Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 1-5 of 15
Page 18
... computed σTOT from the Glauber model ( including all possible effects which the model allows for ) and then found a definite dis- crepancy with experimentally measured Tor - it would very strongly suggest the existence of inelastic ...
... computed σTOT from the Glauber model ( including all possible effects which the model allows for ) and then found a definite dis- crepancy with experimentally measured Tor - it would very strongly suggest the existence of inelastic ...
Page 19
... compute the amplitude one has to bear in mind that at large b , x . ( b ) behaves like a Coulomb phase shift produced by a point charge and hence diverges logarithmically . But we do know the analytic expression for the Coulomb ...
... compute the amplitude one has to bear in mind that at large b , x . ( b ) behaves like a Coulomb phase shift produced by a point charge and hence diverges logarithmically . But we do know the analytic expression for the Coulomb ...
Page 20
... computed numerically Ze2 Xc ( b ) = - v [ ** dz [ d3r ' PA ( ) | r - r ' | = where r ( b , z ) . Note that dz lim xa ( b ) = v Ze2 [ ** def d''PA ( 1 ) Hence , for large b , xc ( b ) → xc2 ( b ) and the integral for M converges . Let ...
... computed numerically Ze2 Xc ( b ) = - v [ ** dz [ d3r ' PA ( ) | r - r ' | = where r ( b , z ) . Note that dz lim xa ( b ) = v Ze2 [ ** def d''PA ( 1 ) Hence , for large b , xc ( b ) → xc2 ( b ) and the integral for M converges . Let ...
Page 23
... compute the correction factor to M = ( M ( △ ; 81 ... SA ) ) assuming the wave function to be in the form of a product of the c.m. wave function and the internal wave function . M = ( R ( r ) | exp ( i △ ⋅r ) | R ( r ) ) ( Þ 。( rı ...
... compute the correction factor to M = ( M ( △ ; 81 ... SA ) ) assuming the wave function to be in the form of a product of the c.m. wave function and the internal wave function . M = ( R ( r ) | exp ( i △ ⋅r ) | R ( r ) ) ( Þ 。( rı ...
Page 27
... compute the cross section . Suppose there is some deformation in the final state : Po * ( s , 2 ) → o ' * ( A , s , z ) ( one can assume that the deformation is defined by the momentum transfer A ) . Then we should replace p ( 8 ) → I ...
... compute the cross section . Suppose there is some deformation in the final state : Po * ( s , 2 ) → o ' * ( A , s , z ) ( one can assume that the deformation is defined by the momentum transfer A ) . Then we should replace p ( 8 ) → I ...
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