## Interactions of High Energy Particles with Nuclei |

### From inside the book

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Page 1

( b ) The very high energy

( b ) The very high energy

**incident particles**may also be important for physicists working on nuclear structure - although this point does not seem to be well established ( presumably due to poor energy resolutions of high energy beams ) ... Page 2

In other words , in all the processes we are going to discuss , strongly interacting particles appear ( as real or ... The expression 1 - eix ; ( b ) = y ; ( b ) is called the profile of the jth nucleon ,

In other words , in all the processes we are going to discuss , strongly interacting particles appear ( as real or ... The expression 1 - eix ; ( b ) = y ; ( b ) is called the profile of the jth nucleon ,

**incident particle**collision . Page 3

and assuming that the particle goes through the target so fast that all the nucleons are ' frozen ' at certain positions ... One can also use some arguments based on approximate solutions of the wave equation of the

and assuming that the particle goes through the target so fast that all the nucleons are ' frozen ' at certain positions ... One can also use some arguments based on approximate solutions of the wave equation of the

**incident particle**... Page 7

Əz m = 1 Note that " compositeness " of the

Əz m = 1 Note that " compositeness " of the

**incident particle**is responsible for the existence of more than one channel . For instance , the presence of an anomalous magnetic moment can be looked upon as a mark of " compositeness . Page 10

Elastic Scattering of Hadrons from Nuclei Let us go back for a moment to scattering of

Elastic Scattering of Hadrons from Nuclei Let us go back for a moment to scattering of

**incident particles**whose internal structure one can neglect ( in particular the internal quantum numbers can be neglected ) .### What people are saying - Write a review

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### 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