Interactions of High Energy Particles with Nuclei |
From inside the book
Results 1-5 of 23
Page 2
The expression 1- eix ; ( b ) = Yi ( 6 ) is called the profile of the jth nucleon , incident particle collision . Assuming x ( b ) = Ï xi ( b - 8 ; ) ) and assuming that the particle goes through the target so.
The expression 1- eix ; ( b ) = Yi ( 6 ) is called the profile of the jth nucleon , incident particle collision . Assuming x ( b ) = Ï xi ( b - 8 ; ) ) and assuming that the particle goes through the target so.
Page 3
and assuming that the particle goes through the target so fast that all the nucleons are ' frozen ' at certain positions , we get for the amplitude ik Msi = db ) 2 . l dru ... dor \ , * ( no ... ra ) sa ra ) | < ob exp ( ia.b ) x { 1- ...
and assuming that the particle goes through the target so fast that all the nucleons are ' frozen ' at certain positions , we get for the amplitude ik Msi = db ) 2 . l dru ... dor \ , * ( no ... ra ) sa ra ) | < ob exp ( ia.b ) x { 1- ...
Page 12
For the sake of simplicity let us take the wave functions of ( a ) and ( b ) in the form of products of single particle wave functions . Let us assume also that all particles have the same single particle wave functions .
For the sake of simplicity let us take the wave functions of ( a ) and ( b ) in the form of products of single particle wave functions . Let us assume also that all particles have the same single particle wave functions .
Page 14
1( -AB sod 5–90–96 where the p's were defined before and we assume that all y ; i's are the same . ... If one assumes that y ( 6 ) is a very narrow function of b ( hence the components of the two hadrons are very small ) we can write ...
1( -AB sod 5–90–96 where the p's were defined before and we assume that all y ; i's are the same . ... If one assumes that y ( 6 ) is a very narrow function of b ( hence the components of the two hadrons are very small ) we can write ...
Page 19
We shall assume that , in the high energy limit , the total phase shift is the sum of the Coulomb phase shift ( xc , the phase shift one would get if the strong interactions were switched off ) and the strong interaction phase shift ...
We shall assume that , in the high energy limit , the total phase shift is the sum of the Coulomb phase shift ( xc , the phase shift one would get if the strong interactions were switched off ) and the strong interaction phase shift ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Common terms and phrases
absorption additivity analysis approximately assume attenuation beam Bureau of Standards charge coherent collision complete components compute consider contribution corrections Coulomb Coulomb interactions coupling cross section db exp depend describe deuteron diffractive production processes discussed effects elastic scattering elastic scattering amplitude equation example excited existence exp ia.b 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 National Bureau Note nuclear nuclear targets nuclei nucleon numbers objects obtained parameters phase shifts photon photoproduction physical position possible present problem profiles regeneration shadowing single Standards step strong structure technical vector meson wave function
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 |