Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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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 18
... weak ( at least at energies of a few GeV ) compared to elastic scattering processes ( the cross section is ~ 10 of elastic cross section ) . ( In fact this is one of the very important questions to be answered by the very high energy ...
... weak ( at least at energies of a few GeV ) compared to elastic scattering processes ( the cross section is ~ 10 of elastic cross section ) . ( In fact this is one of the very important questions to be answered by the very high energy ...
Page 30
... the same order of magnitude one does predict some characteristics of production processes from the knowledge of elastic scattering . Compare the end of this section . we accept that diffractive production processes are weak compared to 30.
... the same order of magnitude one does predict some characteristics of production processes from the knowledge of elastic scattering . Compare the end of this section . we accept that diffractive production processes are weak compared to 30.
Page 31
Wiesław Czyż. we accept that diffractive production processes are weak compared to elastic scattering . This may mean that the transformation from | X ; ) to | A ; ) differs little from unity : Cij = dij + Eij tij small , hence e2 terms ...
Wiesław Czyż. we accept that diffractive production processes are weak compared to elastic scattering . This may mean that the transformation from | X ; ) to | A ; ) differs little from unity : Cij = dij + Eij tij small , hence e2 terms ...
Page 36
... 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 , 0 ) + ...
... 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 , 0 ) + ...
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