Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 18
... existence of inelastic shadowing phenomena described above . In fact such an analysis has recently been done for π - d scattering and seems to indicate the existence of such a discrepancy for energies above ~ 40 GeV [ 48 ] . The ...
... existence of inelastic shadowing phenomena described above . In fact such an analysis has recently been done for π - d scattering and seems to indicate the existence of such a discrepancy for energies above ~ 40 GeV [ 48 ] . The ...
Page 25
... existence of diffractive minima , which are filled by the real part of M. ( In order to have Re M0 we have to have a0 ) . ( iii ) The importance of the c.m. motion correction can be seen from the factor exp ( R242 / 4A ) . For small A ...
... existence of diffractive minima , which are filled by the real part of M. ( In order to have Re M0 we have to have a0 ) . ( iii ) The importance of the c.m. motion correction can be seen from the factor exp ( R242 / 4A ) . For small A ...
Page 26
... ( existence of the D - state in the deuteron ground state ) . Let us discuss this effect in more detail . The ground state deuteron wave function is : Pm ( r ) = ( 4π ) -1 / 2-1 [ u ( r ) + 8-1 / 2 S12W ( r ) Jx1.m where u ( r ) and w ( r ) ...
... ( existence of the D - state in the deuteron ground state ) . Let us discuss this effect in more detail . The ground state deuteron wave function is : Pm ( r ) = ( 4π ) -1 / 2-1 [ u ( r ) + 8-1 / 2 S12W ( r ) Jx1.m where u ( r ) and w ( r ) ...
Page 32
... existence . When we let the beam hit another target we can regenerate K , mesons because K ° and K ° interact differently with matter , they are absorbed differently . ( e.g. , Ko ( S = −1 ) + p → Ao ( S = − 1 ) + π + while K ° ( S ...
... existence . When we let the beam hit another target we can regenerate K , mesons because K ° and K ° interact differently with matter , they are absorbed differently . ( e.g. , Ko ( S = −1 ) + p → Ao ( S = − 1 ) + π + while K ° ( S ...
Page 52
... existence . ( ii ) If one wants to extract on or y , 2 / 4π , one can do it very safely because the analysis , at large enough q2 , depends insensitively on 7. First one extracts ( do / dt ) PNN and then by taking the ratio 2 Ye2 α 81 ...
... existence . ( ii ) If one wants to extract on or y , 2 / 4π , one can do it very safely because the analysis , at large enough q2 , depends insensitively on 7. First one extracts ( do / dt ) PNN and then by taking the ratio 2 Ye2 α 81 ...
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