Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 13
... EXCITED STATES Suppose we reject the intermediate excited states and take only the ground state as a possible inter- mediate state ( this is the way to eliminate all channels but one ) . Then each y ; can be averaged over r1 ( b ) ...
... EXCITED STATES Suppose we reject the intermediate excited states and take only the ground state as a possible inter- mediate state ( this is the way to eliminate all channels but one ) . Then each y ; can be averaged over r1 ( b ) ...
Page 14
... excited states , neither of ( b ) nor of ( a ) . So , the Chou & Yang [ 13 ] limit A , B → looses all excited state contributions and becomes ( 3.4 ) . Equation ( 3.4 ) gives the well - known " droplet model " [ 13 ] elastic scattering ...
... excited states , neither of ( b ) nor of ( a ) . So , the Chou & Yang [ 13 ] limit A , B → looses all excited state contributions and becomes ( 3.4 ) . Equation ( 3.4 ) gives the well - known " droplet model " [ 13 ] elastic scattering ...
Page 18
... excited states of the projectile present at intermediate steps ) are excluded . O O O They are the source of the so - called inelastic screening ( or inelastic shadowing ) phenomenon [ 47 ] . In order to include them we have to ascribe ...
... excited states of the projectile present at intermediate steps ) are excluded . O O O They are the source of the so - called inelastic screening ( or inelastic shadowing ) phenomenon [ 47 ] . In order to include them we have to ascribe ...
Page 62
... excited states . This makes good sense if one believes ( following Good and Walker [ 23 ] ) that in the high energy limit the ground and excited states of the incident system ( e.g. , a pion ) are considered to be approximately ...
... excited states . This makes good sense if one believes ( following Good and Walker [ 23 ] ) that in the high energy limit the ground and excited states of the incident system ( e.g. , a pion ) are considered to be approximately ...
Page 65
... excited states | m ) from which the system | 2 ) emerges . On the mass scale M ( mass ) m states < m | 5 | m > < mc1 weak transition the ground state which does not " mix " with m - states . Its elastic scattering profile is < 1 | r | 1 > ...
... excited states | m ) from which the system | 2 ) emerges . On the mass scale M ( mass ) m states < m | 5 | m > < mc1 weak transition the ground state which does not " mix " with m - states . Its elastic scattering profile is < 1 | r | 1 > ...
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