Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
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Page 25
... ground for multiple scattering theories ( or models ) . ( i ) In experiments ( compare deuteron data contained in [ S1 ] ) , one can clearly see the single and double scattering . do log dA Deuteron Target Single Double Δ 2 Remark : In ...
... ground for multiple scattering theories ( or models ) . ( i ) In experiments ( compare deuteron data contained in [ S1 ] ) , one can clearly see the single and double scattering . do log dA Deuteron Target Single Double Δ 2 Remark : In ...
Page 26
... ground state ) . Let us discuss this effect in more detail . The ground state deuteron wave function is : Pm ( r ) = ( 4π ) -1 / 2-1 [ u ( r ) + 8-1 / 2 S12W ( r ) Jx1.m where u ( r ) and w ( r ) are the radial S and D functions and Sız ...
... ground state ) . Let us discuss this effect in more detail . The ground state deuteron wave function is : Pm ( r ) = ( 4π ) -1 / 2-1 [ u ( r ) + 8-1 / 2 S12W ( r ) Jx1.m where u ( r ) and w ( r ) are the radial S and D functions and Sız ...
Page 47
... ground state wave function we have ik v M ( y → V ) = = 2π A db exp ( i △ · b ) f ď3rı ...... . ď3ra d3r1 ... d3r II p ( r ; ) j - 1 × ΣII [ 1 - yv ( b − s ; ) 0 ( 2 ; —2 ; ) ] vv , ( b − s ; ) exp ( ¿ A || 2 ; ) i ji Note that this ...
... ground state wave function we have ik v M ( y → V ) = = 2π A db exp ( i △ · b ) f ď3rı ...... . ď3ra d3r1 ... d3r II p ( r ; ) j - 1 × ΣII [ 1 - yv ( b − s ; ) 0 ( 2 ; —2 ; ) ] vv , ( b − s ; ) exp ( ¿ A || 2 ; ) i ji Note that this ...
Page 49
... ground state j # i | ¥ ( † 1 ... ... ... ¤A ) | 2 ≈ ÎÌ p ( t ; ) jun1 - becomes the formula given above . Note that the same reasoning gives , in the limit of large A , M [ ( Y → V ) = A [ with d2b dz exp ( i △ b + i △ || 2 ) p ( b ...
... ground state j # i | ¥ ( † 1 ... ... ... ¤A ) | 2 ≈ ÎÌ p ( t ; ) jun1 - becomes the formula given above . Note that the same reasoning gives , in the limit of large A , M [ ( Y → V ) = A [ with d2b dz exp ( i △ b + i △ || 2 ) p ( b ...
Page 62
... ground state of the incident particle on the same footing as the excited states . This makes good sense if one believes ( following Good and Walker [ 23 ] ) that in the high energy limit the ground and excited states of the incident ...
... ground state of the incident particle on the same footing as the excited states . This makes good sense if one believes ( following Good and Walker [ 23 ] ) that in the high energy limit the ground and excited states of the incident ...
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