Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 1-5 of 9
Page 7
... coupling between different spin states produced by the term K ( 81.B1 - id1 E102 ) . So , we have to deal with a coupled channels problem . We can also make the following remark : sometimes coupled channels can be decoupled by ...
... coupling between different spin states produced by the term K ( 81.B1 - id1 E102 ) . So , we have to deal with a coupled channels problem . We can also make the following remark : sometimes coupled channels can be decoupled by ...
Page 8
... . Because we have 00 CX ) -CX ) [ a ( x , y , z ) , a ( x , y , z ′ ) ] # 0 . 81 ( A1 + A2 ) Xi One could argue that the coupling to the anomalous moment is weak and hence not very relevant . This is true , but one can give some other 8.
... . Because we have 00 CX ) -CX ) [ a ( x , y , z ) , a ( x , y , z ′ ) ] # 0 . 81 ( A1 + A2 ) Xi One could argue that the coupling to the anomalous moment is weak and hence not very relevant . This is true , but one can give some other 8.
Page 10
... coupling between various spin channels . To conclude this section we may say that Examples 1 and 2 warn us that if the strong inter- actions are mediated through vector fields ( analogous to the electromagnetic field ) one can expect ...
... coupling between various spin channels . To conclude this section we may say that Examples 1 and 2 warn us that if the strong inter- actions are mediated through vector fields ( analogous to the electromagnetic field ) one can expect ...
Page 36
... coupling be weak so that it is sufficient to take only the lowest order corrections : | Yi ( k , ) ) = Z || kp , 0 , 0 ) + Σ ( knk = \ H ' \ kp ) \ 0 , k « , kn ) + ••• Ekp - Ekn - Ekя knks ( Pp | H ' | PnPx ) Epp - Epn - Epr | P » , 0 ...
... coupling be weak so that it is sufficient to take only the lowest order corrections : | Yi ( k , ) ) = Z || kp , 0 , 0 ) + Σ ( knk = \ H ' \ kp ) \ 0 , k « , kn ) + ••• Ekp - Ekn - Ekя knks ( Pp | H ' | PnPx ) Epp - Epn - Epr | P » , 0 ...
Page 53
... coupling y . ( Here a is the fine structure constant . ) ( iii ) The results of this analysis check beautifully with the results obtained from po photo- production on larger nuclei ( whose cross sections , incidentally , do depend ...
... coupling y . ( Here a is the fine structure constant . ) ( iii ) The results of this analysis check beautifully with the results obtained from po photo- production on larger nuclei ( whose cross sections , incidentally , do depend ...
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