Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 1
... components in such interactions . This article is divided into seven sections : ( 1 ) Introduction , ( 2 ) Description of multiple scat- tering , ( 3 ) Elastic scattering of hadrons from nuclei , ( 4 ) Diffractive dissociation and ...
... components in such interactions . This article is divided into seven sections : ( 1 ) Introduction , ( 2 ) Description of multiple scat- tering , ( 3 ) Elastic scattering of hadrons from nuclei , ( 4 ) Diffractive dissociation and ...
Page 5
... components ( in x , y plane ) are marked 1. Thus , finally , we find a - Əz 2 • - E1 ) - + eV — Kß ( ± 1 · B1— îα1 · E1 ) | = 0 . ( 2.4 ) So , if the anamalous magnetic moment K = 0 , we end up with an expression which is virtually the ...
... components ( in x , y plane ) are marked 1. Thus , finally , we find a - Əz 2 • - E1 ) - + eV — Kß ( ± 1 · B1— îα1 · E1 ) | = 0 . ( 2.4 ) So , if the anamalous magnetic moment K = 0 , we end up with an expression which is virtually the ...
Page 6
... component spinor because F has to satisfy the relation So , F can be taken in the form ( 1 — α3 ) F = 0 , α3 ... components of the spinor x ) . Call In general a ( x , y , z ) = K ( 81 · В1 - ¿ ò1 · Е1σ2 ) . [ a ( x , y , z ) , A ...
... component spinor because F has to satisfy the relation So , F can be taken in the form ( 1 — α3 ) F = 0 , α3 ... components of the spinor x ) . Call In general a ( x , y , z ) = K ( 81 · В1 - ¿ ò1 · Е1σ2 ) . [ a ( x , y , z ) , A ...
Page 11
... component of re , ) , with f ( ke ) correctly given by the inverse of y ( b ) . One can see this by shifting the origin of integra- tion to ke1 : Then and 8 = kei + q ( we introduce a new variable q ) . zk2 - 82 + 8.b≈kr- 1 q2r 2 k ...
... component of re , ) , with f ( ke ) correctly given by the inverse of y ( b ) . One can see this by shifting the origin of integra- tion to ke1 : Then and 8 = kei + q ( we introduce a new variable q ) . zk2 - 82 + 8.b≈kr- 1 q2r 2 k ...
Page 12
... COMPONENTS ( b ) B COMPONENTS The profile describing the collision of two elements is : Yjk ( b - s , + s , ( a ) ) . For the sake of simplicity let us take the wave functions of ( a ) and ( b ) in the form of products of single ...
... COMPONENTS ( b ) B COMPONENTS The profile describing the collision of two elements is : Yjk ( b - s , + s , ( a ) ) . For the sake of simplicity let us take the wave functions of ( a ) and ( b ) in the form of products of single ...
Common terms and phrases
absorption additivity of phase anomalous magnetic moment ú approximately assume attenuation beam Bureau of Standards coherent diffractive production collision Compton scattering compute Coulomb interactions Czyż d³r db bJo 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 Απ γν ΦΩ