Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 2
... 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 the two - dimensional momentum transfer b is the impact ...
... 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 the two - dimensional momentum transfer b is the impact ...
Page 3
... positions , we get for the amplitude Mfi = ik 27 / d3rı dr ... ray , * ( r ... ra ) | bexp ( iA + b ) × { 1 - exp [ Σx ; ( b − j ; ) ] } ¥ , ( r1 . . . r △ ) ik = 27 db exp ( iA.b ) d [ dr ... ... d3rAY * 2π ادر where ; and Y , are ...
... positions , we get for the amplitude Mfi = ik 27 / d3rı dr ... ray , * ( r ... ra ) | bexp ( iA + b ) × { 1 - exp [ Σx ; ( b − j ; ) ] } ¥ , ( r1 . . . r △ ) ik = 27 db exp ( iA.b ) d [ dr ... ... d3rAY * 2π ادر where ; and Y , are ...
Page 7
... positions ) are , in general , noncommuting operators and there is no way of adding phase shifts ( or , equivalently , multiplying profiles ) . We can also see that the physical reason for this phenomenon is the coupling between ...
... positions ) are , in general , noncommuting operators and there is no way of adding phase shifts ( or , equivalently , multiplying profiles ) . We can also see that the physical reason for this phenomenon is the coupling between ...
Page 17
... 2 ) / k with all nucleons frozen at the positions $ 1 , SA . .. • So , in our model there are three different contributions . OEL ONLY NUCLEONS APPEAR бот NEW PARTICLES ARE PRODUCED OPROD But as long as we construct the profiles of the 17.
... 2 ) / k with all nucleons frozen at the positions $ 1 , SA . .. • So , in our model there are three different contributions . OEL ONLY NUCLEONS APPEAR бот NEW PARTICLES ARE PRODUCED OPROD But as long as we construct the profiles of the 17.
Page 43
... position vectors of the nucleons in the target nucleus , it gives the following contribution to the total photon - nucleus cross section ( which is proportional to A ) : 4π Im MCOMPTON ( 0 ) = A k • 14 [ { N στ ( γρ ) + = στ ( γη A or ...
... position vectors of the nucleons in the target nucleus , it gives the following contribution to the total photon - nucleus cross section ( which is proportional to A ) : 4π Im MCOMPTON ( 0 ) = A k • 14 [ { N στ ( γρ ) + = στ ( γη A or ...
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