Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 6-10 of 16
Page 25
... multiple scattering theories ( or models ) . ( i ) In experiments ( compare deuteron data contained in [ S1 ] ) , one can clearly see the single and double scattering . do log dA Deuteron Target Single Double Δ 2 Remark : In fact , this ...
... multiple scattering theories ( or models ) . ( i ) In experiments ( compare deuteron data contained in [ S1 ] ) , one can clearly see the single and double scattering . do log dA Deuteron Target Single Double Δ 2 Remark : In fact , this ...
Page 43
... scattering contribution of the multiple scattering of vector mesons and is properly taken care of by the VMD model description of photon - nucleus interactions . If , however , the VMD model fails to reproduce the total photon - nucleon ...
... scattering contribution of the multiple scattering of vector mesons and is properly taken care of by the VMD model description of photon - nucleus interactions . If , however , the VMD model fails to reproduce the total photon - nucleon ...
Page 47
... multiple scattering tells us to . For the independent particle ground state wave function we have ik v M ( y → V ) = = 2π A db exp ( i △ · b ) f ď3rı ...... . ď3ra d3r1 ... d3r II p ( r ; ) j - 1 × ΣII [ 1 - yv ( b − s ; ) 0 ( 2 ; —2 ...
... multiple scattering tells us to . For the independent particle ground state wave function we have ik v M ( y → V ) = = 2π A db exp ( i △ · b ) f ď3rı ...... . ď3ra d3r1 ... d3r II p ( r ; ) j - 1 × ΣII [ 1 - yv ( b − s ; ) 0 ( 2 ; —2 ...
Page 49
... scattering of photons from a nucleus derived from the multiple scattering model , with A non- negligible , in the limit of large A and VMD assumed : ik M ( YY ) ( ~~~~ ) == 12 = √ ---- [ db exp ( i △ · b ) { A ƒ dr p ( r ) Y , ( b− s ) ...
... scattering of photons from a nucleus derived from the multiple scattering model , with A non- negligible , in the limit of large A and VMD assumed : ik M ( YY ) ( ~~~~ ) == 12 = √ ---- [ db exp ( i △ · b ) { A ƒ dr p ( r ) Y , ( b− s ) ...
Page 50
... scattering contribution always goes as A ( just as any multiple scattering process ) but it becomes progressively less important as A0 with increasing energy . Recall that the experi- ments discussed above [ 37 ] had shown that when or ...
... scattering contribution always goes as A ( just as any multiple scattering process ) but it becomes progressively less important as A0 with increasing energy . Recall that the experi- ments discussed above [ 37 ] had shown that when or ...
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