Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 6-10 of 15
Page 30
... physical states of the system , | X ; ) ( which are analogous to the states „ and nye , of the photon ) . We want to compute ( X ; | TX ; ) . We expand | X ; ) into a set of states | A ) whose scattering and absorption in the target we ...
... physical states of the system , | X ; ) ( which are analogous to the states „ and nye , of the photon ) . We want to compute ( X ; | TX ; ) . We expand | X ; ) into a set of states | A ) whose scattering and absorption in the target we ...
Page 35
... physical proton and the physical neutron - pion pair through the " bare " states of the proton ( p ) and the neutron - pion pair ( ññ ) . π Initial state : p = + = = d1o | μ ) + d1⁄23 | ññ ) p ñ small admixture 35 π Final state : n + π ...
... physical proton and the physical neutron - pion pair through the " bare " states of the proton ( p ) and the neutron - pion pair ( ññ ) . π Initial state : p = + = = d1o | μ ) + d1⁄23 | ññ ) p ñ small admixture 35 π Final state : n + π ...
Page 42
... physical . " More precisely : as far as strong interactions go , it is physical . The situation is very similar to that in the K - K , regeneration problem : we are expanding our physical states into states which are " physical in their ...
... physical . " More precisely : as far as strong interactions go , it is physical . The situation is very similar to that in the K - K , regeneration problem : we are expanding our physical states into states which are " physical in their ...
Page 54
... physical high energy photon , of some strongly interacting components . The condition for the applicability of the high energy limit was that the characteristic length , l , defined by the incident energy and the lowest available ...
... physical high energy photon , of some strongly interacting components . The condition for the applicability of the high energy limit was that the characteristic length , l , defined by the incident energy and the lowest available ...
Page 61
... physical pion state , respectively . For instance , the following scheme ( which imitates K - K , regeneration ) ... physically more accurate to describe the initial and final states as composed , approxi- mately , of one and three ...
... physical pion state , respectively . For instance , the following scheme ( which imitates K - K , regeneration ) ... physically more accurate to describe the initial and final states as composed , approxi- mately , of one and three ...
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