Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 30
... collision then contains , in general , a new particle ( or a collection of new particles ) . First we introduce the physical states of the system , | X ; ) ( which are analogous to the states „ and nye , of the photon ) . We want to ...
... collision then contains , in general , a new particle ( or a collection of new particles ) . First we introduce the physical states of the system , | X ; ) ( which are analogous to the states „ and nye , of the photon ) . We want to ...
Page 31
... collision of strongly interacting particles : K ° and K ° ( they are different because they have opposite strangeness , unlike pions where are identical to ! ) which have the same masses , and thus can be considered as a two component ...
... collision of strongly interacting particles : K ° and K ° ( they are different because they have opposite strangeness , unlike pions where are identical to ! ) which have the same masses , and thus can be considered as a two component ...
Page 35
... collision is very small and we have exp [ -i ( E— E * ) τ ] ~ 1 to very good accuracy . In fact the same argument shows that the incident state and the produced state can also be considered degenerate in the limit p → ( the fact that p ...
... collision is very small and we have exp [ -i ( E— E * ) τ ] ~ 1 to very good accuracy . In fact the same argument shows that the incident state and the produced state can also be considered degenerate in the limit p → ( the fact that p ...
Page 45
... colliding beam experiments . So , it is un- likely that one should reduce it by a factor of almost 2 ! ( Unless there is a strong dependence on the invariant mass of a virtual photon ) . One can also get the correct answer when one ...
... colliding beam experiments . So , it is un- likely that one should reduce it by a factor of almost 2 ! ( Unless there is a strong dependence on the invariant mass of a virtual photon ) . One can also get the correct answer when one ...
Page 54
... Collisions The Standard Analysis We have already discussed some general features of diffractive production processes by hadrons ( in the limit of very high energy ) . Let us now look into a few details of such processes with special ...
... Collisions The Standard Analysis We have already discussed some general features of diffractive production processes by hadrons ( in the limit of very high energy ) . Let us now look into a few details of such processes with special ...
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