Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
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Page 25
... 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.
... 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 26
... fact the ( m | | m ' ) contributions are indeed the most important but they always lead to a sharp diffractive minimum : log doel dA 2 DEUTERON TARGET SINGLE DOUBLE 12 A But ( m | S12 m ' ) # 0 in general ( also ( m | S12 S12 | m ...
... fact the ( m | | m ' ) contributions are indeed the most important but they always lead to a sharp diffractive minimum : log doel dA 2 DEUTERON TARGET SINGLE DOUBLE 12 A But ( m | S12 m ' ) # 0 in general ( also ( m | S12 S12 | m ...
Page 27
... fact is that in exactly the same form one can write the Delbrück amplitude Delbrück M ( A ) ~ ƒ d2b exp ( i △ · b ) I1 ( A , s ) { 1— exp [ ix. ̄ ( b − 1⁄28 ) + ix . + ( b + 1⁄2s ) ] } where x . are the Coulomb phase shifts of the ...
... fact is that in exactly the same form one can write the Delbrück amplitude Delbrück M ( A ) ~ ƒ d2b exp ( i △ · b ) I1 ( A , s ) { 1— exp [ ix. ̄ ( b − 1⁄28 ) + ix . + ( b + 1⁄2s ) ] } where x . are the Coulomb phase shifts of the ...
Page 31
... fact , one usually determines them experimentally ( see the end of this section ) . So far as the e¡ ; are concerned , they are small - hence some perturbation theory can be used to compute them . We shall give some examples further in ...
... fact , one usually determines them experimentally ( see the end of this section ) . So far as the e¡ ; are concerned , they are small - hence some perturbation theory can be used to compute them . We shall give some examples further in ...
Page 35
... fact the same argument shows that the incident state and the produced state can also be considered degenerate in the limit p → ( the fact that p will also change slightly during the collision does not change this conclusion ) . Note ...
... fact the same argument shows that the incident state and the produced state can also be considered degenerate in the limit p → ( the fact that p will also change slightly during the collision does not change this conclusion ) . Note ...
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