Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 1
... problems related to the interactions of hadrons , photons , and electrons ( virtual photons ) with nuclei - we must choose a certain point of view which unifies all these problems . The common denominator which we shall emphasize is the ...
... problems related to the interactions of hadrons , photons , and electrons ( virtual photons ) with nuclei - we must choose a certain point of view which unifies all these problems . The common denominator which we shall emphasize is the ...
Page 7
... problem . We can also make the following remark : sometimes coupled channels can be decoupled by diagonalization . · A remark about “ decoupling " channels through a diagonalization procedure Start with a generalization ( to N channels ) ...
... problem . We can also make the following remark : sometimes coupled channels can be decoupled by diagonalization . · A remark about “ decoupling " channels through a diagonalization procedure Start with a generalization ( to N channels ) ...
Page 12
... problem from the point of view of a Glauber - like description of scattering of two composite objects . The formulae given below are interesting also because they may be used to analyze high energy nucleus - nucleus collisions ( which ...
... problem from the point of view of a Glauber - like description of scattering of two composite objects . The formulae given below are interesting also because they may be used to analyze high energy nucleus - nucleus collisions ( which ...
Page 18
... problem in more detail , one has to link it with diffractive production processes and we shall postpone such a discussion until our analysis of such processes . Here , let us make only the following points : ( i ) Diffractive production ...
... problem in more detail , one has to link it with diffractive production processes and we shall postpone such a discussion until our analysis of such processes . Here , let us make only the following points : ( i ) Diffractive production ...
Page 23
... problems . Let us introduce the transverse component of the c.m. vector r = 1 A 1⁄2 Sj , and the relative coordinates which are not independent any more : s1 = s ; -r , 8 , s ' + r A Ź s ; ' = 0 = 0 . The operator M ( A ; $ 1 ... SA ) ...
... problems . Let us introduce the transverse component of the c.m. vector r = 1 A 1⁄2 Sj , and the relative coordinates which are not independent any more : s1 = s ; -r , 8 , s ' + r A Ź s ; ' = 0 = 0 . The operator M ( A ; $ 1 ... SA ) ...
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