Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 23
... nucleons in the nucleus are unimportant for dose / dî or do 。 dî . They are of some importance for do Dr / dî ( especially at small momentum transfers [ 15 ] , [ 3 ] ) . The confrontation with experiment is impressive . ( Compare ...
... nucleons in the nucleus are unimportant for dose / dî or do 。 dî . They are of some importance for do Dr / dî ( especially at small momentum transfers [ 15 ] , [ 3 ] ) . The confrontation with experiment is impressive . ( Compare ...
Page 24
... nucleons . When one cannot factorize the c.m. coordinate and one has to use the above formula the numerical calculations become much more involved ( from trivial - they become difficult [ 18 ] ) . An illustrative example : the ground ...
... nucleons . When one cannot factorize the c.m. coordinate and one has to use the above formula the numerical calculations become much more involved ( from trivial - they become difficult [ 18 ] ) . An illustrative example : the ground ...
Page 25
... Remark : In fact , this clear distinction between single and double scattering was used to extract the p - nucleon total cross section in y - p production experiments on deuterons ( see section 4.2 ) . ( ii ) One can also see ( again , 25.
... Remark : In fact , this clear distinction between single and double scattering was used to extract the p - nucleon total cross section in y - p production experiments on deuterons ( see section 4.2 ) . ( ii ) One can also see ( again , 25.
Page 28
... nucleons or nuclei . K - Kπ , KππT etc. The nucleon and nuclear targets supplement each other because the nuclear medium amplifies the scattering of the produced objects . The model of diffractive processes described below is based on ...
... nucleons or nuclei . K - Kπ , KππT etc. The nucleon and nuclear targets supplement each other because the nuclear medium amplifies the scattering of the produced objects . The model of diffractive processes described below is based on ...
Page 33
... nucleon scattering amplitudes assuming isospin symmetry : ƒK ° n ( 0 ) = ƒk * p ( 0 ) , ƒÃon ( 0 ) = ƒÂ ̄p ( 0 ) , ƒK ° p ( 0 ) = ƒk * n ( 0 ) , fKp ( 0 ) = ƒK ̄n ( 0 ) . The standard way of calculating these amplitudes is : ( i ) the ...
... nucleon scattering amplitudes assuming isospin symmetry : ƒK ° n ( 0 ) = ƒk * p ( 0 ) , ƒÃon ( 0 ) = ƒÂ ̄p ( 0 ) , ƒK ° p ( 0 ) = ƒk * n ( 0 ) , fKp ( 0 ) = ƒK ̄n ( 0 ) . The standard way of calculating these amplitudes is : ( i ) the ...
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