Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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... physical measurement ; coordinates that system with measurement systems of other nations ; and furnishes essential services leading to accurate and uniform physical measurements throughout the Nation's scientific community , industry ...
... physical measurement ; coordinates that system with measurement systems of other nations ; and furnishes essential services leading to accurate and uniform physical measurements throughout the Nation's scientific community , industry ...
Page 1
... physical situa- tions may occur which stem from the complexity of the target . For example , in the case of π - nucleus scattering in the region of the ( 3 , 3 ) resonance [ 5 , 6 ] one may hope to learn something about the nature of ...
... physical situa- tions may occur which stem from the complexity of the target . For example , in the case of π - nucleus scattering in the region of the ( 3 , 3 ) resonance [ 5 , 6 ] one may hope to learn something about the nature of ...
Page 7
... physical reason for this phenomenon is the coupling between different spin states produced by the term K ( 81.B1 - id1 E102 ) . So , we have to deal with a coupled channels problem . We can also make the following remark : sometimes ...
... physical reason for this phenomenon is the coupling between different spin states produced by the term K ( 81.B1 - id1 E102 ) . So , we have to deal with a coupled channels problem . We can also make the following remark : sometimes ...
Page 30
... physical states of the system , | X ; ) ( which are analogous to the states „ and nye , of the photon ) . We want to compute ( X ; | TX ; ) . We expand | X ; ) into a set of states | A ) whose scattering and absorption in the target we ...
... physical states of the system , | X ; ) ( which are analogous to the states „ and nye , of the photon ) . We want to compute ( X ; | TX ; ) . We expand | X ; ) into a set of states | A ) whose scattering and absorption in the target we ...
Page 35
... physical proton and the physical neutron - pion pair through the " bare " states of the proton ( p ) and the neutron - pion pair ( ññ ) . π Initial state : p = + = = d1o | μ ) + d1⁄23 | ññ ) p ñ small admixture 35 π Final state : n + π ...
... physical proton and the physical neutron - pion pair through the " bare " states of the proton ( p ) and the neutron - pion pair ( ññ ) . π Initial state : p = + = = d1o | μ ) + d1⁄23 | ññ ) p ñ small admixture 35 π Final state : n + π ...
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 |