Interactions of High Energy Particles with Nuclei |
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Page 2
The expression 1- eix ; ( b ) = Yi ( 6 ) is called the profile of the jth nucleon , incident particle collision . Assuming x ( b ) = Ï xi ( b - 8 ; ) ) and assuming that the particle goes through the target so.
The expression 1- eix ; ( b ) = Yi ( 6 ) is called the profile of the jth nucleon , incident particle collision . Assuming x ( b ) = Ï xi ( b - 8 ; ) ) and assuming that the particle goes through the target so.
Page 7
... and Q2 generated by two sources of the electromagnetic field ( at two different positions ) are , in general , noncommuting operators and there is no way of adding phase shifts ( or , equivalently , multiplying profiles ) .
... and Q2 generated by two sources of the electromagnetic field ( at two different positions ) are , in general , noncommuting operators and there is no way of adding phase shifts ( or , equivalently , multiplying profiles ) .
Page 11
... incident wave already has a profile different from unity we get : ) incident wave : g ( x , y ) eikz transmitted wave : g ( x , y ) eik2 ( 1-4 ( x , y ) ) ( this is all under the assumption z « L ) . z 2 Let us construct the " shape ...
... incident wave already has a profile different from unity we get : ) incident wave : g ( x , y ) eikz transmitted wave : g ( x , y ) eik2 ( 1-4 ( x , y ) ) ( this is all under the assumption z « L ) . z 2 Let us construct the " shape ...
Page 12
Let us look at the profile of the jth nucleon : B B T ; ( d's II “ 1,16 ) = 58 , ... " ( - > [ 1- ( 1 – ya ( b-- ) ) ] ( " ÍI ; js . ) ( ) 1 - Vic 1 1- ( 1 - Ỹ ( 6 ) B , where we assumed all profiles to be identical and introduced y Vj ...
Let us look at the profile of the jth nucleon : B B T ; ( d's II “ 1,16 ) = 58 , ... " ( - > [ 1- ( 1 – ya ( b-- ) ) ] ( " ÍI ; js . ) ( ) 1 - Vic 1 1- ( 1 - Ỹ ( 6 ) B , where we assumed all profiles to be identical and introduced y Vj ...
Page 15
... collisions ( whose scattering amplitude is determined by the profile y ( b ) ) . As the wave passes a scatterer it gets modified by a factor 1-7 ( 6 ) . Hence , the probability that the particle gets removed from the incident beam ...
... collisions ( whose scattering amplitude is determined by the profile y ( b ) ) . As the wave passes a scatterer it gets modified by a factor 1-7 ( 6 ) . Hence , the probability that the particle gets removed from the incident beam ...
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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 |