Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Results 1-5 of 18
Page 2
... exp ( i △ b ) ( 1 — eix¿ ( b ) ) , is shifted to the position of the jth nucleon : f ; ( 8 ) = ik 11⁄2 / db exp ( i △ · b ) { 1— exp [ ix ; ( b − s ; ) ] } , where k is the momentum of the incident particle in laboratory frame A is ...
... exp ( i △ b ) ( 1 — eix¿ ( b ) ) , is shifted to the position of the jth nucleon : f ; ( 8 ) = ik 11⁄2 / db exp ( i △ · b ) { 1— exp [ ix ; ( b − s ; ) ] } , where k is the momentum of the incident particle in laboratory frame A is ...
Page 3
... exp [ Σx ; ( b − j ; ) ] } ¥ , ( r1 . . . r △ ) ik = 27 db exp ( iA.b ) d [ dr ... ... d3rAY * 2π ادر where ; and Y , are the initial and final wave functions of the target nucleus . Yi , ( 2.1 ) One can produce many arguments which ...
... exp [ Σx ; ( b − j ; ) ] } ¥ , ( r1 . . . r △ ) ik = 27 db exp ( iA.b ) d [ dr ... ... d3rAY * 2π ادر where ; and Y , are the initial and final wave functions of the target nucleus . Yi , ( 2.1 ) One can produce many arguments which ...
Page 6
... ( b , 2 ' ) ) , 22 [ d3rī svoеV ( b , 2 ) , where = u ( k ' ) exp ( iEz + iA . b ) , we get m f · .00 z ) 91x ( k ' , k ) = " " , û ( k ' ) rou ( k ) i ƒ db exp ( i △ -b ) [ 1 - exp ( -ie [ * dz V ( b , 2 ) ) ] M f ** 81 2π ū . So , in this ...
... ( b , 2 ' ) ) , 22 [ d3rī svoеV ( b , 2 ) , where = u ( k ' ) exp ( iEz + iA . b ) , we get m f · .00 z ) 91x ( k ' , k ) = " " , û ( k ' ) rou ( k ) i ƒ db exp ( i △ -b ) [ 1 - exp ( -ie [ * dz V ( b , 2 ) ) ] M f ** 81 2π ū . So , in this ...
Page 14
... ( b ) we may still use a generalized Glauber model with additivity of all ... exp ( i △ · b ) [ 1– e xp ( − AB [ - d2s « « > d2s « b ) p ( a ) ( s ( a ) ... db exp ( i △ · b ) | [ 1- ( 1- S · AB d2g ( a ) d2g ( b ) p ( a ) ( s ( a ) ) y ...
... ( b ) we may still use a generalized Glauber model with additivity of all ... exp ( i △ · b ) [ 1– e xp ( − AB [ - d2s « « > d2s « b ) p ( a ) ( s ( a ) ... db exp ( i △ · b ) | [ 1- ( 1- S · AB d2g ( a ) d2g ( b ) p ( a ) ( s ( a ) ) y ...
Page 20
Wiesław Czyż. where Mc ( P ) = ik · ƒ db exp ( i △ • b ) [ 1 — eix : P ] n 2k sin2 ( 120 ) exp [ -2in ln sin ( 20 ) + 2ioo ] n exp [ -in ln ( A2 / 4k2 ) Jezio A2 / 2k n = Ze2 / v , = 0 arg r ( 1 + in ) . and hence we get the convergent ...
Wiesław Czyż. where Mc ( P ) = ik · ƒ db exp ( i △ • b ) [ 1 — eix : P ] n 2k sin2 ( 120 ) exp [ -2in ln sin ( 20 ) + 2ioo ] n exp [ -in ln ( A2 / 4k2 ) Jezio A2 / 2k n = Ze2 / v , = 0 arg r ( 1 + in ) . and hence we get the convergent ...
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