Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 12
... experimental pro- jects under way ) . The geometry of the process is shown in figure 3 . 255 O A COMPONENTS ( b ) ( 0 ) O B COMPONENTS The profile describing the collision of two elements is : Yjk ( b − s¿ ( b ) + s , ( @ ) ) . For the ...
... experimental pro- jects under way ) . The geometry of the process is shown in figure 3 . 255 O A COMPONENTS ( b ) ( 0 ) O B COMPONENTS The profile describing the collision of two elements is : Yjk ( b − s¿ ( b ) + s , ( @ ) ) . For the ...
Page 14
... experiment . 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 ...
... experiment . 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 ...
Page 15
... experiment ) . In the form given above , the droplet model is very crude and I do not want to go beyond this qualitative description . One should perhaps mention at this point that the amplitude ( 3.4 ) contains the geometric shape of ...
... experiment ) . In the form given above , the droplet model is very crude and I do not want to go beyond this qualitative description . One should perhaps mention at this point that the amplitude ( 3.4 ) contains the geometric shape of ...
Page 18
... experiments of the future : how much cross section goes into diffractive production processes . ) ( ii ) Nondiffractive processes are presumably not contributing to the inelastic shadow- because the whole configuration of the target ...
... experiments of the future : how much cross section goes into diffractive production processes . ) ( ii ) Nondiffractive processes are presumably not contributing to the inelastic shadow- because the whole configuration of the target ...
Page 21
... - particles which interact strongly as 20 GeV nucleons . ( 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.
... - particles which interact strongly as 20 GeV nucleons . ( 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.
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 |