## Interactions of High Energy Particles with Nuclei |

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Work on

Work on

**vector meson**production on nuclei or 31 ( 51 ) coherent diffractive production ( compare refs . [ S3 , S4 , S5 ] ) ' is a good example of the role of nuclear targets . One observed also excitations of specific nuclear levels by ... Page 9

Let us consider a vector particle ( hence a very relevant kind of particle to our further analysis ) . Example 2. Scattering of a charged

Let us consider a vector particle ( hence a very relevant kind of particle to our further analysis ) . Example 2. Scattering of a charged

**vector meson**in a static field ( we shall quote the results , for more details see refs . Page 38

Our description also contains , as a special case , the so - called

Our description also contains , as a special case , the so - called

**vector meson**dominance models which are employed to describe interactions with hadronic targets at high energy , a process which will be discussed later . Page 41

Example 3 : Photoprocesses and

Example 3 : Photoprocesses and

**vector meson**dominance : It is now a well established fact that , at high energy , photons exhibit shadowing . The total photo cross sections for complex nuclei vary approximately as A0.9 in the few GeV ... Page 42

Since we know strongly interacting

Since we know strongly interacting

**vector mesons**with the same quantum numbers as the photon , the simplest possible assumption one can make is to accept that the o , n ) states are dominated by a**vector meson**( or mesons ) .### 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 hadrons Hence high energy limit important incident particle inelastic initial Institute interactions introduce magnetic mass materials measurement momentum transfer multiple scattering National Bureau Note nuclear nuclear targets nuclei nucleon numbers objects obtained parameters phase shifts photon photoproduction physical position possible problem profiles shadowing single Standards step strong structure technical vector meson wave function