Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Page 42
... nuclear radius ) we shall have shadowing fully developed . We can see , therefore , that full shadowing occurs at high enough energies . At low photon energies | E - E , | is large and the corresponding fluctuation cannot interact with ...
... nuclear radius ) we shall have shadowing fully developed . We can see , therefore , that full shadowing occurs at high enough energies . At low photon energies | E - E , | is large and the corresponding fluctuation cannot interact with ...
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 47
... nuclear volume . We construct the production amplitude as the ( previously introduced ) picture of multiple scattering tells us to . For the independent particle ground state wave function we have ik v M ( y → V ) = = 2π A db exp ( i ...
... nuclear volume . We construct the production amplitude as the ( previously introduced ) picture of multiple scattering tells us to . For the independent particle ground state wave function we have ik v M ( y → V ) = = 2π A db exp ( i ...
Page 53
... nuclear excitations should be removed ( ii ) processes which lead to π production ( other than p - production ) should be subtracted , ( iii ) one has to decide which invariant masses of are p ° ' s and which belong to some kind of ...
... nuclear excitations should be removed ( ii ) processes which lead to π production ( other than p - production ) should be subtracted , ( iii ) one has to decide which invariant masses of are p ° ' s and which belong to some kind of ...
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