Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Page 10
... field B. This particle follows a circular trajectory with frequency - 13 B. m Its magnetic moment ( hence its spin ) precesses with frequency M e ωρ B = B. S m So eq ( 2.7 ) makes these two frequencies equal . But that means that the ...
... field B. This particle follows a circular trajectory with frequency - 13 B. m Its magnetic moment ( hence its spin ) precesses with frequency M e ωρ B = B. S m So eq ( 2.7 ) makes these two frequencies equal . But that means that the ...
Page 12
... fields that " internal structure " ( in these cases the internal spin quantum numbers + anomalous magnetic moment ) breaks down the " ansatz " of additivity of phase shifts . We can also have a look at this problem from the point of ...
... fields that " internal structure " ( in these cases the internal spin quantum numbers + anomalous magnetic moment ) breaks down the " ansatz " of additivity of phase shifts . We can also have a look at this problem from the point of ...
Page 28
... field , Delbrück scattering , Compton scattering , etc. in hadron physics ; all kinds of elastic hadron - hadron scattering do = ƒ ( A2 ) dA2 inelastic processes : ( experiments seem to indicate that the differential cross sections ...
... field , Delbrück scattering , Compton scattering , etc. in hadron physics ; all kinds of elastic hadron - hadron scattering do = ƒ ( A2 ) dA2 inelastic processes : ( experiments seem to indicate that the differential cross sections ...
Page 39
... plete ) but in total agreement with the Bethe and Maximon formulae [ 34 ] for the high energy limit of the pair production cross section in a strong Coulomb field [ 35 ] . Example 2 : One particle exchange process : Drell and 39 AND ...
... plete ) but in total agreement with the Bethe and Maximon formulae [ 34 ] for the high energy limit of the pair production cross section in a strong Coulomb field [ 35 ] . Example 2 : One particle exchange process : Drell and 39 AND ...
Page 69
... Field : Bound States in the Infinite Moment Frame and Multi - Photon Exchange , Institute of Nuclear Physics in Krakow , preprint ( to be published ) ( 1973 ) . [ 31 ] Drell , S. D. , and Hiida , L. , Phys . Rev. Letters 7 , 199 ( 1961 ) ...
... Field : Bound States in the Infinite Moment Frame and Multi - Photon Exchange , Institute of Nuclear Physics in Krakow , preprint ( to be published ) ( 1973 ) . [ 31 ] Drell , S. D. , and Hiida , L. , Phys . Rev. Letters 7 , 199 ( 1961 ) ...
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