Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 3
... present the solution in the form k ( x , y , z ) = eik z ( x , y , z ) . If the potential is smooth enough ( so that second derivatives of can be neglected ) , one can show that satisfies the approximate equation3 ❤ which gives მ ę ...
... present the solution in the form k ( x , y , z ) = eik z ( x , y , z ) . If the potential is smooth enough ( so that second derivatives of can be neglected ) , one can show that satisfies the approximate equation3 ❤ which gives მ ę ...
Page 4
... present it here . In fact it is amazing that ( 2.1 ) works so well . Even in the conceptually simplest cases of rela- tivistic potential scattering one can give examples in which it breaks down . Examples Example 1. Dirac particle with ...
... present it here . In fact it is amazing that ( 2.1 ) works so well . Even in the conceptually simplest cases of rela- tivistic potential scattering one can give examples in which it breaks down . Examples Example 1. Dirac particle with ...
Page 8
... present ( hence B = 0 , but E0 ) , we have M ( A ) ~ ix , + + { S 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 ...
... present ( hence B = 0 , but E0 ) , we have M ( A ) ~ ix , + + { S 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 ...
Page 18
... present at intermediate steps ) are excluded . O O O They are the source of the so - called inelastic screening ( or inelastic shadowing ) phenomenon [ 47 ] . In order to include them we have to ascribe some kind of structure to the ...
... present at intermediate steps ) are excluded . O O O They are the source of the so - called inelastic screening ( or inelastic shadowing ) phenomenon [ 47 ] . In order to include them we have to ascribe some kind of structure to the ...
Page 22
... present ) that to a good approximation ( note that since this formula does not exhibit a forward dip , it is not valid for small △ ) do DT = a dn N | 2 A IS . ( A ) 1a + 2152 ( A ) 1 ] , Ꮓ A where the " effective number of nucleons ...
... present ) that to a good approximation ( note that since this formula does not exhibit a forward dip , it is not valid for small △ ) do DT = a dn N | 2 A IS . ( A ) 1a + 2152 ( A ) 1 ] , Ꮓ A where the " effective number of nucleons ...
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