Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 14
... exp ( i △ · b ) [ 1– e xp ( − AB [ - d2s « « > d2s « b ) p ( a ) ( s ( a ) ) y ( b − s ( 6 ) —s ( 4 ) ) p ( b ) ... db exp ( i △ · b ) | [ 1- ( 1- S · AB d2g ( a ) d2g ( b ) p ( a ) ( s ( a ) ) y ( b − s + s ( a ) ) p ( b ) ( s ( b ) ...
... exp ( i △ · b ) [ 1– e xp ( − AB [ - d2s « « > d2s « b ) p ( a ) ( s ( a ) ) y ( b − s ( 6 ) —s ( 4 ) ) p ( b ) ... db exp ( i △ · b ) | [ 1- ( 1- S · AB d2g ( a ) d2g ( b ) p ( a ) ( s ( a ) ) y ( b − s + s ( a ) ) p ( b ) ( s ( b ) ...
Page 16
... db exp ( iồ • b ) √ ( b ) ƒ ďb'exp ( −ið · b ′ ) y * ( b ′ ) For small we have : hence ( 2π ) d28 = dô & do k20 do do , σel = [ d2b | v ( b ) | 2 . Now let us go over to composite targets . Consider the case when one " elementary ...
... db exp ( iồ • b ) √ ( b ) ƒ ďb'exp ( −ið · b ′ ) y * ( b ′ ) For small we have : hence ( 2π ) d28 = dô & do k20 do do , σel = [ d2b | v ( b ) | 2 . Now let us go over to composite targets . Consider the case when one " elementary ...
Page 19
... db bJo ( Ab ) { 1— exp [ i ( x . ( b ) + x . ( b ) ) ] } M = ik Xc is purely real but x , is not x . ( b ) = i§ ( b ) + § ( b ) , Im M = k 0 * S Re M = k 00 db bJo ( Ab ) { 1 — e − § ( b ) cos ( xc ( b ) + § ( b ) ) db bJo ( Ab ) e - ...
... db bJo ( Ab ) { 1— exp [ i ( x . ( b ) + x . ( b ) ) ] } M = ik Xc is purely real but x , is not x . ( b ) = i§ ( b ) + § ( b ) , Im M = k 0 * S Re M = k 00 db bJo ( Ab ) { 1 — e − § ( b ) cos ( xc ( b ) + § ( b ) ) db bJo ( Ab ) e - ...
Page 20
... exp [ -2in ln sin ( 20 ) + 2ioo ] n exp [ -in ln ( A2 / 4k2 ) Jezio A2 / 2k n = Ze2 / v , = 0 arg r ( 1 + in ) . and ... db bJ , ( Ab ) [ 1 − exp ( ix . ” ( b ) ) ] + ik [ * db bJo ( Ab ) exp [ ix . ” ( b ) + ix . ( b ) ] · Mc ( P ) + ...
... exp [ -2in ln sin ( 20 ) + 2ioo ] n exp [ -in ln ( A2 / 4k2 ) Jezio A2 / 2k n = Ze2 / v , = 0 arg r ( 1 + in ) . and ... db bJ , ( Ab ) [ 1 − exp ( ix . ” ( b ) ) ] + ik [ * db bJo ( Ab ) exp [ ix . ” ( b ) + ix . ( b ) ] · Mc ( P ) + ...
Page 22
... 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 course , the elastic cross section . The cross section which , upon ...
... 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 course , the elastic cross section . The cross section which , upon ...
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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