Interactions of High Energy Particles with Nuclei |
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Page 2
... of the incident particle in laboratory frame A is the two - dimensional momentum transfer b is the impact parameter xi ( b ) is the phase shift which characterizes the incident particle -- jth nucleon elastic scattering amplitude .
... of the incident particle in laboratory frame A is the two - dimensional momentum transfer b is the impact parameter xi ( b ) is the phase shift which characterizes the incident particle -- jth nucleon elastic scattering amplitude .
Page 14
... 1 ( 21 ) 2 where k is a free parameter . K If we accept that the densities of hadronic matter are 14.
... 1 ( 21 ) 2 where k is a free parameter . K If we accept that the densities of hadronic matter are 14.
Page 15
Hence , the probability that the particle gets removed from the incident beam is 1-11 - ( 6 ) 12 = 2 Rey ( 6 ) – 10 ( 6 ) | 2 ( at the impact parameter b ) . Notice that here we use the same expression as - in the following paragraphs ...
Hence , the probability that the particle gets removed from the incident beam is 1-11 - ( 6 ) 12 = 2 Rey ( 6 ) – 10 ( 6 ) | 2 ( at the impact parameter b ) . Notice that here we use the same expression as - in the following paragraphs ...
Page 16
because , due to the same arguments as before , 1-11- ( T ) | 2 gives the probability ( at the impact parameter b ) of losing the incident particle from the elastic channel . It is convenient however to split the second term into two ...
because , due to the same arguments as before , 1-11- ( T ) | 2 gives the probability ( at the impact parameter b ) of losing the incident particle from the elastic channel . It is convenient however to split the second term into two ...
Page 17
Hence 1-1 n ( b , sı ... sa ) 12 gives ( compare the formulae ( 3.5 ) of the standard partial wave analysis ) the production cross section at the impact parameter b = ( 1 + 12 ) / k with all nucleons frozen at the positions sı , ..SA .
Hence 1-1 n ( b , sı ... sa ) 12 gives ( compare the formulae ( 3.5 ) of the standard partial wave analysis ) the production cross section at the impact parameter b = ( 1 + 12 ) / k with all nucleons frozen at the positions sı , ..SA .
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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 |