## Interactions of High Energy Particles with Nuclei |

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Page 38

Hence one can use the same technique to

Hence one can use the same technique to

**describe**the processes on simple and composite ( e.g. , nuclei ) targets ( S4 ] . Relation of the above model to some well established techniques of**describing**diffractive dissociation . Page 46

27 M ( 7V ) is given graphically below rum v In the high energy limit ( wo ) one can also

27 M ( 7V ) is given graphically below rum v In the high energy limit ( wo ) one can also

**describe**this process as follows : the photon penetrates the nucleus up to a certain point where it converts into a V meson which scatters ... Page 51

Just to give some idea of how the results look , let us

Just to give some idea of how the results look , let us

**describe**briefly the results of po photoproduction on deuterium ( R. L. Anderson et al . [ 39 ] ) and a DESY - MIT experiment ( H. Alvensleben et al . Page 60

( From ( 5.5 ) one can see again that the " one step ” formula ( 5.3 ) is incapable of

( From ( 5.5 ) one can see again that the " one step ” formula ( 5.3 ) is incapable of

**describing**K1 - K , regeneration on nuclei ) . Let us go back to the general case of incoming particle 1 and outgoing particle 2. Page 61

( In the weak coupling case ” it is physically more accurate to

( In the weak coupling case ” it is physically more accurate to

**describe**the initial and final states as composed , approximately , of one and three particles , respectively . ) Note the following amusing point : Assuming | * ) to be in ...### 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