Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 2
... amplitude . The expression 1 - ex ; ( b ) = y ; ( b ) is called the profile of the jth nucleon , incident particle collision . Assuming x ( b ) = Σx ; ( b − s ; ) j = 1 and assuming that the particle goes through the target so 2.
... amplitude . The expression 1 - ex ; ( b ) = y ; ( b ) is called the profile of the jth nucleon , incident particle collision . Assuming x ( b ) = Σx ; ( b − s ; ) j = 1 and assuming that the particle goes through the target so 2.
Page 7
... profiles ) . We can also see that the physical reason for this phenomenon is the coupling between different spin states produced by the term K ( 81.B1 - iỏ1 · E1σ2 ) . So , we have to deal with a coupled channels problem . We can also ...
... profiles ) . We can also see that the physical reason for this phenomenon is the coupling between different spin states produced by the term K ( 81.B1 - iỏ1 · E1σ2 ) . So , we have to deal with a coupled channels problem . We can also ...
Page 11
... profile different from unity we get : incident wave : transmitted wave : g ( x , y ) eikz g ( x , y ) eik ( 1 - y ( x , y ) ) ( this is all under the assumption z « < L ) . Let us construct the " shape of the shadow " for a collection ...
... profile different from unity we get : incident wave : transmitted wave : g ( x , y ) eikz g ( x , y ) eik ( 1 - y ( x , y ) ) ( this is all under the assumption z « < L ) . Let us construct the " shape of the shadow " for a collection ...
Page 12
... profile of the jth nucleon : ( b ) B B á ( b ) = √ d2s® ... d23⁄4® II p® ( s1 ) - - II - ... = 1- ( 1-7 , ( b ) ) B , 1 where we assumed all profiles to be identical and introduced ỹ j i ( b − 81 ) ) ] ñ ; ( b ) = [ d ¥ rı çob ) ...
... profile of the jth nucleon : ( b ) B B á ( b ) = √ d2s® ... d23⁄4® II p® ( s1 ) - - II - ... = 1- ( 1-7 , ( b ) ) B , 1 where we assumed all profiles to be identical and introduced ỹ j i ( b − 81 ) ) ] ñ ; ( b ) = [ d ¥ rı çob ) ...
Page 15
... profile ( b ) ) . As the wave passes a scatterer it gets modified by a factor 1 - y ( b ) . Hence , the probability that the particle gets removed from the incident beam is 1- | 1 — y ( b ) | 2 = 2 Rey ( b ) ( b ) 2 ( at the impact ...
... profile ( b ) ) . As the wave passes a scatterer it gets modified by a factor 1 - y ( b ) . Hence , the probability that the particle gets removed from the incident beam is 1- | 1 — y ( b ) | 2 = 2 Rey ( b ) ( b ) 2 ( at the impact ...
Common terms and phrases
absorption additivity of phase anomalous magnetic moment ú approximately assume attenuation beam Bureau of Standards coherent diffractive production collision Compton scattering compute Coulomb interactions Czyż d³r db bJo 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 Απ γν ΦΩ