Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 12
... describing the collision of two elements is : Yjk ( b − s¿ ( b ) + s , ( @ ) ) . For the sake of simplicity let us take the wave functions of ( a ) and ( b ) in the form of products of single particle wave functions . Let us assume ...
... describing the collision of two elements is : Yjk ( b − s¿ ( b ) + s , ( @ ) ) . For the sake of simplicity let us take the wave functions of ( a ) and ( b ) in the form of products of single particle wave functions . Let us assume ...
Page 14
... describe hadron - hadron scattering in the high energy limit . For example , the limit when A and B become very large was considered [ 13 ] ( compare also [ 12 ] ) : lim M = A , B → ∞ ik 2π d2b exp ( i △ · b ) [ 1– e xp ( − AB ...
... describe hadron - hadron scattering in the high energy limit . For example , the limit when A and B become very large was considered [ 13 ] ( compare also [ 12 ] ) : lim M = A , B → ∞ ik 2π d2b exp ( i △ · b ) [ 1– e xp ( − AB ...
Page 28
... describe diffractive production processes in very close analogy to diffractive dissociation phenomena which are well known in the case of systems where degeneracy exists . Let us start with an example taken from optics . Consider the ...
... describe diffractive production processes in very close analogy to diffractive dissociation phenomena which are well known in the case of systems where degeneracy exists . Let us start with an example taken from optics . Consider the ...
Page 34
... describing the regeneration process K - K , we drew heavily on the known structure of K and K , ° : they are superpositions of K ° and Ko , whose elastic scattering from nucleons is reason- ably well known . 4.1 . Generalizing to Other ...
... describing the regeneration process K - K , we drew heavily on the known structure of K and K , ° : they are superpositions of K ° and Ko , whose elastic scattering from nucleons is reason- ably well known . 4.1 . Generalizing to Other ...
Page 36
... describing elastic scattering we have approximately ( compare eq ( 4.4 ) ) The production amplitude is : p≈p , + p≈π + р . Msi = ( p | T | p ) d1o d1⁄2 TM ” + ( ññ | Т | ññ ) d1⁄2o d ̧ TM ” . Suppose the target is a nucleon , then ( p ...
... describing elastic scattering we have approximately ( compare eq ( 4.4 ) ) The production amplitude is : p≈p , + p≈π + р . Msi = ( p | T | p ) d1o d1⁄2 TM ” + ( ññ | Т | ññ ) d1⁄2o d ̧ TM ” . Suppose the target is a nucleon , then ( p ...
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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