Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 21
... expression ( 3.7 ) one can see that the interplay of xc ( b ) and § ( b ) is , in this optical limit , determined by the size and sign of an and a ,. Some calculations were done [ 15 ] with p ( r ) : Po ( 1 - exp [ ( r - R ) / c ] ...
... expression ( 3.7 ) one can see that the interplay of xc ( b ) and § ( b ) is , in this optical limit , determined by the size and sign of an and a ,. Some calculations were done [ 15 ] with p ( r ) : Po ( 1 - exp [ ( r - R ) / c ] ...
Page 33
... expression for Ko , where • + ∞ P.p ( b ) = po dz [ 1+ exp ( ~~ ) ] " . - Rn.p Cn.p The final formula is MKL → KS 0 = 1 ik 22π :) . db exp ( i △ · b ) { exp [ ixño ( b ) ] — exp [ ixà ° ( b ) ] } . The elementary amplitudes can be ...
... expression for Ko , where • + ∞ P.p ( b ) = po dz [ 1+ exp ( ~~ ) ] " . - Rn.p Cn.p The final formula is MKL → KS 0 = 1 ik 22π :) . db exp ( i △ · b ) { exp [ ixño ( b ) ] — exp [ ixà ° ( b ) ] } . The elementary amplitudes can be ...
Page 40
... expressions associated with the vertex d2 " of the processes ( i ) – ( iv ) : n = ~ ( P1 , Bw , En = √ B2 w2 + p2 + m 2 ( 0 , w1 Ep = √w2 + w , = m2 ) р = i ( -p ( 1-8 ) w , E , √√ ( 1 - B ) 2 w2 + p2 + m2 ) ( 0 < B < 1 ) where the ...
... expressions associated with the vertex d2 " of the processes ( i ) – ( iv ) : n = ~ ( P1 , Bw , En = √ B2 w2 + p2 + m 2 ( 0 , w1 Ep = √w2 + w , = m2 ) р = i ( -p ( 1-8 ) w , E , √√ ( 1 - B ) 2 w2 + p2 + m2 ) ( 0 < B < 1 ) where the ...
Page 47
... [ 1 - yv ( b − s ; ) 0 ( 2 ; —2 ; ) ] vv , ( b − s ; ) exp ( ¿ A || 2 ; ) i ji Note that this expression satisfies the correct " weak interaction " limit : when the V interaction is negligible the amplitude reduces to ikv M ( y → 47.
... [ 1 - yv ( b − s ; ) 0 ( 2 ; —2 ; ) ] vv , ( b − s ; ) exp ( ¿ A || 2 ; ) i ji Note that this expression satisfies the correct " weak interaction " limit : when the V interaction is negligible the amplitude reduces to ikv M ( y → 47.
Page 48
... expression d3r1 . A . . . M ( v →→ V ) = f ď3r ... ... Pra | ¥ ( x1 , ... ... r1 ) | 2 Σ M , π - V ( q ) exp ( iq⋅r ; ) where q = ( 4 , 4 ) , and M , i are the amplitudes for the production of a V meson on the jth nucleon with the ...
... expression d3r1 . A . . . M ( v →→ V ) = f ď3r ... ... Pra | ¥ ( x1 , ... ... r1 ) | 2 Σ M , π - V ( q ) exp ( iq⋅r ; ) where q = ( 4 , 4 ) , and M , i are the amplitudes for the production of a V meson on the jth nucleon with the ...
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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