Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 14
... incident particle is decisive in destroying or satisfying additivity . The other " moral " is that if we know the structure of the com- posite body ( b ) we may still use a generalized Glauber model with additivity of all possible phase ...
... incident particle is decisive in destroying or satisfying additivity . The other " moral " is that if we know the structure of the com- posite body ( b ) we may still use a generalized Glauber model with additivity of all possible phase ...
Page 15
... proton charge form factors from elastic scattering hadron - hadron cross sections . ( ii ) predict diffractive ... particle gets removed from the incident beam is 1— | 1 — y ( b ) | 2 = 2 Rey ( b ) ( b ) 2 ( at the impact parameter ...
... proton charge form factors from elastic scattering hadron - hadron cross sections . ( ii ) predict diffractive ... particle gets removed from the incident beam is 1— | 1 — y ( b ) | 2 = 2 Rey ( b ) ( b ) 2 ( at the impact parameter ...
Page 16
... -1- ( r ) 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 physically different contributions : 16.
... -1- ( r ) 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 physically different contributions : 16.
Page 18
... incident particle . Earlier in these notes we gave some examples of such cases . To analyze this problem in more detail , one has to link it with diffractive production processes and we shall postpone such a discussion until our ...
... incident particle . Earlier in these notes we gave some examples of such cases . To analyze this problem in more detail , one has to link it with diffractive production processes and we shall postpone such a discussion until our ...
Page 27
... incident particle ( the M ( △ , s ) operator does not act on spin quantum numbers . ) All the other spin effects are presumably not important . ( iii ) Calculations such as the one above , as well as more sophisticated calculations ...
... incident particle ( the M ( △ , s ) operator does not act on spin quantum numbers . ) All the other spin effects are presumably not important . ( iii ) Calculations such as the one above , as well as more sophisticated calculations ...
Common terms and phrases
absorption additivity of phase anomalous magnetic moment ú approximately assume attenuation b+½s beam Bureau of Standards coherent diffractive production collision Compton scattering compute Coulomb interactions Czyż d³r db exp i▲·b deuteron diagonalization diffractive production processes diffractive scattering discussed double scattering elastic scattering amplitude electromagnetic equation example excited experiments factor Feynman diagrams formula four-momentum Glauber model hadrons Hence high energy limit incident particle incident wave inelastic shadowing Interactions of High invariant mass K mesons multiple scattering National Bureau neutrino neutrons ññ Note nuclear matter nuclear targets nuclei nucleon obtained optical theorem parameters phase shifts photon photoproduction of vector physical pion production amplitude profiles quantum numbers regeneration Řº shadowing effects single scattering spin strongly interacting target nucleus total cross section vector meson VMD model wave function γν Σ Σ