Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 14
... components of ( a ) and ( b ) . Let us consider some limiting cases of eq ( 3.2 ) ( compare ref . [ 12 ] ) . Let the radii of the two composite objects be R. and Rь . The calculations of ref . [ 12 ] show that the smaller is R , the ...
... components of ( a ) and ( b ) . Let us consider some limiting cases of eq ( 3.2 ) ( compare ref . [ 12 ] ) . Let the radii of the two composite objects be R. and Rь . The calculations of ref . [ 12 ] show that the smaller is R , the ...
Page 18
... components of σTOT ( σel , σDT , σPROD ) it follows that the measure- ments of σror may be a good way of finding out whether the inelastic shadowing ( or inelastic screening ) corrections are important at very high energies : If one ...
... components of σTOT ( σel , σDT , σPROD ) it follows that the measure- ments of σror may be a good way of finding out whether the inelastic shadowing ( or inelastic screening ) corrections are important at very high energies : If one ...
Page 23
... component of the c.m. vector r = 1 A 1⁄2 Sj , and the relative coordinates which are not independent any more : s1 = s ; -r , 8 , s ' + r A Ź s ; ' = 0 = 0 . The operator M ( A ; $ 1 ... SA ) = ik f · r : / 2π d2b exp ( i △ b ) г ( b ...
... component of the c.m. vector r = 1 A 1⁄2 Sj , and the relative coordinates which are not independent any more : s1 = s ; -r , 8 , s ' + r A Ź s ; ' = 0 = 0 . The operator M ( A ; $ 1 ... SA ) = ik f · r : / 2π d2b exp ( i △ b ) г ( b ...
Page 28
... wave polarized in the x direction and V , is the wave polarized in the y direction . z ñxez X nx = cos a tc ny = cos ( 90 - a ) ******* Nicol absorbs completely this component Suppose the target is a Nicol prism oriented in such 28.
... wave polarized in the x direction and V , is the wave polarized in the y direction . z ñxez X nx = cos a tc ny = cos ( 90 - a ) ******* Nicol absorbs completely this component Suppose the target is a Nicol prism oriented in such 28.
Page 29
... component which goes through is n ,, . But it can be decomposed into n and nXe , components . Hence due to the process of absorption , a new object is created : the wave which is polarized in the direction n Xe .. Let us compute the ...
... component which goes through is n ,, . But it can be decomposed into n and nXe , components . Hence due to the process of absorption , a new object is created : the wave which is polarized in the direction n Xe .. Let us compute the ...
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