Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 18
... corrections to be discussed ( although they are , in principle , included in the algorithm presented above ) are : ( i ) the Coulomb corrections which play an important role in elastic scattering from nuclei of charged hadrons , and ...
... corrections to be discussed ( although they are , in principle , included in the algorithm presented above ) are : ( i ) the Coulomb corrections which play an important role in elastic scattering from nuclei of charged hadrons , and ...
Page 19
Wiesław Czyż. 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 cal- culation has been done , e.g. ...
Wiesław Czyż. 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 cal- culation has been done , e.g. ...
Page 22
... corrections insignificant in do DT / do . How important are the details of the target nucleus wave function ? Not very important . The most important are general characteristics : density distributions ( hence possible deformations ) ...
... corrections insignificant in do DT / do . How important are the details of the target nucleus wave function ? Not very important . The most important are general characteristics : density distributions ( hence possible deformations ) ...
Page 23
... correction factor to M = ( M ( △ ; 81 ... SA ) ) assuming the wave function to be in the form of a product of the ... corrected amplitude . ( 3.9 ) Hence if we can factor out the c.m. wave function 23.
... correction factor to M = ( M ( △ ; 81 ... SA ) ) assuming the wave function to be in the form of a product of the ... corrected amplitude . ( 3.9 ) Hence if we can factor out the c.m. wave function 23.
Page 24
... correction factor : ( R ( r ) | exp ( i △ · r ) | R ( r ) ) −1 . This can be done explicitly in the case of oscillator potential wave functions ( this is partly the reason why they are so popular ! ) . There ® ( r ) = ( A / π3R6 ) 1/4 ...
... correction factor : ( R ( r ) | exp ( i △ · r ) | R ( r ) ) −1 . This can be done explicitly in the case of oscillator potential wave functions ( this is partly the reason why they are so popular ! ) . There ® ( r ) = ( A / π3R6 ) 1/4 ...
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 |
| Export Citation | BiBTeX EndNote RefMan |