## Interactions of High Energy Particles with Nuclei |

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Page 3

One can produce many arguments which make this important

One can produce many arguments which make this important

**formula**plausible . One can use , e.g. , an optical description of attenuation of a wave penetrating a medium . One can also use some arguments based on approximate solutions of ... Page 4

There are many simplifications made in obtaining the fundamental

There are many simplifications made in obtaining the fundamental

**formula**( 2.1 ) ; the reliability of this**formula**is of primary importance . The most complete analysis one can perform is presumably to employ the Watson multiple ... Page 12

... çor % ) * ( prąk ) çu " ( 776 ) ¥ ; ( b – 5,6 " ) which is the profile for elastic scattering of ( 6 ) from the jth nucleon of ( a ) and a two - dimensional density +00 = so Then the additivity of phase shifts gives us the

... çor % ) * ( prąk ) çu " ( 776 ) ¥ ; ( b – 5,6 " ) which is the profile for elastic scattering of ( 6 ) from the jth nucleon of ( a ) and a two - dimensional density +00 = so Then the additivity of phase shifts gives us the

**formula**. Page 13

Then the additivity of phase shifts gives us the

Then the additivity of phase shifts gives us the

**formula**: ik M = | ab exp ( ia.b ) s * ( " ... dosa ( a ) d's , ” ỘI on " ( a ) { 1- ÎI ( 1 – r , ( b –s , ) pe , 1- - ) } ( - ( 3.3 ) 21 j This is different from ( 3.2 ) . Page 14

Some special cases of

Some special cases of

**formula**( 3.2 ) were also employed to describe hadron - hadron scattering in the high energy limit . For example , the limit when A and B become very large was considered [ 13 ] ( compare also [ 12 ] ) : ik lim M ...### 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