Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 6-10 of 27
Page 14
... example , the limit when A and B become very large was considered [ 13 ] ( compare also [ 12 ] ) : lim M = A , B → ∞ ik 2π d2b exp ( i △ · b ) [ 1– e xp ( − AB [ - d2s « « > d2s « b ) p ( a ) ( s ( a ) ) y ( b − s ( 6 ) —s ( 4 ) ...
... example , the limit when A and B become very large was considered [ 13 ] ( compare also [ 12 ] ) : lim M = A , B → ∞ ik 2π d2b exp ( i △ · b ) [ 1– e xp ( − AB [ - d2s « « > d2s « b ) p ( a ) ( s ( a ) ) y ( b − s ( 6 ) —s ( 4 ) ...
Page 18
... examples of such cases . To analyze this problem in more detail , one has to link it with diffractive production processes and we shall postpone such a discussion until our analysis of such processes . Here , let us make only the ...
... examples of such cases . To analyze this problem in more detail , one has to link it with diffractive production processes and we shall postpone such a discussion until our analysis of such processes . Here , let us make only the ...
Page 23
... example , a 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 For example , the elastic scattering amplitude is M ( A ) = ik 2π db exp ( i ...
... example , a 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 For example , the elastic scattering amplitude is M ( A ) = ik 2π db exp ( i ...
Page 24
... example : the ground state wave function is a Gaussian [ 19 ] . The ground state densities and the elementary amplitudes are taken in the form | ¥。| 2 = ÎÌ p ( r ' ; ) , f ( k ) = = j = 1 ( i + a ) ko 4π p ( r ) = po exp ( -r / R2 ) ...
... example : the ground state wave function is a Gaussian [ 19 ] . The ground state densities and the elementary amplitudes are taken in the form | ¥。| 2 = ÎÌ p ( r ' ; ) , f ( k ) = = j = 1 ( i + a ) ko 4π p ( r ) = po exp ( -r / R2 ) ...
Page 27
... 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 : Po * ( s , 2 ) → o ' * ( A , s , z ) ...
... 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 : Po * ( s , 2 ) → o ' * ( A , s , z ) ...
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