Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Results 6-9 of 9
Page 10
... equation M = g ( e / 2m ) S ) the projection of the polarization on the direction of motion is constant , and hence there is no coupling between various spin channels . To conclude this section we may say that Examples 1 and 2 warn us ...
... equation M = g ( e / 2m ) S ) the projection of the polarization on the direction of motion is constant , and hence there is no coupling between various spin channels . To conclude this section we may say that Examples 1 and 2 warn us ...
Page 14
... Equation ( 3.4 ) gives the well - known " droplet model " [ 13 ] elastic scattering amplitude of two composite objects whose hadronic matter distributions are given by pa ) ( s ( a ) ) and p ( b ) ( s ( b ) ) . If one assumes that y ( b ) ...
... Equation ( 3.4 ) gives the well - known " droplet model " [ 13 ] elastic scattering amplitude of two composite objects whose hadronic matter distributions are given by pa ) ( s ( a ) ) and p ( b ) ( s ( b ) ) . If one assumes that y ( b ) ...
Page 44
... equation was used in the analysis published recently by D. O. Caldwell et al . [ 37 ] . Another possible test is , e.g. , the equation σT ( Y , hadron ) = π k , Σ V Απα Y12 Im M ( V → V ) . Assuming M ( V → V ) purely imaginary ( in ...
... equation was used in the analysis published recently by D. O. Caldwell et al . [ 37 ] . Another possible test is , e.g. , the equation σT ( Y , hadron ) = π k , Σ V Απα Y12 Im M ( V → V ) . Assuming M ( V → V ) purely imaginary ( in ...
Page 57
... equation is valid for nucleon targets . Hence we can eliminate d and get M ( 1-2 ) : = f21 [ ( 2 Î ) ( 2 | T ‹ N ) | 2 ) − ( 1 | T ‹ ~ ) | Ĭ ) [ ‹ 2 | T ‹ 4 ) | 2 ) — ( 1 | T ‹ 4 ) | Ï ) ] , which gives the production amplitude on the ...
... equation is valid for nucleon targets . Hence we can eliminate d and get M ( 1-2 ) : = f21 [ ( 2 Î ) ( 2 | T ‹ N ) | 2 ) − ( 1 | T ‹ ~ ) | Ĭ ) [ ‹ 2 | T ‹ 4 ) | 2 ) — ( 1 | T ‹ 4 ) | Ï ) ] , which gives the production amplitude on the ...
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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