Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 9
Wiesław Czyż. This is true , but one can give some other - though much more complex - examples of scattering from a ... gives the same relation between magnetic moment and spin when x = 1 ! So , in both Examples , when к and ĩ are ...
Wiesław Czyż. This is true , but one can give some other - though much more complex - examples of scattering from a ... gives the same relation between magnetic moment and spin when x = 1 ! So , in both Examples , when к and ĩ are ...
Page 11
... gives , as r → ∞ , ( compare D. R. Yennie article in [ S3 ] ) ¥ ( r ) = eik2 + [ ƒ ( ke1 ) / r ] exp ( ikr ) , ( e = component of re2 ) , with f ( ke ) correctly given by the inverse of y ( b ) . One can see this by shifting the ...
... gives , as r → ∞ , ( compare D. R. Yennie article in [ S3 ] ) ¥ ( r ) = eik2 + [ ƒ ( ke1 ) / r ] exp ( ikr ) , ( e = component of re2 ) , with f ( ke ) correctly given by the inverse of y ( b ) . One can see this by shifting the ...
Page 12
... ; t ( b − 8 , ® ) which is the profile for elastic scattering of ( b ) from the jth nucleon of ( a ) and a two - dimensional density p ( s ) = ƒ ** dz 4o * ( r ) ço ( r ) . 81 Then the additivity of phase shifts gives us the formula 121.
... ; t ( b − 8 , ® ) which is the profile for elastic scattering of ( b ) from the jth nucleon of ( a ) and a two - dimensional density p ( s ) = ƒ ** dz 4o * ( r ) ço ( r ) . 81 Then the additivity of phase shifts gives us the formula 121.
Page 13
... gives : ALL POSSIBLE EXCITED STATES Suppose we reject the intermediate excited states and take only the ground state as a possible inter- mediate state ( this is the way to eliminate all channels but one ) . Then each y ; can be ...
... gives : ALL POSSIBLE EXCITED STATES Suppose we reject the intermediate excited states and take only the ground state as a possible inter- mediate state ( this is the way to eliminate all channels but one ) . Then each y ; can be ...
Page 14
... 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 ) is a very ...
... 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 ) is a very ...
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