Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 6-10 of 15
Page 29
... compute the elastic and inelastic scattering amplitudes . Since the transmitted wave is = n , the wave which goes into scattering and production is ¥ n = nyyλeln + λinelnxe ; But hence ¥ 1 = Ny ¥ n — N2 ¥ ¤ × ¢ z ; λel = ny2 , λinel ...
... compute the elastic and inelastic scattering amplitudes . Since the transmitted wave is = n , the wave which goes into scattering and production is ¥ n = nyyλeln + λinelnxe ; But hence ¥ 1 = Ny ¥ n — N2 ¥ ¤ × ¢ z ; λel = ny2 , λinel ...
Page 30
... compute ( X ; | TX ; ) . We expand | X ; ) into a set of states | A ) whose scattering and absorption in the target we assume known : | { ; ) = Σdij | λ ; ) | Xi ) = Σcij | X ; ) 2 | Xi ) , | X ; ) form orthonormal sets ( 4.1 ) of ...
... compute ( X ; | TX ; ) . We expand | X ; ) into a set of states | A ) whose scattering and absorption in the target we assume known : | { ; ) = Σdij | λ ; ) | Xi ) = Σcij | X ; ) 2 | Xi ) , | X ; ) form orthonormal sets ( 4.1 ) of ...
Page 31
... compute them . We shall give some examples further in the text . How does one implement this program ? There are strongly interacting particles which realize precisely the above outlined scheme and we even know d ;; ' s and 7 , ' s ...
... compute them . We shall give some examples further in the text . How does one implement this program ? There are strongly interacting particles which realize precisely the above outlined scheme and we even know d ;; ' s and 7 , ' s ...
Page 35
... Compute the transition matrix element by making the components scatter elastically from the target . If one can implement such a program , one can treat diffractive production processes on nucleons ( elementary targets ) and nuclei ...
... Compute the transition matrix element by making the components scatter elastically from the target . If one can implement such a program , one can treat diffractive production processes on nucleons ( elementary targets ) and nuclei ...
Page 36
... computed à la Glauber [ 29 ] , [ S4 ] . The standard noncovariant perturbation theory is an " obvious " tool to construct such states . Let H ' be the interaction Hamiltonian which couples the states | p ) and | ññ ) . Let this coupling ...
... computed à la Glauber [ 29 ] , [ S4 ] . The standard noncovariant perturbation theory is an " obvious " tool to construct such states . Let H ' be the interaction Hamiltonian which couples the states | p ) and | ññ ) . Let this coupling ...
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