Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 15
... elastic scattering hadron - hadron cross sections . ( ii ) predict diffractive structure ( e.g. , diffractive minima ) of the high energy hadron - hadron collisions . The very recent measurements of p - p elastic collisions confirm the ...
... elastic scattering hadron - hadron cross sections . ( ii ) predict diffractive structure ( e.g. , diffractive minima ) of the high energy hadron - hadron collisions . The very recent measurements of p - p elastic collisions confirm the ...
Page 18
... elastic scattering , the processes like the one shown in figure 7 ( with excited states of the projectile present at ... elastic scattering processes ( the cross section is ~ 10 of elastic cross section ) . ( In fact this is one of the ...
... elastic scattering , the processes like the one shown in figure 7 ( with excited states of the projectile present at ... elastic scattering processes ( the cross section is ~ 10 of elastic cross section ) . ( In fact this is one of the ...
Page 19
... scattering . 1 x ( b ) ¦ = - • + ∞ 00 dz [ V . ( b , z ) + V . ( b , z ) ... elastic cross section is invariant against the change of sign of . If ... elastic cross section for and it implies that there is no real part in the π - nucleus ...
... scattering . 1 x ( b ) ¦ = - • + ∞ 00 dz [ V . ( b , z ) + V . ( b , z ) ... elastic cross section is invariant against the change of sign of . If ... elastic cross section for and it implies that there is no real part in the π - nucleus ...
Page 22
... elastic scattering ( in which the target nucleus stays in the ground state ) . In order to have a genuine elastic scattering one would have to have an energy resolution AE a fraction of an MeV , which for E ~ 20 GeV is still ...
... elastic scattering ( in which the target nucleus stays in the ground state ) . In order to have a genuine elastic scattering one would have to have an energy resolution AE a fraction of an MeV , which for E ~ 20 GeV is still ...
Page 23
... elastic scattering amplitude is M ( A ) = ik 2π db exp ( i △ · b ) ƒ d3r | ø ( r ) l2 [ v , ( b − 1⁄2s ) + Yn ( b + 1⁄2s ) - Yр ( b − 1⁄2s ) Yn ( b + 1⁄2s ) ] . In the case of more complicated targets the situation is much more ...
... elastic scattering amplitude is M ( A ) = ik 2π db exp ( i △ · b ) ƒ d3r | ø ( r ) l2 [ v , ( b − 1⁄2s ) + Yn ( b + 1⁄2s ) - Yр ( b − 1⁄2s ) Yn ( b + 1⁄2s ) ] . In the case of more complicated targets the situation is much more ...
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