Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 20
... charge amplitude : M = ik = 00 db bJ , ( Ab ) [ 1 − exp ( ix . ” ( b ) ) ] + ik [ * db bJo ( Ab ) exp [ ix . ” ( b ) + ix . ( b ) ] · Mc ( P ) + ik 5 00 0 db bJo ( Ab ) [ exp ( ixeP ( b ) ) — exp ( ixe ( b ) ) ( 1 − r ( b ) ) ] . P ...
... charge amplitude : M = ik = 00 db bJ , ( Ab ) [ 1 − exp ( ix . ” ( b ) ) ] + ik [ * db bJo ( Ab ) exp [ ix . ” ( b ) + ix . ( b ) ] · Mc ( P ) + ik 5 00 0 db bJo ( Ab ) [ exp ( ixeP ( b ) ) — exp ( ixe ( b ) ) ( 1 − r ( b ) ) ] . P ...
Page 21
... CHARGE POSITIVE CHARGE 15 20 PLAB , mrad For heavy nuclei there are virtually no experiments with good 21.
... CHARGE POSITIVE CHARGE 15 20 PLAB , mrad For heavy nuclei there are virtually no experiments with good 21.
Page 31
... charge Q = baryon no . 12NB + strangeness isospin 1/28 + T3 the partners of K + , Ko particles are K- , Ko antiparticles . Hence there are two different neutral K mesons which can be produced in the collision of strongly interacting ...
... charge Q = baryon no . 12NB + strangeness isospin 1/28 + T3 the partners of K + , Ko particles are K- , Ko antiparticles . Hence there are two different neutral K mesons which can be produced in the collision of strongly interacting ...
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