Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 1-5 of 20
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 of phase anomalous magnetic moment ú approximately assume attenuation b+½s beam Bureau of Standards coherent diffractive production collision Compton scattering compute Coulomb interactions Czyż d³r db exp i▲·b deuteron diagonalization diffractive production processes diffractive scattering discussed double scattering elastic scattering amplitude electromagnetic equation example excited experiments factor Feynman diagrams formula four-momentum Glauber model hadrons Hence high energy limit incident particle incident wave inelastic shadowing Interactions of High invariant mass K mesons multiple scattering National Bureau neutrino neutrons ññ Note nuclear matter nuclear targets nuclei nucleon obtained optical theorem parameters phase shifts photon photoproduction of vector physical pion production amplitude profiles quantum numbers regeneration Řº shadowing effects single scattering spin strongly interacting target nucleus total cross section vector meson VMD model wave function γν Σ Σ