Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
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Page 1
... incident particle - target nucleon , some new 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 ...
... incident particle - target nucleon , some new 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 ...
Page 2
... particle scatters from a collection of A particles at very small angles ( in the Glauber model [ S1 ] ) . TARGET ... incident particle in laboratory frame A is the two - dimensional momentum transfer b is the impact parameter x ; ( b ) ...
... particle scatters from a collection of A particles at very small angles ( in the Glauber model [ S1 ] ) . TARGET ... incident particle in laboratory frame A is the two - dimensional momentum transfer b is the impact parameter x ; ( b ) ...
Page 3
... incident particle interacting through potentials with the target particles . For instance , in the case of the Schrödinger equation E ↓ = 2m • ( 22 + V ) v in the limit E → ∞ , 2 and for the incident particle moving along the z axis ...
... incident particle interacting through potentials with the target particles . For instance , in the case of the Schrödinger equation E ↓ = 2m • ( 22 + V ) v in the limit E → ∞ , 2 and for the incident particle moving along the z axis ...
Page 7
... incident particle is responsible for the existence of more than one channel . For instance , the presence of an anomalous magnetic moment can be looked upon as a mark of " compositeness . " Suppose Anm ( F , F1 , ... ... ... , r ^ ) = Ĉ ...
... incident particle is responsible for the existence of more than one channel . For instance , the presence of an anomalous magnetic moment can be looked upon as a mark of " compositeness . " Suppose Anm ( F , F1 , ... ... ... , r ^ ) = Ĉ ...
Page 10
... incident particles whose internal structure one can neglect ( in particular the internal quantum numbers can be neglected ) . Let us start with just one scatterer : TARGET SHADOW 2 = 0 The incident wave : ekz . The wave immediately ...
... incident particles whose internal structure one can neglect ( in particular the internal quantum numbers can be neglected ) . Let us start with just one scatterer : TARGET SHADOW 2 = 0 The incident wave : ekz . The wave immediately ...
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 |