Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 14
... deuteron - deuteron scattering data are available , but reliable calculations are very difficult because of the high spins involved . Nevertheless , there exist some calculations [ S1 ] and there seems to be reasonable agreement between ...
... deuteron - deuteron scattering data are available , but reliable calculations are very difficult because of the high spins involved . Nevertheless , there exist some calculations [ S1 ] and there seems to be reasonable agreement between ...
Page 23
... deuteron : here taking into account the c.m. motion is trivially accom- plished by using the wave functions of the relative motion , ø ( r ) . + R IN T H2 SH For example , the elastic scattering amplitude is M ( A ) = ik 2π : / db exp ...
... deuteron : here taking into account the c.m. motion is trivially accom- plished by using the wave functions of the relative motion , ø ( r ) . + R IN T H2 SH For example , the elastic scattering amplitude is M ( A ) = ik 2π : / db exp ...
Page 25
... deuteron target . A lot of attention was concentrated on the deuteron because it is a very important testing ground for multiple scattering theories ( or models ) . ( i ) In experiments ( compare deuteron data contained in [ S1 ] ...
... deuteron target . A lot of attention was concentrated on the deuteron because it is a very important testing ground for multiple scattering theories ( or models ) . ( i ) In experiments ( compare deuteron data contained in [ S1 ] ...
Page 26
... deuteron ground state ) . Let us discuss this effect in more detail . The ground state deuteron wave function is : Om ( r ) = ( 4π ) −1 / 2p − 1 [ u ( r ) + 8−1 / 2 S12W ( r ) ] x1 , m where u ( r ) and w ( r ) are the radial S and D ...
... deuteron ground state ) . Let us discuss this effect in more detail . The ground state deuteron wave function is : Om ( r ) = ( 4π ) −1 / 2p − 1 [ u ( r ) + 8−1 / 2 S12W ( r ) ] x1 , m where u ( r ) and w ( r ) are the radial S and D ...
Page 27
... deuteron example . In the standard Glauber model , it is enough to have p ( s ) = √∞ dzó 。* ( s , z ) Þo ( s , z ) to compute the cross section . Suppose there is some deformation in the final state : 40 * ( s , 2 ) → o ' * ( A , s ...
... deuteron example . In the standard Glauber model , it is enough to have p ( s ) = √∞ dzó 。* ( s , z ) Þo ( s , z ) to compute the cross section . Suppose there is some deformation in the final state : 40 * ( s , 2 ) → o ' * ( A , s ...
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