Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 19
... scattering . 1 x ( b ) ¦ = - • + ∞ 00 dz [ V . ( b , z ) + V . ( b , z ) ... amplitude ( 3.6 ) has some simple properties which show that the Coulomb ... elastic cross section is invariant against the change of sign of . If , however , x.0 ...
... scattering . 1 x ( b ) ¦ = - • + ∞ 00 dz [ V . ( b , z ) + V . ( b , z ) ... amplitude ( 3.6 ) has some simple properties which show that the Coulomb ... elastic cross section is invariant against the change of sign of . If , however , x.0 ...
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 ...
Page 24
... amplitudes are taken in the form | ¥。| 2 = ÎÌ p ( r ' ; ) , f ( k ) = = j = 1 ( i + a ) ko 4π p ( r ) = po exp ( -r / R2 ) exp ( −11⁄2ad2 ) . Then the elastic scattering amplitude ( with the c.m. motion correction included ) reads M ...
... amplitudes are taken in the form | ¥。| 2 = ÎÌ p ( r ' ; ) , f ( k ) = = j = 1 ( i + a ) ko 4π p ( r ) = po exp ( -r / R2 ) exp ( −11⁄2ad2 ) . Then the elastic scattering amplitude ( with the c.m. motion correction included ) reads M ...
Page 27
... scattering , where the above model does not apply ( see also [ 48 ] ... elastic processes ) . For large momentum transfers ( A2 / M2 ~ 1 ) this is ... amplitude is M ( ( A ) = 1 √ α ik d2b d2s eia · bI ( △ , s ) { 1— exp [ ix , ( b − 1 ...
... scattering , where the above model does not apply ( see also [ 48 ] ... elastic processes ) . For large momentum transfers ( A2 / M2 ~ 1 ) this is ... amplitude is M ( ( A ) = 1 √ α ik d2b d2s eia · bI ( △ , s ) { 1— exp [ ix , ( b − 1 ...
Page 30
... scattering and absorption in the target we assume known : | { ; ) = Σdij | λ ... amplitude is proportional to the difference in absorptions of the i , j ... elastic scattering . Compare the end of this section . we accept that diffractive ...
... scattering and absorption in the target we assume known : | { ; ) = Σdij | λ ... amplitude is proportional to the difference in absorptions of the i , j ... elastic scattering . Compare the end of this section . we accept that diffractive ...
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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