Interactions of High Energy Particles with Nuclei |
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Page 9
Scattering of a charged vector meson in a static field ( we shall quote the results , for more details see refs . [ 9 , 10 ] ) . Let us allow for our vector particle to have an arbitrary magnetic moment and define the magnetic moment ...
Scattering of a charged vector meson in a static field ( we shall quote the results , for more details see refs . [ 9 , 10 ] ) . Let us allow for our vector particle to have an arbitrary magnetic moment and define the magnetic moment ...
Page 10
In order to make the condition ( 2.7 ) more plausible , let us consider a charged particle with spin S and magnetic moment M given by ( 2.7 ) moving in an almost uniform magnetic field B. This particle follows a circular trajectory with ...
In order to make the condition ( 2.7 ) more plausible , let us consider a charged particle with spin S and magnetic moment M given by ( 2.7 ) moving in an almost uniform magnetic field B. This particle follows a circular trajectory with ...
Page 15
If we accept that the densities of hadronic matter are the same as charge densities , F ( a ) , F ( b ) are the charge form factors of the colliding hadrons . This formula was used successfully to : ( i ) reproduce the proton charge ...
If we accept that the densities of hadronic matter are the same as charge densities , F ( a ) , F ( b ) are the charge form factors of the colliding hadrons . This formula was used successfully to : ( i ) reproduce the proton charge ...
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 ...
... 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 ...
Page 19
This last expression is the Coulomb phase shift produced by a point charge . ... But we do know the analytic expression for the Coulomb scattering amplitude of point - like charges : where Mc ( P ) = ik · ƒ db 19.
This last expression is the Coulomb phase shift produced by a point charge . ... But we do know the analytic expression for the Coulomb scattering amplitude of point - like charges : where Mc ( P ) = ik · ƒ db 19.
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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 |