Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 1
... forward scattering and production processes ) . Such effects are very well established in the case of hadron scattering and photon - nucleus interactions ; they are not well known in the case of neutrino reactions and very virtual ...
... forward scattering and production processes ) . Such effects are very well established in the case of hadron scattering and photon - nucleus interactions ; they are not well known in the case of neutrino reactions and very virtual ...
Page 20
... y ( b ) is very sharp compared to 1/8 ( hence we limit our- selves to forward scattering processes ) we can approximate y ( b ) ≈y ( 0 ) ¿ ( 2 ) ( b ) , hence f ( 0 ) = ik 2π y ( 0 ) , and απ αρ 2π — 2π ix . ( b ) 20.
... y ( b ) is very sharp compared to 1/8 ( hence we limit our- selves to forward scattering processes ) we can approximate y ( b ) ≈y ( 0 ) ¿ ( 2 ) ( b ) , hence f ( 0 ) = ik 2π y ( 0 ) , and απ αρ 2π — 2π ix . ( b ) 20.
Page 21
... forward forward scattering ampli- tude ) are defined by fn.p ( 0 ) = ( i + an.p ) kon , p / 4π where on.p are the total cross section for scattering on either neutron or proton . ( Incidentally , one can define an optical potential ...
... forward forward scattering ampli- tude ) are defined by fn.p ( 0 ) = ( i + an.p ) kon , p / 4π where on.p are the total cross section for scattering on either neutron or proton . ( Incidentally , one can define an optical potential ...
Page 22
... forward dip , it is not valid for small △ ) do DT ΦΩ - N Ꮓ @ [ IS . ( A ) P2 + 2 IS , ( A ) P ] , where the " effective number of nucleons " is A a = A √ db p ( b ) e¬ • Apb ) , where σ is an average total hadron - nucleon cross ...
... forward dip , it is not valid for small △ ) do DT ΦΩ - N Ꮓ @ [ IS . ( A ) P2 + 2 IS , ( A ) P ] , where the " effective number of nucleons " is A a = A √ db p ( b ) e¬ • Apb ) , where σ is an average total hadron - nucleon cross ...
Page 33
... forward direction where the transmission regeneration ( which comes from a coherent process whose coherence extends over the whole block of matter ) dominates . The amplitude ( neglecting ) is MKLK , ° = 2 ( K ° | T | Ko ) – 1⁄2 ( Řo ...
... forward direction where the transmission regeneration ( which comes from a coherent process whose coherence extends over the whole block of matter ) dominates . The amplitude ( neglecting ) is MKLK , ° = 2 ( K ° | T | Ko ) – 1⁄2 ( Řo ...
Common terms and phrases
absorption additivity of phase anomalous magnetic moment ú approximately assume attenuation beam Bureau of Standards coherent diffractive production collision Compton scattering compute Coulomb interactions Czyż d³r db bJo 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 Απ γν ΦΩ