Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Page 14
... Glauber model with additivity of all possible phase shifts of the pairs of components of ( a ) and ( b ) . Let us consider some limiting cases of eq ( 3.2 ) ( compare ref . [ 12 ] ) . Let the radii of the two composite objects be R. and ...
... Glauber model with additivity of all possible phase shifts of the pairs of components of ( a ) and ( b ) . Let us consider some limiting cases of eq ( 3.2 ) ( compare ref . [ 12 ] ) . Let the radii of the two composite objects be R. and ...
Page 18
... 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 shadowing phenomena ...
... 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 shadowing phenomena ...
Page 23
... Glauber in ref . [ S2 ] ) . When we want to discuss light nuclei we have to consider carefully the motion of the center of mass . Take , for example , a deuteron : here taking into account the c.m. motion is trivially accom- plished by ...
... Glauber in ref . [ S2 ] ) . When we want to discuss light nuclei we have to consider carefully the motion of the center of mass . Take , for example , a deuteron : here taking into account the c.m. motion is trivially accom- plished by ...
Page 27
... Glauber model , it is enough to have p ( s ) = √∞ dzó 。* ( s , z ) Þo ( s , z ) to 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 ...
... Glauber model , it is enough to have p ( s ) = √∞ dzó 。* ( s , z ) Þo ( s , z ) to 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 ...
Page 36
... Glauber ) from ( | T | ñ ) and ( ñ | T | ñ ) pion - nucleon and neutron - nucleon elastic scattering amplitudes [ 29 ] . Suppose the target is a nucleus : everything goes the same way except that elastic scattering amplitudes are taken ...
... Glauber ) from ( | T | ñ ) and ( ñ | T | ñ ) pion - nucleon and neutron - nucleon elastic scattering amplitudes [ 29 ] . Suppose the target is a nucleus : everything goes the same way except that elastic scattering amplitudes are taken ...
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