Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 1-5 of 15
Page 18
... computed σTOT from the Glauber model ( including all possible effects which the model allows for ) and then found a definite dis- crepancy with experimentally measured Tor - it would very strongly suggest the existence of inelastic ...
... computed σTOT from the Glauber model ( including all possible effects which the model allows for ) and then found a definite dis- crepancy with experimentally measured Tor - it would very strongly suggest the existence of inelastic ...
Page 19
... compute the amplitude one has to bear in mind that at large b , x . ( b ) behaves like a Coulomb phase shift produced by a point charge and hence diverges logarithmically . But we do know the analytic expression for the Coulomb ...
... compute the amplitude one has to bear in mind that at large b , x . ( b ) behaves like a Coulomb phase shift produced by a point charge and hence diverges logarithmically . But we do know the analytic expression for the Coulomb ...
Page 20
... computed numerically Ze2 Xc ( b ) = - v [ ** dz [ d3r ' PA ( ) | r - r ' | = where r ( b , z ) . Note that dz lim xa ( b ) = v Ze2 [ ** def d''PA ( 1 ) Hence , for large b , xc ( b ) → xc2 ( b ) and the integral for M converges . Let ...
... computed numerically Ze2 Xc ( b ) = - v [ ** dz [ d3r ' PA ( ) | r - r ' | = where r ( b , z ) . Note that dz lim xa ( b ) = v Ze2 [ ** def d''PA ( 1 ) Hence , for large b , xc ( b ) → xc2 ( b ) and the integral for M converges . Let ...
Page 23
... compute the correction factor to M = ( M ( △ ; 81 ... SA ) ) assuming the wave function to be in the form of a product of the c.m. wave function and the internal wave function . M = ( R ( r ) | exp ( i △ ⋅r ) | R ( r ) ) ( Þ 。( rı ...
... compute the correction factor to M = ( M ( △ ; 81 ... SA ) ) assuming the wave function to be in the form of a product of the c.m. wave function and the internal wave function . M = ( R ( r ) | exp ( i △ ⋅r ) | R ( r ) ) ( Þ 。( rı ...
Page 27
... compute the cross section . Suppose there is some deformation in the final state : Po * ( s , 2 ) → o ' * ( A , s , z ) ( one can assume that the deformation is defined by the momentum transfer A ) . Then we should replace p ( 8 ) → I ...
... compute the cross section . Suppose there is some deformation in the final state : Po * ( s , 2 ) → o ' * ( A , s , z ) ( one can assume that the deformation is defined by the momentum transfer A ) . Then we should replace p ( 8 ) → I ...
Common terms and phrases
absorption additivity analysis approximately assume attenuation beam coherent collision complete components compute consider contribution corrections Coulomb Coulomb interactions coupling cross section db exp db exp i▲·b depend describe deuteron diffractive production processes discussed effects elastic scattering elastic scattering amplitude equation example excited existence experimental experiments expression fact factor field final formula forward given gives Glauber ground hadrons Hence high energy limit important incident particle inelastic initial Institute interactions introduce magnetic mass measurement momentum transfer multiple scattering Note nuclear nuclear targets nuclei nucleon numbers objects obtained parameters phase shifts photon photoproduction physical position possible problem profiles regeneration shadowing single Standards step strong structure technical vector meson wave function weak
Bibliographic information
| Title | Interactions of High Energy Particles with Nuclei Volume 139 of NBS monograph |
| Author | Wiesław Czyż |
| Publisher | National Bureau of Standards, 1975 |
| Original from | the University of Michigan |
| Digitized | 21 Nov 2007 |
| Length | 69 pages |
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