Interactions of High Energy Particles with Nuclei |
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Page 18
... O PROD ) it follows that the measurements of otot may be a good way of finding out whether the inelastic shadowing ( or inelastic screening ) corrections are important at very high energies : If one computed o tot from the Glauber ...
... O PROD ) it follows that the measurements of otot may be a good way of finding out whether the inelastic shadowing ( or inelastic screening ) corrections are important at very high energies : If one computed o tot from the Glauber ...
Page 19
In order to compute the amplitude one has to bear in mind that at large b , xc ( 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 ...
In order to compute the amplitude one has to bear in mind that at large b , xc ( 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 ...
Page 20
... exp ( ix ( 6 ) ) ( 1– r ( 6 ) ) ] . с 0 P This last integral has no divergences anymore ( although xe ( b ) and xc ( 6 ) both diverge logarithmically at large b ) . In general x6 ( 6 ) has to be computed numerically Ze2 PA ( r ) !
... exp ( ix ( 6 ) ) ( 1– r ( 6 ) ) ] . с 0 P This last integral has no divergences anymore ( although xe ( b ) and xc ( 6 ) both diverge logarithmically at large b ) . In general x6 ( 6 ) has to be computed numerically Ze2 PA ( r ) !
Page 23
SA ) = exp ( iA.r ) m ' ( A ; si ' ... sa ' ) ( 3.8 ) Then we can compute the correction factor to M = ( M ( A ; 81 ... SA ) ) assuming the wave function to be in the form of a product of the c.m. wave function and the internal wave ...
SA ) = exp ( iA.r ) m ' ( A ; si ' ... sa ' ) ( 3.8 ) Then we can compute the correction factor to M = ( M ( A ; 81 ... SA ) ) assuming the wave function to be in the form of a product of the c.m. wave function and the internal wave ...
Page 27
In the standard Glauber model , it is enough to have p ( s ) = 8 dz o * ( s , z ) $ ( 3 , 2 ) to compute the cross section . Suppose there is some deformation in the final state : 00 * ( s , 2 ) +00 ' * ( A , S , 2 ) * ( one can assume ...
In the standard Glauber model , it is enough to have p ( s ) = 8 dz o * ( s , z ) $ ( 3 , 2 ) to compute the cross section . Suppose there is some deformation in the final state : 00 * ( s , 2 ) +00 ' * ( A , S , 2 ) * ( one can assume ...
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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 |
| Export Citation | BiBTeX EndNote RefMan |