Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 10
... magnetic moment M given by ( 2.7 ) moving in an almost uniform magnetic 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 ...
... magnetic moment M given by ( 2.7 ) moving in an almost uniform magnetic 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 ...
Page 12
... magnetic moment ) breaks down the " ansatz " of additivity of phase shifts . We can also have a look at this problem from the point of view of a Glauber - like description of scattering of two composite objects . The formulae given ...
... magnetic moment ) breaks down the " ansatz " of additivity of phase shifts . We can also have a look at this problem from the point of view of a Glauber - like description of scattering of two composite objects . The formulae given ...
Page 26
... magnetic quantum number m . The elastic cross - section is then doel ΦΩ = 1 Σ Σ ( m | M ( △ , s ) | m ′ ) | 2 3 m , m ' with ik M ( A , s ) = d2b exp ( i △ · b ) { 1— exp [ ix , ( b − 1⁄2s ) + ixn ( b + 1⁄2s ) ] } , 2π which operator ...
... magnetic quantum number m . The elastic cross - section is then doel ΦΩ = 1 Σ Σ ( m | M ( △ , s ) | m ′ ) | 2 3 m , m ' with ik M ( A , s ) = d2b exp ( i △ · b ) { 1— exp [ ix , ( b − 1⁄2s ) + ixn ( b + 1⁄2s ) ] } , 2π which operator ...
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