Interactions of High Energy Particles with Nuclei |
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Page 2
So , the crucial point in our discussion is an understanding of a multiple scattering process of strongly interacting particles inside of nuclear matter ( or more generally : just a multiple scattering process with forces strong enough ...
So , the crucial point in our discussion is an understanding of a multiple scattering process of strongly interacting particles inside of nuclear matter ( or more generally : just a multiple scattering process with forces strong enough ...
Page 10
To conclude this section we may say that Examples 1 and 2 warn us that if the strong interactions are mediated through vector fields ( analogous to the electromagnetic field ) one can expect the " principle of additivity of phase shifts ...
To conclude this section we may say that Examples 1 and 2 warn us that if the strong interactions are mediated through vector fields ( analogous to the electromagnetic field ) one can expect the " principle of additivity of phase shifts ...
Page 19
We shall assume that , in the high energy limit , the total phase shift is the sum of the Coulomb phase shift ( xc , the phase shift one would get if the strong interactions were switched off ) and the strong interaction phase shift ...
We shall assume that , in the high energy limit , the total phase shift is the sum of the Coulomb phase shift ( xc , the phase shift one would get if the strong interactions were switched off ) and the strong interaction phase shift ...
Page 39
... from the above two Feynman diagrams in fact , more complete ) but in total agreement with the Bethe and Maximon formulae [ 34 ] for the high energy limit of the pair production cross section in a strong Coulomb field [ 35 ] .
... from the above two Feynman diagrams in fact , more complete ) but in total agreement with the Bethe and Maximon formulae [ 34 ] for the high energy limit of the pair production cross section in a strong Coulomb field [ 35 ] .
Page 42
More precisely : as far as strong interactions go , it is physical . The situation is very similar to that in the K1 - K , regeneration problem : we are expanding our physical states into ...
More precisely : as far as strong interactions go , it is physical . The situation is very similar to that in the K1 - K , regeneration problem : we are expanding our physical states into ...
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