## Interactions of High Energy Particles with Nuclei |

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So , the crucial point in our discussion is an understanding of a multiple scattering process of strongly interacting particles inside of nuclear matter ( or more generally : just a multiple scattering process with forces

So , the crucial point in our discussion is an understanding of a multiple scattering process of strongly interacting particles inside of nuclear matter ( or more generally : just a multiple scattering process with forces

**strong**enough ... Page 10

To conclude this section we may say that Examples 1 and 2 warn us that if the

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 19

We shall assume that , in the high energy limit , the total phase shift is the sum of the Coulomb phase shift ( xc , the phase shift one would get if the

We shall assume that , in the high energy limit , the total phase shift is the sum of the Coulomb phase shift ( xc , the phase shift one would get if the

**strong**interactions were switched off ) and the**strong**interaction phase shift ... Page 39

... from the above two Feynman diagrams in fact , more complete ) but in total agreement with the Bethe and Maximon formulae [ 34 ] for the high energy limit of the pair production cross section in a

... from the above two Feynman diagrams in fact , more complete ) but in total agreement with the Bethe and Maximon formulae [ 34 ] for the high energy limit of the pair production cross section in a

**strong**Coulomb field [ 35 ] . Page 42

More precisely : as far as

More precisely : as far as

**strong**interactions go , it is physical . The situation is very similar to that in the K1 - K , regeneration problem : we are expanding our physical states into ...### 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