Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 1
... nuclear targets by high energy projectiles are discussed in this article . Special attention is paid to the interaction of high energy hadrons and photons . Interactions of high energy electrons and neutrinos are briefly men- tioned ...
... nuclear targets by high energy projectiles are discussed in this article . Special attention is paid to the interaction of high energy hadrons and photons . Interactions of high energy electrons and neutrinos are briefly men- tioned ...
Page 28
... nuclear targets supplement each other because the nuclear medium amplifies the scattering of the produced objects . The model of diffractive processes described below is based on : M. L. Good and W. D. Walker ( 1960 ) [ 23 ] . The ...
... nuclear targets supplement each other because the nuclear medium amplifies the scattering of the produced objects . The model of diffractive processes described below is based on : M. L. Good and W. D. Walker ( 1960 ) [ 23 ] . The ...
Page 45
... nuclear targets ( nuclear targets : Pb , Cu , C ) [ 37 ] . ω Nucleon targets : The authors assumed the w and contributions to or ( y , nucleon ) to be 20 ± 2 μb ( remember : this is just a small contribution ) . Then , by measuring σr ...
... nuclear targets ( nuclear targets : Pb , Cu , C ) [ 37 ] . ω Nucleon targets : The authors assumed the w and contributions to or ( y , nucleon ) to be 20 ± 2 μb ( remember : this is just a small contribution ) . Then , by measuring σr ...
Page 46
... nuclear targets and , since it is comparatively well docu- mented experimentally , it is instructive to outline it here . The production amplitude of a vector boson is ( in the limit w →→ ∞ ) Υπα M ( Y → V ) = ( 0 , kv | tv | 0 , kv ...
... nuclear targets and , since it is comparatively well docu- mented experimentally , it is instructive to outline it here . The production amplitude of a vector boson is ( in the limit w →→ ∞ ) Υπα M ( Y → V ) = ( 0 , kv | tv | 0 , kv ...
Page 53
... targets were used : H2 , Be , C , Al , Ti , Cu , Ag , Cd , In , Ta , W , Au , Pb , U. The parameters obtained from ... nuclear excitations should be removed ( ii ) processes which lead to π production ( other than p - production ) should ...
... targets were used : H2 , Be , C , Al , Ti , Cu , Ag , Cd , In , Ta , W , Au , Pb , U. The parameters obtained from ... nuclear excitations should be removed ( ii ) processes which lead to π production ( other than p - production ) should ...
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 |