Interactions of High Energy Particles with Nuclei |
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Page 3
... the initial and final wave functions of the target nucleus . One can produce many arguments which make this important formula plausible . One can use , e.g. , an optical description of attenuation of a wave penetrating a medium .
... the initial and final wave functions of the target nucleus . One can produce many arguments which make this important formula plausible . One can use , e.g. , an optical description of attenuation of a wave penetrating a medium .
Page 27
Without going into any explanation of this discrepancy , let us emphasize the following point : It is important to realize that when we use the same internal wave function in the initial and final states , we exclude , by doing this ...
Without going into any explanation of this discrepancy , let us emphasize the following point : It is important to realize that when we use the same internal wave function in the initial and final states , we exclude , by doing this ...
Page 33
... ik and an analogous expression for Ko , where + pemel ) -- [ * [ 1+ exp ( = ' ) ) " ] رام Pn.p ( = po dz -Rn , Chip The final formula is 1 ik Mkl - Kso | ab exp ( ia.b ) { exp [ ixx • ( b ) ] – exp [ ixxo ( b ) ] } . ( b ) ] } .
... ik and an analogous expression for Ko , where + pemel ) -- [ * [ 1+ exp ( = ' ) ) " ] رام Pn.p ( = po dz -Rn , Chip The final formula is 1 ik Mkl - Kso | ab exp ( ia.b ) { exp [ ixx • ( b ) ] – exp [ ixxo ( b ) ] } . ( b ) ] } .
Page 35
Then their energies differ : > M2 - M * E - E * = Vp ? + M2- Vpa + M * 2 2p p large 4 ( The only important thing in these approximations is to have very large longitudinal momenta in the initial and final states . ) ...
Then their energies differ : > M2 - M * E - E * = Vp ? + M2- Vpa + M * 2 2p p large 4 ( The only important thing in these approximations is to have very large longitudinal momenta in the initial and final states . ) ...
Page 36
T P Final state : nta = + = d , ** | ñ ) + d2an 17 ) . ñ small admixture In the sense given earlier in these notes , for the purpose of describing elastic scattering we have approximately ( compare eq ( 4.4 ) ) = a p = p * + pTp .
T P Final state : nta = + = d , ** | ñ ) + d2an 17 ) . ñ small admixture In the sense given earlier in these notes , for the purpose of describing elastic scattering we have approximately ( compare eq ( 4.4 ) ) = a p = p * + pTp .
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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 |