## Interactions of High Energy Particles with Nuclei |

### From inside the book

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Page 18

In fact such an analysis has recently been done for - d scattering and seems to indicate the

In fact such an analysis has recently been done for - d scattering and seems to indicate the

**existence**of such a discrepancy for energies above ~ 40 GeV [ 48 ] . The remaining important corrections to be discussed ( although they are ... Page 25

A geometrical picture of single- , double- , etc. scattering contributions is as follows : log / ml Single ( positive ) Double ( negative ) Triple ( positive ) A2 ( ii ) With this picture it is easy to establish the

A geometrical picture of single- , double- , etc. scattering contributions is as follows : log / ml Single ( positive ) Double ( negative ) Triple ( positive ) A2 ( ii ) With this picture it is easy to establish the

**existence**of ... Page 26

( ii ) One can also see ( again , compare [ S1 ] ) how important the deformation of the target is (

( ii ) One can also see ( again , compare [ S1 ] ) how important the deformation of the target is (

**existence**of the D - state in the deuteron ground state ) . Let us discuss this effect in more detail . The ground state deuteron wave ... Page 32

TARGET WHERE ko ARE CREATED ~ 50 % of ki DECAY FASTER DECAY SLOWER KO ~ 50 % of Kit DISTANCE FROM THE TARGET So , after some distance only the K2 beam is in

TARGET WHERE ko ARE CREATED ~ 50 % of ki DECAY FASTER DECAY SLOWER KO ~ 50 % of Kit DISTANCE FROM THE TARGET So , after some distance only the K2 beam is in

**existence**. Page 52

There are a few points which should be stressed again at this stage : ( i ) This is the most direct measurement of the elastic p - nucleon cross section in

There are a few points which should be stressed again at this stage : ( i ) This is the most direct measurement of the elastic p - nucleon cross section in

**existence**. ( ii ) If one wants to extract op or 7/47 , one can do it very ...### 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