of nuclear targets . One observed also excitations of specific nuclear levels by high energy hadrons [ 1 , 2 ] . This opens a possibility [ 2 ] of selecting diffractive productions with ... Page 4

**Examples Example**1. Dirac particle with anomalous magnetic moment in a given electromagnetic static field ( notation from Bjorken and Drell [ 87 ] ) : ке iv( i - ex + „ Po m ) --- ix - Our = 0 , 4m ке where X = yoA - YA , i Our = 2 ( y ... Page 9

This is true , but one can give some other - though much more complex --

This is true , but one can give some other - though much more complex --

**examples**of scattering from a classical ...**Example**2. Scattering of a charged vector meson in a static field ( we shall quote the results , for more details see ... Page 10

To conclude this section we may say that

To conclude this section we may say that

**Examples**1 and 2 warn us that if the strong interactions are mediated through vector fields ( analogous to the electromagnetic field ) one can expect the " principle of additivity of phase shifts ... Page 12

We already saw in the

We already saw in the

**examples**of scattering of relativistic particles from external electromagnetic fields that " internal structure ” ( in these cases the internal spin quantum numbers + anomalous magnetic moment ) breaks down the ...### What people are saying - Write a review

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### Common terms and phrases

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