Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 13
... contribution of the second order because [ d3r , ®po® • ( r , ® ) ¥ u ( b − s , ® + 81® ) ) 2ı ( b − 8 , +82 ) ) % ( rz ) = = ( b ) [ dar , ®d3r , ®'ço © ® * ( ri ) vu ( b − 8 ; ® + si® ) Σ ¢ „ ® ( r¿® ) ¢ „ 6 ) * ( rzb ) ' ) XY21 ...
... contribution of the second order because [ d3r , ®po® • ( r , ® ) ¥ u ( b − s , ® + 81® ) ) 2ı ( b − 8 , +82 ) ) % ( rz ) = = ( b ) [ dar , ®d3r , ®'ço © ® * ( ri ) vu ( b − 8 ; ® + si® ) Σ ¢ „ ® ( r¿® ) ¢ „ 6 ) * ( rzb ) ' ) XY21 ...
Page 14
... contributions and becomes ( 3.4 ) . Equation ( 3.4 ) 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 ...
... contributions and becomes ( 3.4 ) . Equation ( 3.4 ) 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 ...
Page 16
... 1- ( r ) 2 gives the probability ( at the impact parameter b ) of losing the incident particle from the elastic channel . It is convenient however to split the second term into two physically different contributions : 16.
... 1- ( r ) 2 gives the probability ( at the impact parameter b ) of losing the incident particle from the elastic channel . It is convenient however to split the second term into two physically different contributions : 16.
Page 17
Wiesław Czyż. split the second term into two physically different contributions : [ ď2b [ 2 Re ( r ) − | ( r ) | 2 ] = [ ď3b [ ( r + r ) — | ( r ) | 2 ] = σDT + [ db [ 2 Re ( r ) — ( r + r ) ] = σ PROD Interpretation The first contribution ...
Wiesław Czyż. split the second term into two physically different contributions : [ ď2b [ 2 Re ( r ) − | ( r ) | 2 ] = [ ď3b [ ( r + r ) — | ( r ) | 2 ] = σDT + [ db [ 2 Re ( r ) — ( r + r ) ] = σ PROD Interpretation The first contribution ...
Page 18
... contributions to aror discussed above do approximately exhaust the list of processes contributing to elastic scattering . From our discussion of the components of σTOT ( σel , σDT , σPROD ) it follows that the measure- ments of σror may ...
... contributions to aror discussed above do approximately exhaust the list of processes contributing to elastic scattering . From our discussion of the components of σTOT ( σel , σDT , σPROD ) it follows that the measure- ments of σror may ...
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