Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 18
... 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.
... 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 22
... hadron . Hence the above formula can be applied to a certain " effective " number of nucleons . Indeed one can show ( compare ref . [ 15 ] -the calculation was done with the Coulomb interactions present ) that to a good approximation ...
... hadron . Hence the above formula can be applied to a certain " effective " number of nucleons . Indeed one can show ( compare ref . [ 15 ] -the calculation was done with the Coulomb interactions present ) that to a good approximation ...
Page 28
... hadron physics ; all kinds of elastic hadron - hadron scattering do = ƒ ( A2 ) dA2 inelastic processes : ( experiments seem to indicate that the differential cross sections depend weakly on energy ) γρ π → 5π p → n + π on nucleons or ...
... hadron physics ; all kinds of elastic hadron - hadron scattering do = ƒ ( A2 ) dA2 inelastic processes : ( experiments seem to indicate that the differential cross sections depend weakly on energy ) γρ π → 5π p → n + π on nucleons or ...
Page 30
Wiesław Czyż. We shall extend this description to diffractive production processes of hadronic systems . We consider the incident hadron to be a superposition of some states which get eaten up at different rates during the passage ...
Wiesław Czyż. We shall extend this description to diffractive production processes of hadronic systems . We consider the incident hadron to be a superposition of some states which get eaten up at different rates during the passage ...
Page 38
... hadronic targets at high energy , a process which will be discussed later . Example 1 : The processes of QED : ( a ) Bremsstrahlung : the Feynman diagrams हु Z AND давно go over to AND where the dot means that complete 38.
... hadronic targets at high energy , a process which will be discussed later . Example 1 : The processes of QED : ( a ) Bremsstrahlung : the Feynman diagrams हु Z AND давно go over to AND where the dot means that complete 38.
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