## Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |

### From inside the book

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**absorption**, which is given by ( b ) because this is the dominating process , but not ( b ) ) . If the Coulomb interaction is absent ( x = 0 ) the elastic cross section is invariant against the change of sign of . If , however , x.0 ... Page 28

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**absorption**of polarized light by an anisotropic absorber . The incident wave is polarized in the direction n ( perpendicular to the z direction ) . n = ( nz , ny ) ¥ n = nz ¥ z + Ny ¥ v where is the wave polarized in the x direction and ... Page 29

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**ABSORBING**TARGET + Z = 0 = Vn 2 < 0 z > 0 . The " undisturbed " wave is Y , everywhere , hence the scattered wave is 0 , z < 0 = z > 0 . Actually it is more important for our purposes to introduce partial**absorption**( in general ... Page 30

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**absorption**in the target we assume known : | λ ; ) = Σ dij | λ ; ) | λ ; ) = Σ Cij | X ; ) | | X ) , | X ) form orthonormal sets of states . | \ ; ) = Σ Σ c ;; djɩ | λr ) = | Xi ) , hence ( 4.1 ) Į j Σcij djr = dil . j The states ) are ... Page 31

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**absorption**of the incident particle . One still faces the problem of specifying the**absorption**parameters ŋ ; and the coefficients ij . The coefficient n ; of the incident particle is , as a rule , easy because this is a well - known ...### Common terms and phrases

absorption additivity of phase anomalous magnetic moment Ãº 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