Interactions of High Energy Particles with Nuclei |
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Page 3
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 ...
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 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 ...
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 formula.
... 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 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 ) .
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 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 ...
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 ...
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