Interactions of High Energy Particles with Nuclei |
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Page 3
Yi , ( 2.1 ) 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 ...
Yi , ( 2.1 ) 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 ...
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
... t ( b − 8 , ® ) which is the profile for elastic scattering of ( b ) from the jth nucleon of ( a ) and a two - dimensional density p ( s ) = ƒ ** dz 4o * ( r ) ço ( r ) . 81 Then the additivity of phase shifts gives us the formula 121.
... t ( b − 8 , ® ) which is the profile for elastic scattering of ( b ) from the jth nucleon of ( a ) and a two - dimensional density p ( s ) = ƒ ** dz 4o * ( r ) ço ( r ) . 81 Then the additivity of phase shifts gives us the formula 121.
Page 13
Then the additivity of phase shifts gives us the formula : ik M = 2π | 2bexp ( ia + b ) / 8 ) ... d8 , II , ( , ) ( a ) » Î » « ( 9 , - ) { 1– ÎI ( 1 − r , ( b − x / ... ) ) } . j p ( a ) ( 1 - г ; ( b - s , 8,0 ) ) } .
Then the additivity of phase shifts gives us the formula : ik M = 2π | 2bexp ( ia + b ) / 8 ) ... d8 , II , ( , ) ( a ) » Î » « ( 9 , - ) { 1– ÎI ( 1 − r , ( b − x / ... ) ) } . j p ( a ) ( 1 - г ; ( b - s , 8,0 ) ) } .
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 ] ) : lim M = A ...
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 ] ) : lim M = A ...
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Bibliographic information
| Title | Interactions of High Energy Particles with Nuclei Volume 139 of NBS monograph |
| Author | Wiesław Czyż |
| Publisher | National Bureau of Standards, 1975 |
| Original from | the University of Michigan |
| Digitized | 21 Nov 2007 |
| Length | 69 pages |
| Export Citation | BiBTeX EndNote RefMan |