Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 46
Wiesław Czyż. Conclusion : The VMD model is only approximately correct . There is no commonly accepted explanation of the discrepancies described above . Perhaps the Compton - like contributions to M ( → ) ( as suggested by Brodsky ...
Wiesław Czyż. Conclusion : The VMD model is only approximately correct . There is no commonly accepted explanation of the discrepancies described above . Perhaps the Compton - like contributions to M ( → ) ( as suggested by Brodsky ...
Page 52
... approximately by ( see also fig . 45 ) d2ôF ( 8 ) ƒ „ » ' » ( 1⁄2A + 8 ) ƒ » y TM ( 1⁄2 △ −8 ) + [ d2ôF ( 8 ) ƒ „ ‚ ‹ TM ( 1⁄2 △ −8 ) ƒ » x » ( 1⁄2A + 8 ) . Q PP So , by measuring the cross section at large momentum transfers we can ...
... approximately by ( see also fig . 45 ) d2ôF ( 8 ) ƒ „ » ' » ( 1⁄2A + 8 ) ƒ » y TM ( 1⁄2 △ −8 ) + [ d2ôF ( 8 ) ƒ „ ‚ ‹ TM ( 1⁄2 △ −8 ) ƒ » x » ( 1⁄2A + 8 ) . Q PP So , by measuring the cross section at large momentum transfers we can ...
Page 55
... approximately energy independent . Hence one should expect an increase of the do21 / dA2 cross section ( obtained from the 3 ( 1-2 ) amplitude given above ) as the incident energy increases and e → 1 . ( Note the difference with vector ...
... approximately energy independent . Hence one should expect an increase of the do21 / dA2 cross section ( obtained from the 3 ( 1-2 ) amplitude given above ) as the incident energy increases and e → 1 . ( Note the difference with vector ...
Page 62
... approximately equal to σ , ( they cannot be exactly equal to σ , because we would have no production ! ) . When we do that , we have approximately ( due to ( 5.9 ) ) the elastic amplitude of the form ( 5.8 ) , and the production ...
... approximately equal to σ , ( they cannot be exactly equal to σ , because we would have no production ! ) . When we do that , we have approximately ( due to ( 5.9 ) ) the elastic amplitude of the form ( 5.8 ) , and the production ...
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