Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Results 6-10 of 23
Page 22
... cross section for such " inclusive " processes is do sc ΦΩ = n n ik Σ db exp ( i △ · b ) ( Y2 | Ã ( b ; 81 . . . 8. ) | Yo ) 12 = ( 2π ) 2 2π d2b d2b ′ exp [ i △ · ( b− b ′ ) ] { % | г + r | ¥。) . 2 This cross section includes , of ...
... cross section for such " inclusive " processes is do sc ΦΩ = n n ik Σ db exp ( i △ · b ) ( Y2 | Ã ( b ; 81 . . . 8. ) | Yo ) 12 = ( 2π ) 2 2π d2b d2b ′ exp [ i △ · ( b− b ′ ) ] { % | г + r | ¥。) . 2 This cross section includes , of ...
Page 25
... cross section in y - p production experiments on deuterons ( see section 4.2 ) . ( ii ) One can also see ( again , 25.
... cross section in y - p production experiments on deuterons ( see section 4.2 ) . ( ii ) One can also see ( again , 25.
Page 26
... 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 , in this approximation , does not ...
... 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 , in this approximation , does not ...
Page 27
... cross sections in excellent agreement with experiment . ( We are not considering here backward scattering , where ... section . Suppose there is some deformation in the final state : Po * ( s , 2 ) → o ' * ( A , s , z ) ( one can assume ...
... cross sections in excellent agreement with experiment . ( We are not considering here backward scattering , where ... section . Suppose there is some deformation in the final state : Po * ( s , 2 ) → o ' * ( A , s , z ) ( one can assume ...
Page 39
... cross section in a strong Coulomb field [ 35 ] . Example 2 : One particle exchange process : Drell and 39 AND ...
... cross section in a strong Coulomb field [ 35 ] . Example 2 : One particle exchange process : Drell and 39 AND ...
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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