Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 1-5 of 14
Page 19
... absorption , which is given by dominating process , but not έ ( 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 some drastic changes may ...
... absorption , which is given by dominating process , but not έ ( 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 some drastic changes may ...
Page 28
... 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 ) ¥ 2 = n2 ¥ z + ny where is the wave polarized in the x direction and V ...
... 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 ) ¥ 2 = n2 ¥ z + ny where is the wave polarized in the x direction and V ...
Page 29
... ABSORBING TARGET Z = 0 29 y = = 2 < 0 z > 0 . The " undisturbed " wave is Y , everywhere , hence the scattered wave is 0 , Y2 - Y = - z < 0 Yn - 4 , z > 0 . Actually it is more important for our purposes to introduce partial absorption ...
... ABSORBING TARGET Z = 0 29 y = = 2 < 0 z > 0 . The " undisturbed " wave is Y , everywhere , hence the scattered wave is 0 , Y2 - Y = - z < 0 Yn - 4 , z > 0 . Actually it is more important for our purposes to introduce partial absorption ...
Page 30
... absorption in the target we assume known : | { ; ) = Σdij | λ ; ) | Xi ) = Σcij | X ; ) 2 | Xi ) , | X ; ) form orthonormal sets ( 4.1 ) of states . | λ ; ) = Σ Σ c ;; d ; 1 | Mı ) = | λi ) , hence Σcij djr = dil . j So , The states ...
... absorption in the target we assume known : | { ; ) = Σdij | λ ; ) | Xi ) = Σcij | X ; ) 2 | Xi ) , | X ; ) form orthonormal sets ( 4.1 ) of states . | λ ; ) = Σ Σ c ;; d ; 1 | Mı ) = | λi ) , hence Σcij djr = dil . j So , The states ...
Page 31
... absorption of the incident particle . One still faces the problem of specifying the absorption parameters 7 ; and the coefficients e¿j . The coefficient 7 ; of the incident particle is , as a rule , easy because this is a well - known ...
... absorption of the incident particle . One still faces the problem of specifying the absorption parameters 7 ; and the coefficients e¿j . The coefficient 7 ; 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 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