Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 16
... profile is ( r ) = ( or ( b ; Si ... SA ) | Yo ) , and we can write the same relations as before : σTOT = d2b | ( T ) | 2 + √ dob [ 2 Re ( г ) — | ( r ) | 2 ] because , due to the same arguments as before , 1-1- ( r ) 2 gives the ...
... profile is ( r ) = ( or ( b ; Si ... SA ) | Yo ) , and we can write the same relations as before : σTOT = d2b | ( T ) | 2 + √ dob [ 2 Re ( г ) — | ( r ) | 2 ] because , due to the same arguments as before , 1-1- ( r ) 2 gives the ...
Page 17
... 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 construct the profiles of the ...
... 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 construct the profiles of the ...
Page 18
Wiesław Czyż. But as long as we construct the profiles of the target nucleus from profiles of elastic scattering , the processes like the one shown in figure 7 ( with excited states of the projectile present at intermediate steps ) are ...
Wiesław Czyż. But as long as we construct the profiles of the target nucleus from profiles of elastic scattering , the processes like the one shown in figure 7 ( with excited states of the projectile present at intermediate steps ) are ...
Page 20
... profiles and densities ) we have ( N number of neutrons , Z - number of protons ) : - ixs ( b ) ≈ — Nyn ( 0 ) În ( b ) — ZYp ( 0 ) Pp ( b ) . Pn When yn ( b ) and y , ( b ) are very sharp compared with pn ( s ) and pp ( s ) we have ix ...
... profiles and densities ) we have ( N number of neutrons , Z - number of protons ) : - ixs ( b ) ≈ — Nyn ( 0 ) În ( b ) — ZYp ( 0 ) Pp ( b ) . Pn When yn ( b ) and y , ( b ) are very sharp compared with pn ( s ) and pp ( s ) we have ix ...
Page 26
... profiles " than ( m | M | m ) , thus resulting in oscillations which are out of phase with oscillations of ( m | M | m ) and fill the diffractive minimum : log doel m = m ' CONTRIBUTION doel log THE SUM E - t m # m ' CONTRIB . ব ...
... profiles " than ( m | M | m ) , thus resulting in oscillations which are out of phase with oscillations of ( m | M | m ) and fill the diffractive minimum : log doel m = m ' CONTRIBUTION doel log THE SUM E - t m # m ' CONTRIB . ব ...
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