Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 12
... experimental pro- jects under way ) . The geometry of the process is shown in figure 3 . 255 O A COMPONENTS ( b ) ( 0 ) O B COMPONENTS The profile describing the collision of two elements is : Yjk ( b − s¿ ( b ) + s , ( @ ) ) . For the ...
... experimental pro- jects under way ) . The geometry of the process is shown in figure 3 . 255 O A COMPONENTS ( b ) ( 0 ) O B COMPONENTS The profile describing the collision of two elements is : Yjk ( b − s¿ ( b ) + s , ( @ ) ) . For the ...
Page 14
... experiment . But we shall talk about comparison with experiment at other occasions . Some special cases of formula ( 3.2 ) were also employed to describe hadron - hadron scattering in the high energy limit . For example , the limit when ...
... experiment . But we shall talk about comparison with experiment at other occasions . Some special cases of formula ( 3.2 ) were also employed to describe hadron - hadron scattering in the high energy limit . For example , the limit when ...
Page 15
... experiment ) . In the form given above , the droplet model is very crude and I do not want to go beyond this qualitative description . One should perhaps mention at this point that the amplitude ( 3.4 ) contains the geometric shape of ...
... experiment ) . In the form given above , the droplet model is very crude and I do not want to go beyond this qualitative description . One should perhaps mention at this point that the amplitude ( 3.4 ) contains the geometric shape of ...
Page 18
... experiments of the future : how much cross section goes into diffractive production processes . ) ( ii ) Nondiffractive processes are presumably not contributing to the inelastic shadow- because the whole configuration of the target ...
... experiments of the future : how much cross section goes into diffractive production processes . ) ( ii ) Nondiffractive processes are presumably not contributing to the inelastic shadow- because the whole configuration of the target ...
Page 21
... - particles which interact strongly as 20 GeV nucleons . ( b / sr ) d & LAB 10 103 10 O 100 % 10 5 10 NEUTRAL NEGATIVE CHARGE POSITIVE CHARGE 15 20 PLAB , mrad For heavy nuclei there are virtually no experiments with good 21.
... - particles which interact strongly as 20 GeV nucleons . ( b / sr ) d & LAB 10 103 10 O 100 % 10 5 10 NEUTRAL NEGATIVE CHARGE POSITIVE CHARGE 15 20 PLAB , mrad For heavy nuclei there are virtually no experiments with good 21.
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