Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 11
... eik z = II [ 1 — y ; ( b − s ; ) ] ę ik z j = 1 A r ( b , s1 . . . SA ) = 1 — [ 1 - y ; ( b - s , ) ] . j = 1 So , we get again the formulae of section 2 . The previous case dealt with an elementary object scattering from 11 =
... eik z = II [ 1 — y ; ( b − s ; ) ] ę ik z j = 1 A r ( b , s1 . . . SA ) = 1 — [ 1 - y ; ( b - s , ) ] . j = 1 So , we get again the formulae of section 2 . The previous case dealt with an elementary object scattering from 11 =
Page 12
Wiesław Czyż. The previous case dealt with an elementary object scattering from a composite object . We already saw in the ... objects . The formulae given below are interesting also because they may be used to analyze high energy nucleus ...
Wiesław Czyż. The previous case dealt with an elementary object scattering from a composite object . We already saw in the ... objects . The formulae given below are interesting also because they may be used to analyze high energy nucleus ...
Page 14
... objects be R. and Rь . The calculations of ref . [ 12 ] show that the smaller is R , the nearer we are to the additivity of ( b ) -nucleon phase shifts . But that means that this additivity improves with increase of the binding of ( b ) ...
... objects be R. and Rь . The calculations of ref . [ 12 ] show that the smaller is R , the nearer we are to the additivity of ( b ) -nucleon phase shifts . But that means that this additivity improves with increase of the binding of ( b ) ...
Page 15
... objects ( e.g. , their transverse density distributions ) . If these geometric characteristics do not depend on energy , one gets the total cross section ( from the optical theorem ) which is energy independent . So , it seems to be ...
... objects ( e.g. , their transverse density distributions ) . If these geometric characteristics do not depend on energy , one gets the total cross section ( from the optical theorem ) which is energy independent . So , it seems to be ...
Page 28
... objects . The model of diffractive processes described below is based on : M. L. Good and W. D. Walker ( 1960 ) [ 23 ] . The article which discusses some very early papers on the subject is : E. L. Feinberg and I. Pomerančuk ( 1956 ) ...
... objects . The model of diffractive processes described below is based on : M. L. Good and W. D. Walker ( 1960 ) [ 23 ] . The article which discusses some very early papers on the subject is : E. L. Feinberg and I. Pomerančuk ( 1956 ) ...
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