Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Page 41
... forward amplitudes ) M ( b ) —— M ( c ) , and that they cancel to a large extent ( they cancel exactly in the forward direction if σpp = σpn ) . We can also see the correspondence between our diagrams and the " one pion exchange ...
... forward amplitudes ) M ( b ) —— M ( c ) , and that they cancel to a large extent ( they cancel exactly in the forward direction if σpp = σpn ) . We can also see the correspondence between our diagrams and the " one pion exchange ...
Page 42
... Ev | ky , 0 ) . Then the photoproduction of V ( on a hadronic target ) has the forward amplitude ( kv | H ' | kq ) M ( y → V ) = ( 0 , kv | tv | 0 , kv ) E - Ev Similarly , the elastic scattering of a high energy photon 42.
... Ev | ky , 0 ) . Then the photoproduction of V ( on a hadronic target ) has the forward amplitude ( kv | H ' | kq ) M ( y → V ) = ( 0 , kv | tv | 0 , kv ) E - Ev Similarly , the elastic scattering of a high energy photon 42.
Page 43
... forward amplitude M ( v → y ) = Σ ( 0 , kv | tv | 0 , kv ) ( ky | H ' | kv ) ( kv | H ' | k , ) V ( E , — Ev ) ( E , —Ev ) Graphically mly → V ) : ~ m ~ Y VP mly → y ) : Vp Vein V & V & + ( There are three known vector mesons : p , w ...
... forward amplitude M ( v → y ) = Σ ( 0 , kv | tv | 0 , kv ) ( ky | H ' | kv ) ( kv | H ' | k , ) V ( E , — Ev ) ( E , —Ev ) Graphically mly → V ) : ~ m ~ Y VP mly → y ) : Vp Vein V & V & + ( There are three known vector mesons : p , w ...
Page 44
... forward value . T ky Σ Απα Y12 Im M ( VV ) lo , П OT ( Y , hadron ) = Απα γν Σ ky v Yv2 για νπ πα Im M ( y → V ) lo dov | M ( y → V ) | o | 2 = ( 1 + nv2 ) ( Im M ( y → V ) |。) 2 = do where ny is the ratio of the real to the ...
... forward value . T ky Σ Απα Y12 Im M ( VV ) lo , П OT ( Y , hadron ) = Απα γν Σ ky v Yv2 για νπ πα Im M ( y → V ) lo dov | M ( y → V ) | o | 2 = ( 1 + nv2 ) ( Im M ( y → V ) |。) 2 = do where ny is the ratio of the real to the ...
Page 48
... forward production amplitude on one nucleon corresponding to the profile YvŸ . The above formulae can also be obtained from the expression d3r1 . A . . . M ( v →→ V ) = f ď3r ... ... Pra | ¥ ( x1 , ... ... r1 ) | 2 Σ M , π - V ( q ) ...
... forward production amplitude on one nucleon corresponding to the profile YvŸ . The above formulae can also be obtained from the expression d3r1 . A . . . M ( v →→ V ) = f ď3r ... ... Pra | ¥ ( x1 , ... ... r1 ) | 2 Σ M , π - V ( q ) ...
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