Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 8
... ( hence B = 0 , but E0 ) , we have M ( A ) ~ ix , + + { S db exp ( ia - b ) [ 1– exp ( -ie [ ** dz V ( b , z ) + i + if ** dza ( b , z ) > ) } } Xi , where 0 , -i ( x - iy ) V ' ( r ) a ( b , z ) = K r i ( x + iy ) , 0 Note that since the ...
... ( hence B = 0 , but E0 ) , we have M ( A ) ~ ix , + + { S db exp ( ia - b ) [ 1– exp ( -ie [ ** dz V ( b , z ) + i + if ** dza ( b , z ) > ) } } Xi , where 0 , -i ( x - iy ) V ' ( r ) a ( b , z ) = K r i ( x + iy ) , 0 Note that since the ...
Page 9
... ( hence a very relevant kind of particle to our further analysis ) . Example 2. Scattering of a charged vector meson in a static field ( we shall quote the results , for more details see refs . [ 9 , 10 ] ) . Let us allow for our vector ...
... ( hence a very relevant kind of particle to our further analysis ) . Example 2. Scattering of a charged vector meson in a static field ( we shall quote the results , for more details see refs . [ 9 , 10 ] ) . Let us allow for our vector ...
Page 10
... ( hence when ( 2.7 ) is valid because the definition of g is through the equation M = g ( e / 2m ) S ) the projection of the polarization on the direction of motion is constant , and hence there is no coupling between various spin ...
... ( hence when ( 2.7 ) is valid because the definition of g is through the equation M = g ( e / 2m ) S ) the projection of the polarization on the direction of motion is constant , and hence there is no coupling between various spin ...
Page 11
... Hence , away from the scatterer , one would guess the following shape of the wave ( compare D. R. Yennie article in [ S3 ] ) : 1 eik 2- d2d exp ( iz√k2 - d2 ) exp ( id · b ) ƒ ( 8 ) → ik z — y ( b ) e ik z ( for small z's ) . ( 3.1 ) ...
... Hence , away from the scatterer , one would guess the following shape of the wave ( compare D. R. Yennie article in [ S3 ] ) : 1 eik 2- d2d exp ( iz√k2 - d2 ) exp ( id · b ) ƒ ( 8 ) → ik z — y ( b ) e ik z ( for small z's ) . ( 3.1 ) ...
Page 13
... Hence the formula ( 3.2 ) sums over all intermediate excited states . For instance , the above contribution gives : ALL POSSIBLE EXCITED STATES Suppose we reject the intermediate excited states and take only the ground state as a ...
... Hence the formula ( 3.2 ) sums over all intermediate excited states . For instance , the above contribution gives : ALL POSSIBLE EXCITED STATES Suppose we reject the intermediate excited states and take only the ground state as a ...
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