Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 1-5 of 10
Page 18
... corrections to be discussed ( although they are , in principle , included in the algorithm presented above ) are : ( i ) the Coulomb corrections which play an important role in elastic scattering from nuclei of charged hadrons , and ...
... corrections to be discussed ( although they are , in principle , included in the algorithm presented above ) are : ( i ) the Coulomb corrections which play an important role in elastic scattering from nuclei of charged hadrons , and ...
Page 19
Wiesław Czyż. Let us consider first the Coulomb corrections for heavy nuclei . One can , in principle , use the individual amplitudes which have Coulomb interactions built into them ( this very tedious cal- culation has been done , e.g. ...
Wiesław Czyż. Let us consider first the Coulomb corrections for heavy nuclei . One can , in principle , use the individual amplitudes which have Coulomb interactions built into them ( this very tedious cal- culation has been done , e.g. ...
Page 22
... corrections insignificant in do DT / do . How important are the details of the target nucleus wave function ? Not very important . The most important are general characteristics : density distributions ( hence possible deformations ) ...
... corrections insignificant in do DT / do . How important are the details of the target nucleus wave function ? Not very important . The most important are general characteristics : density distributions ( hence possible deformations ) ...
Page 23
... correction factor to M = ( M ( △ ; 81 ... SA ) ) assuming the wave function to be in the form of a product of the ... corrected amplitude . ( 3.9 ) Hence if we can factor out the c.m. wave function 23.
... correction factor to M = ( M ( △ ; 81 ... SA ) ) assuming the wave function to be in the form of a product of the ... corrected amplitude . ( 3.9 ) Hence if we can factor out the c.m. wave function 23.
Page 24
... correction factor : ( R ( r ) | exp ( i △ · r ) | R ( r ) ) −1 . This can be done explicitly in the case of oscillator potential wave functions ( this is partly the reason why they are so popular ! ) . There ® ( r ) = ( A / π3R6 ) 1/4 ...
... correction factor : ( R ( r ) | exp ( i △ · r ) | R ( r ) ) −1 . This can be done explicitly in the case of oscillator potential wave functions ( this is partly the reason why they are so popular ! ) . There ® ( r ) = ( A / π3R6 ) 1/4 ...
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