Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 6-10 of 12
Page 27
... introducing relativistic deformations occurs - modeled on QED ! These and other related problems have been discussed in a series of papers by Cheng and Wu [ 21 , 22 ] ( see also [ 30 ] , [ S4 ] ) . 4. Diffractive Dissociation and ...
... introducing relativistic deformations occurs - modeled on QED ! These and other related problems have been discussed in a series of papers by Cheng and Wu [ 21 , 22 ] ( see also [ 30 ] , [ S4 ] ) . 4. Diffractive Dissociation and ...
Page 29
... introduce partial absorption ( in general different for the two components ( x , y ) ) . The incident wave : The transmitted wave : The scattered wave : and we get ¥ n = n2 ¥ z + ny ❤ = nzNz ¥ x + Nyny ¥ v Y2 = ( 1 - nz ) n2 ¥ z + ( 1 ...
... introduce partial absorption ( in general different for the two components ( x , y ) ) . The incident wave : The transmitted wave : The scattered wave : and we get ¥ n = n2 ¥ z + ny ❤ = nzNz ¥ x + Nyny ¥ v Y2 = ( 1 - nz ) n2 ¥ z + ( 1 ...
Page 30
... introduce the physical states of the system , | X ; ) ( which are analogous to the states „ and nye , of the photon ) . We want to compute ( X ; | TX ; ) . We expand | X ; ) into a set of states | A ) whose scattering and absorption in ...
... introduce the physical states of the system , | X ; ) ( which are analogous to the states „ and nye , of the photon ) . We want to compute ( X ; | TX ; ) . We expand | X ; ) into a set of states | A ) whose scattering and absorption in ...
Page 35
... introduce some important corrections at low energies . But in the limit of very high energies and small momentum transfer , all such effects dis- appear . Let us take , e.g. , two such states and give them the same momentum p . Then ...
... introduce some important corrections at low energies . But in the limit of very high energies and small momentum transfer , all such effects dis- appear . Let us take , e.g. , two such states and give them the same momentum p . Then ...
Page 54
... of vector mesons on nuclear targets we can easily remedy this situation . So , the only change we should introduce into the formulae given for vector meson photoproduction is an attenuation of the incident beam of 54.
... of vector mesons on nuclear targets we can easily remedy this situation . So , the only change we should introduce into the formulae given for vector meson photoproduction is an attenuation of the incident beam of 54.
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