Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Results 1-5 of 21
Page 2
... db exp ( i △ · b ) { 1— exp [ ix ; ( b − s ; ) ] } , where k is the momentum of the incident particle in laboratory frame A is the two - dimensional momentum transfer b is the impact parameter x ; ( b ) is the phase shift which ...
... db exp ( i △ · b ) { 1— exp [ ix ; ( b − s ; ) ] } , where k is the momentum of the incident particle in laboratory frame A is the two - dimensional momentum transfer b is the impact parameter x ; ( b ) is the phase shift which ...
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 4
... exp exp ( − : S_dzV ( b , 2 ' ) ) d2b exp ( iA.b ) [ ** ik = 1 db exp ( ia - b ) [ 1- exp ( − ̄_dz'V ( b , 2 ' ) ) ] ,十三- A = k - k ' . 81 2π We can see that from the additivity of the potentials A V = Σ Vj , j = 1 we recover ...
... exp exp ( − : S_dzV ( b , 2 ' ) ) d2b exp ( iA.b ) [ ** ik = 1 db exp ( ia - b ) [ 1- exp ( − ̄_dz'V ( b , 2 ' ) ) ] ,十三- A = k - k ' . 81 2π We can see that from the additivity of the potentials A V = Σ Vj , j = 1 we recover ...
Page 6
... 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 case we also have additivity of phase shifts - hence the ...
... 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 case we also have additivity of phase shifts - hence the ...
Page 8
... db exp ( ia - b ) [ 1– exp ( -ie [ ** dz V ( b , z ) + i + if ** dza ( b , z ) > ) } } Xi , where 0 , -i ( x - iy ) V ' ( r ) a ( b , z ) = K r i ( x + iy ) , 0 Note that since the z dependence is outside the spinor matrix this does ...
... db exp ( ia - b ) [ 1– exp ( -ie [ ** dz V ( b , z ) + i + if ** dza ( b , z ) > ) } } Xi , where 0 , -i ( x - iy ) V ' ( r ) a ( b , z ) = K r i ( x + iy ) , 0 Note that since the z dependence is outside the spinor matrix this does ...
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