Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 29
... object is created : the wave which is polarized in the direction n Xe .. Let us compute the elastic and inelastic scattering amplitudes . Since the transmitted wave is = n , the wave which goes into scattering and production is ¥ n ...
... object is created : the wave which is polarized in the direction n Xe .. Let us compute the elastic and inelastic scattering amplitudes . Since the transmitted wave is = n , the wave which goes into scattering and production is ¥ n ...
Page 31
... objects ; e.g. , when 3 are produced in the → 3 reaction : are then its n's given by the absorption of 37 in the target ? In fact , one usually determines them experimentally ( see the end of this section ) . So far as the e¡ ; are ...
... objects ; e.g. , when 3 are produced in the → 3 reaction : are then its n's given by the absorption of 37 in the target ? In fact , one usually determines them experimentally ( see the end of this section ) . So far as the e¡ ; are ...
Page 57
... objects 1 and 2 from the target nucleus 2π d2b exp ( i △ b ) { 1- exp [ -202'T ( b ) ] } , ik ( 2 | T ( 4 ) | 2 ) : = ( Ï | T ‹ 4 ) | Ï ) = ik 2π d2b exp ( i △ b ) { 1- exp [ -201'T ( b ) ] } , where T ( b ) = A dz p ( b , z ) , o ...
... objects 1 and 2 from the target nucleus 2π d2b exp ( i △ b ) { 1- exp [ -202'T ( b ) ] } , ik ( 2 | T ( 4 ) | 2 ) : = ( Ï | T ‹ 4 ) | Ï ) = ik 2π d2b exp ( i △ b ) { 1- exp [ -201'T ( b ) ] } , where T ( b ) = A dz p ( b , z ) , o ...
Page 60
... objects which undergo diffractive scattering . Remark : Let us note that we may write the amplitude ( 5.4 ) so that it has the KK , regeneration amplitude on a single nucleon as a factor similarly to that appearing in the " one step ...
... objects which undergo diffractive scattering . Remark : Let us note that we may write the amplitude ( 5.4 ) so that it has the KK , regeneration amplitude on a single nucleon as a factor similarly to that appearing in the " one step ...
Page 61
... objects produced are the same in this limit as at the experimentally available energies . ) Let us accept that and and ( and positive ) , | ☛ ) = -— / 2 ( 1 ) + | 2 ) ) = | 1 ) 1 | 3π ) = — ( | 1 ) — | 2 ) ) = | 2 ) . ( 5.6 ) ( Note ...
... objects produced are the same in this limit as at the experimentally available energies . ) Let us accept that and and ( and positive ) , | ☛ ) = -— / 2 ( 1 ) + | 2 ) ) = | 1 ) 1 | 3π ) = — ( | 1 ) — | 2 ) ) = | 2 ) . ( 5.6 ) ( Note ...
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