Interactions of High Energy Particles with Nuclei |
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Page 12
The formulae given below are interesting also because they may be used to analyze high energy nucleus - nucleus collisions ( which is not an academic problem because there are experimental pro- jects under way ) .
The formulae given below are interesting also because they may be used to analyze high energy nucleus - nucleus collisions ( which is not an academic problem because there are experimental pro- jects under way ) .
Page 14
But we shall talk about comparison with experiment at other occasions . Some special cases of formula ( 3.2 ) were also employed to describe hadron - hadron scattering in the high energy limit . For example , the limit when A and B ...
But we shall talk about comparison with experiment at other occasions . Some special cases of formula ( 3.2 ) were also employed to describe hadron - hadron scattering in the high energy limit . For example , the limit when A and B ...
Page 15
The very recent measurements of p - p elastic collisions confirm the existence of such a structure ( CERN - Serpukhov experiment ) . In the form given above , the droplet model is very crude and I do not want to go beyond this ...
The very recent measurements of p - p elastic collisions confirm the existence of such a structure ( CERN - Serpukhov experiment ) . In the form given above , the droplet model is very crude and I do not want to go beyond this ...
Page 18
( In fact this is one of the very important questions to be answered by the very high energy experiments of the future : how much cross section goes into diffractive production processes . ) ( ii ) Nondiffractive processes are ...
( In fact this is one of the very important questions to be answered by the very high energy experiments of the future : how much cross section goes into diffractive production processes . ) ( ii ) Nondiffractive processes are ...
Page 21
( b / sr ) d & LAB 10 103 10 O 100 % 10 5 10 NEUTRAL NEGATIVE CHARGE POSITIVE CHARGE 15 20 PLAB , mrad For heavy nuclei there are virtually no experiments with good 21.
( b / sr ) d & LAB 10 103 10 O 100 % 10 5 10 NEUTRAL NEGATIVE CHARGE POSITIVE CHARGE 15 20 PLAB , mrad For heavy nuclei there are virtually no experiments with good 21.
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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 |