Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 6-10 of 10
Page 25
... correction can be seen from the factor exp ( R242 / 4A ) . For small A ( say A = 2 , 3 or 4 ) it can be a correction of as much as 2 orders of magnitude for A2 0.3 GeV2 . A few concluding remarks about the deuteron target . A lot of ...
... correction can be seen from the factor exp ( R242 / 4A ) . For small A ( say A = 2 , 3 or 4 ) it can be a correction of as much as 2 orders of magnitude for A2 0.3 GeV2 . A few concluding remarks about the deuteron target . A lot of ...
Page 35
... corrections at low energies . But in the limit of very high energies and small momentum transfer , all such effects dis- appear . Let us take , e.g. , two such states and give them the same momentum p . Then their energies differ : E ...
... corrections at low energies . But in the limit of very high energies and small momentum transfer , all such effects dis- appear . Let us take , e.g. , two such states and give them the same momentum p . Then their energies differ : E ...
Page 36
... 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 ) + • • ( 4.6 ) | ¥ s ( Pn , Pr ) ) = Z | | 0 , Pn , Px ) – Σ where ...
... 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 ) + • • ( 4.6 ) | ¥ s ( Pn , Pr ) ) = Z | | 0 , Pn , Px ) – Σ where ...
Page 53
... corrections in order to obtain the coherent p - production cross sections : ( i ) nuclear excitations should be removed ( ii ) processes which lead to π production ( other than p - production ) should be subtracted , ( iii ) one has to ...
... corrections in order to obtain the coherent p - production cross sections : ( i ) nuclear excitations should be removed ( ii ) processes which lead to π production ( other than p - production ) should be subtracted , ( iii ) one has to ...
Page 54
... corrected for a non - negligible longitudinal momentum transfer for the case of vector meson production ( the formula for elastic photon scattering was also given with- out derivation ) . 3. The Vector Meson Dominance model was briefly ...
... corrected for a non - negligible longitudinal momentum transfer for the case of vector meson production ( the formula for elastic photon scattering was also given with- out derivation ) . 3. The Vector Meson Dominance model was briefly ...
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