Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 9
... charged vector meson in a static field ( we shall quote the results , for more details see refs . [ 9 , 10 ] ) . Let us ... charge and m the mass of the particle . Note that eq ( 2.6 ) gives the same relation between magnetic moment and ...
... charged vector meson in a static field ( we shall quote the results , for more details see refs . [ 9 , 10 ] ) . Let us ... charge and m the mass of the particle . Note that eq ( 2.6 ) gives the same relation between magnetic moment and ...
Page 10
... charged particle with spin S and magnetic moment M given by ( 2.7 ) moving in an almost uniform magnetic field B. This particle follows a circular trajectory with frequency - 13 B. m Its magnetic moment ( hence its spin ) precesses with ...
... charged particle with spin S and magnetic moment M given by ( 2.7 ) moving in an almost uniform magnetic field B. This particle follows a circular trajectory with frequency - 13 B. m Its magnetic moment ( hence its spin ) precesses with ...
Page 15
... charge densities , F ( a ) , F ( b ) are the charge form factors of the colliding hadrons . This formula was used successfully to : ( i ) reproduce the proton charge form factors from elastic scattering hadron - hadron cross sections ...
... charge densities , F ( a ) , F ( b ) are the charge form factors of the colliding hadrons . This formula was used successfully to : ( i ) reproduce the proton charge form factors from elastic scattering hadron - hadron cross sections ...
Page 18
... elastic scattering from nuclei of charged hadrons , and ( ii ) the corrections for the c.m. motion which are important for light nuclei but unimportant for heavy ones . Let us consider first the Coulomb corrections for heavy nuclei 18.
... elastic scattering from nuclei of charged hadrons , and ( ii ) the corrections for the c.m. motion which are important for light nuclei but unimportant for heavy ones . Let us consider first the Coulomb corrections for heavy nuclei 18.
Page 19
... charge of the incident beam of particles . For isospin zero targets ( He , 160 ) , if one finds no difference between the elastic cross section for and it implies that there is no real part in the π - nucleus elastic scattering strong ...
... charge of the incident beam of particles . For isospin zero targets ( He , 160 ) , if one finds no difference between the elastic cross section for and it implies that there is no real part in the π - nucleus elastic scattering strong ...
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