Interactions of High Energy Particles with Nuclei |
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Page 18
From our discussion of the components of otot ( oel , odt , 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 ...
From our discussion of the components of otot ( oel , odt , 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 ...
Page 19
Let us consider first the Coulomb corrections for heavy nuclei . One can , in principle , use the individual amplitudes which have Coulomb interactions built into them ( this very tedious calculation has been done , e.g. , in refs .
Let us consider first the Coulomb corrections for heavy nuclei . One can , in principle , use the individual amplitudes which have Coulomb interactions built into them ( this very tedious calculation has been done , e.g. , in refs .
Page 22
These two factors make Coulomb corrections insignificant in dopt / d2 . How important are the details of the target nucleus wave function ? Not very important . The most important are general characteristics : density distributions ...
These two factors make Coulomb corrections insignificant in dopt / d2 . How important are the details of the target nucleus wave function ? Not very important . The most important are general characteristics : density distributions ...
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 24
Hence if we can factor out the c.m. wave function from the product Vo = II ; $ ; ( r ; ) we can stick to calculating M with y , but we have to multiply it by a correction factor : ( Q ( r ) | exp ( iA.r ) | R ( r ) ) - 1 .
Hence if we can factor out the c.m. wave function from the product Vo = II ; $ ; ( r ; ) we can stick to calculating M with y , but we have to multiply it by a correction factor : ( Q ( r ) | exp ( iA.r ) | R ( r ) ) - 1 .
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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 |