Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 2
... parameter x ; ( b ) is the phase shift which characterizes the incident particle - jth nucleon elastic scat- tering amplitude . The expression 1 - eix ; ( b ) = y ; ( b ) is called the profile of the jth nucleon , incident particle ...
... parameter x ; ( b ) is the phase shift which characterizes the incident particle - jth nucleon elastic scat- tering amplitude . The expression 1 - eix ; ( b ) = y ; ( b ) is called the profile of the jth nucleon , incident particle ...
Page 14
... ( a ) ( s ( a ) ) y ( b − s ( b ) + s ( a ) ) p ( b ) ( s ( b ) ) = k where K is a free parameter . 1 = ( 2x ) 2 √ dq exp ( −iq • b ) F ( a ) ( 9 ) Fo ( 9 ) , If we accept that the densities of hadronic matter are 14.
... ( a ) ( s ( a ) ) y ( b − s ( b ) + s ( a ) ) p ( b ) ( s ( b ) ) = k where K is a free parameter . 1 = ( 2x ) 2 √ dq exp ( −iq • b ) F ( a ) ( 9 ) Fo ( 9 ) , If we accept that the densities of hadronic matter are 14.
Page 15
... that the particle gets removed from the incident beam is 1— | 1 — y ( b ) | 2 = 2 Rey ( b ) ( b ) 2 ( at the impact parameter b ) . Notice that here we use the same expression as in the following paragraphs : we identify 1–7 with y 15.
... that the particle gets removed from the incident beam is 1— | 1 — y ( b ) | 2 = 2 Rey ( b ) ( b ) 2 ( at the impact parameter b ) . Notice that here we use the same expression as in the following paragraphs : we identify 1–7 with y 15.
Page 16
... 1-1- ( 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.
... 1-1- ( 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
... parameter b≈ ( l + 1⁄2 ) / k with all nucleons frozen at the positions $ 1 , SA . .. • So , in our model there are three different contributions . OEL ONLY NUCLEONS APPEAR бот NEW PARTICLES ARE PRODUCED OPROD But as long as we ...
... parameter b≈ ( l + 1⁄2 ) / k with all nucleons frozen at the positions $ 1 , SA . .. • So , in our model there are three different contributions . OEL ONLY NUCLEONS APPEAR бот NEW PARTICLES ARE PRODUCED OPROD But as long as we ...
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