Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 15
... cross section ( from the optical theorem ) which is energy independent . So , it seems to be difficult to reconcile this model with the recent evidence for the increase of the total hadron - proton cross sections at very high energies ...
... cross section ( from the optical theorem ) which is energy independent . So , it seems to be difficult to reconcile this model with the recent evidence for the increase of the total hadron - proton cross sections at very high energies ...
Page 17
... cross section at the impact parameter b≈ ( l + 1⁄2 ) / k with all nucleons frozen at the positions $ 1 , SA . .. • So , in our model there are three different contributions . OEL ONLY NUCLEONS APPEAR бот NEW PARTICLES ARE PRODUCED ...
... cross section at the impact parameter b≈ ( l + 1⁄2 ) / k with all nucleons frozen at the positions $ 1 , SA . .. • So , in our model there are three different contributions . OEL ONLY NUCLEONS APPEAR бот NEW PARTICLES ARE PRODUCED ...
Page 18
... cross section is ~ 10 of elastic cross section ) . ( 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 ...
... cross section is ~ 10 of elastic cross section ) . ( 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 ...
Page 19
... cross section is doel do = | Im M2 + | Re M 2 . ( 3.6 ) ( b ) ( which is , as a rule , ( b ) because this is the The amplitude ( 3.6 ) has some simple properties which show that the Coulomb interaction may help us in learning about the ...
... cross section is doel do = | Im M2 + | Re M 2 . ( 3.6 ) ( b ) ( which is , as a rule , ( b ) because this is the The amplitude ( 3.6 ) has some simple properties which show that the Coulomb interaction may help us in learning about the ...
Page 21
... cross section for scattering on either neutron or proton . ( Incidentally , one can define an optical potential — ( 1 / v ) ƒ ‰ dz Vopt ( b , z ) = x . ( b ) which is equivalent to our multiple scattering description ) . - 00 = From ...
... cross section for scattering on either neutron or proton . ( Incidentally , one can define an optical potential — ( 1 / v ) ƒ ‰ dz Vopt ( b , z ) = x . ( b ) which is equivalent to our multiple scattering description ) . - 00 = From ...
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 |