Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 1
... nuclear targets by high energy projectiles are discussed in this article . Special attention is paid to the interaction of high energy hadrons and photons . Interactions of high energy electrons and neutrinos are briefly men- tioned ...
... nuclear targets by high energy projectiles are discussed in this article . Special attention is paid to the interaction of high energy hadrons and photons . Interactions of high energy electrons and neutrinos are briefly men- tioned ...
Page 28
... nuclear targets supplement each other because the nuclear medium amplifies the scattering of the produced objects . The model of diffractive processes described below is based on : M. L. Good and W. D. Walker ( 1960 ) [ 23 ] . The ...
... nuclear targets supplement each other because the nuclear medium amplifies the scattering of the produced objects . The model of diffractive processes described below is based on : M. L. Good and W. D. Walker ( 1960 ) [ 23 ] . The ...
Page 45
... nuclear targets ( nuclear targets : Pb , Cu , C ) [ 37 ] . ω Nucleon targets : The authors assumed the w and contributions to or ( y , nucleon ) to be 20 ± 2 μb ( remember : this is just a small contribution ) . Then , by measuring σr ...
... nuclear targets ( nuclear targets : Pb , Cu , C ) [ 37 ] . ω Nucleon targets : The authors assumed the w and contributions to or ( y , nucleon ) to be 20 ± 2 μb ( remember : this is just a small contribution ) . Then , by measuring σr ...
Page 46
... nuclear targets and , since it is comparatively well docu- mented experimentally , it is instructive to outline it here . The production amplitude of a vector boson is ( in the limit w →→ ∞ ) Υπα M ( Y → V ) = ( 0 , kv | tv | 0 , kv ...
... nuclear targets and , since it is comparatively well docu- mented experimentally , it is instructive to outline it here . The production amplitude of a vector boson is ( in the limit w →→ ∞ ) Υπα M ( Y → V ) = ( 0 , kv | tv | 0 , kv ...
Page 53
... targets were used : H2 , Be , C , Al , Ti , Cu , Ag , Cd , In , Ta , W , Au , Pb , U. The parameters obtained from ... nuclear excitations should be removed ( ii ) processes which lead to π production ( other than p - production ) should ...
... targets were used : H2 , Be , C , Al , Ti , Cu , Ag , Cd , In , Ta , W , Au , Pb , U. The parameters obtained from ... nuclear excitations should be removed ( ii ) processes which lead to π production ( other than p - production ) should ...
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