Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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... field of high energy diffractive scattering and production processes . In addition to reviewing some well - known material there is much here that is new , both in content and form of presentation . The material presented here is also ...
... field of high energy diffractive scattering and production processes . In addition to reviewing some well - known material there is much here that is new , both in content and form of presentation . The material presented here is also ...
Page 4
... field ( notation from Bjorken and Drell [ S7 ] ) : iv - eA- ке ( i - c + Fm ) = 0 , 4m where y ° A ° -y . A , i ке ... fields ( E , B ) in terms of which 1⁄2KoμF = -21⁄2K ( σ01 Ex + σ02E + 003 E2 ) where Σ = ( 023 , 31 , σ12 ) 023 ...
... field ( notation from Bjorken and Drell [ S7 ] ) : iv - eA- ке ( i - c + Fm ) = 0 , 4m where y ° A ° -y . A , i ке ... fields ( E , B ) in terms of which 1⁄2KoμF = -21⁄2K ( σ01 Ex + σ02E + 003 E2 ) where Σ = ( 023 , 31 , σ12 ) 023 ...
Page 7
... field ( at two different positions ) are , in general , noncommuting operators and there is no way of adding phase shifts ( or , equivalently , multiplying profiles ) . We can also see that the physical reason for this phenomenon is the ...
... field ( at two different positions ) are , in general , noncommuting operators and there is no way of adding phase shifts ( or , equivalently , multiplying profiles ) . We can also see that the physical reason for this phenomenon is the ...
Page 8
... field at two different points . Then 0 , \ i [ ( x − x1 ) + i ( y — yı ) ] , a = a1 + a2 = K Vi ( r- Ir - ri - ri D ) ' 0 , + K V2r - r2 ) | r - r2 | ---- \ i [ ( x − x2 ) + i ( y — Y2 ) ] , — i [ ( x − x1 ) — i ( y — iyı ) ] ) 0 — i [ ...
... field at two different points . Then 0 , \ i [ ( x − x1 ) + i ( y — yı ) ] , a = a1 + a2 = K Vi ( r- Ir - ri - ri D ) ' 0 , + K V2r - r2 ) | r - r2 | ---- \ i [ ( x − x2 ) + i ( y — Y2 ) ] , — i [ ( x − x1 ) — i ( y — iyı ) ] ) 0 — i [ ...
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... field in which the " principle of additivity of phase shifts " is also violated . Let us consider a vector particle ( hence a very relevant kind of particle to our further analysis ) . Example 2. Scattering of a charged vector meson in ...
... field in which the " principle of additivity of phase shifts " is also violated . Let us consider a vector particle ( hence a very relevant kind of particle to our further analysis ) . Example 2. Scattering of a charged vector meson in ...
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