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 possible phase shifts of the pairs of ... exp ( i △ · b ) [ 1– e xp ( − AB [ - d2s « « > d2s « b ) p ( a ) ( s ( a ) ) y ( b − s ( 6 ) —s ( 4 ) ) p ( b ) ( s ( b ) ...
... ( b ) we may still use a generalized Glauber model with additivity of all possible phase shifts of the pairs of ... exp ( i △ · b ) [ 1– e xp ( − AB [ - d2s « « > d2s « b ) p ( a ) ( s ( a ) ) y ( b − s ( 6 ) —s ( 4 ) ) p ( b ) ( s ( b ) ...
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 ...
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absorption additivity analysis approximately assume attenuation beam coherent collision complete components compute consider contribution corrections Coulomb Coulomb interactions coupling cross section db exp db exp i▲·b depend describe deuteron diffractive production processes discussed effects elastic scattering elastic scattering amplitude equation example excited existence experimental experiments expression fact factor field final formula forward given gives Glauber ground hadrons Hence high energy limit important incident particle inelastic initial Institute interactions introduce magnetic mass measurement momentum transfer multiple scattering Note nuclear nuclear targets nuclei nucleon numbers objects obtained parameters phase shifts photon photoproduction physical position possible problem profiles regeneration shadowing single Standards step strong structure technical vector meson wave function weak