Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 4
... magnetic moment in a given electromagnetic static field ( notation from Bjorken and Drell [ S7 ] ) : iv - eA- ке ( i - c + Fm ) = 0 , 4m where y ° A ° -y . A , i ке σμν Ξ ( y " y " —yy " ) . Denote K = 2 2m ( izoo and multiply it by y ...
... magnetic moment in a given electromagnetic static field ( notation from Bjorken and Drell [ S7 ] ) : iv - eA- ке ( i - c + Fm ) = 0 , 4m where y ° A ° -y . A , i ке σμν Ξ ( y " y " —yy " ) . Denote K = 2 2m ( izoo and multiply it by y ...
Page 5
... magnetic moment K = 0 , we end up with an expression which is virtually the same as in the case of the Schrödinger equation : a ( -i + ev ) p = 0 dz whose solution ❤ = u ( k ) exp k ) exp ( -ie [ ' _ da'V ( b , a ' ) ) 00 gives where u ...
... magnetic moment K = 0 , we end up with an expression which is virtually the same as in the case of the Schrödinger equation : a ( -i + ev ) p = 0 dz whose solution ❤ = u ( k ) exp k ) exp ( -ie [ ' _ da'V ( b , a ' ) ) 00 gives where u ...
Page 7
... magnetic moment can be looked upon as a mark of " compositeness . " Suppose Anm ( F , F1 , ... ... ... , r ^ ) = Ĉ q☺ ( r − r ; ) . j1 m Diagonalization should produce a diagonal matrix of the form : S - 1as = = \ { 3 ) ( r − r , ) 0 ...
... magnetic moment can be looked upon as a mark of " compositeness . " Suppose Anm ( F , F1 , ... ... ... , r ^ ) = Ĉ q☺ ( r − r ; ) . j1 m Diagonalization should produce a diagonal matrix of the form : S - 1as = = \ { 3 ) ( r − r , ) 0 ...
Page 8
... magnetic moment , K # 0 . Without going into any details of the calculation let us quote the results . In the case when only one Coulomb potential is present ( hence B = 0 , but E0 ) , we have M ( A ) ~ ix , + + { S db exp ( ia - b ) ...
... magnetic moment , K # 0 . Without going into any details of the calculation let us quote the results . In the case when only one Coulomb potential is present ( hence B = 0 , but E0 ) , we have M ( A ) ~ ix , + + { S db exp ( ia - b ) ...
Page 9
... magnetic moment and define the magnetic moment operator e M = ( 1 + x ) - s , 2m ( 2.6 ) ( S - spin operator ) , where i determines the value of the magnetic moment . When = 0 the equations of motion of such a particle are the so ...
... magnetic moment and define the magnetic moment operator e M = ( 1 + x ) - s , 2m ( 2.6 ) ( S - spin operator ) , where i determines the value of the magnetic moment . When = 0 the equations of motion of such a particle are the so ...
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