Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 27
... WAVE FUNCTION Diffractive Scattering from the target FINAL ELECTRON - POSITRON WAVE FUNCTION the " relativistic wave functions " in an analogous way to that shown above in the case of the deuteron . Here the possibility of a well ...
... WAVE FUNCTION Diffractive Scattering from the target FINAL ELECTRON - POSITRON WAVE FUNCTION the " relativistic wave functions " in an analogous way to that shown above in the case of the deuteron . Here the possibility of a well ...
Page 47
... wave function we have ik v M ( y → V ) = = 2π A db exp ( i △ · b ) f ď3rı ...... . ď3ra d3r1 ... d3r II p ( r ; ) j - 1 × ΣII [ 1 - yv ( b − s ; ) 0 ( 2 ; —2 ; ) ] vv , ( b − s ; ) exp ( ¿ A || 2 ; ) i ji Note that this expression ...
... wave function we have ik v M ( y → V ) = = 2π A db exp ( i △ · b ) f ď3rı ...... . ď3ra d3r1 ... d3r II p ( r ; ) j - 1 × ΣII [ 1 - yv ( b − s ; ) 0 ( 2 ; —2 ; ) ] vv , ( b − s ; ) exp ( ¿ A || 2 ; ) i ji Note that this expression ...
Page 51
... WAVE FUNCTION FILLS THIS MINIMUM , DOUBLE SCATTERING | t | q2 0.5 1.0 1.5 ( GeV ) 2 From the above formulae we can see that at small momentum transfers we are essentially measuring the amplitudes for photoproduction of po on neutrons ...
... WAVE FUNCTION FILLS THIS MINIMUM , DOUBLE SCATTERING | t | q2 0.5 1.0 1.5 ( GeV ) 2 From the above formulae we can see that at small momentum transfers we are essentially measuring the amplitudes for photoproduction of po on neutrons ...
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