Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 16
... Consider the case when one " elementary " particle scatters from a " composite " nucleus . In this case the profile is ( r ) = ( or ( b ; Si ... SA ) | Yo ) , and we can write the same relations as before : σTOT = d2b | ( T ) | 2 + ...
... Consider the case when one " elementary " particle scatters from a " composite " nucleus . In this case the profile is ( r ) = ( or ( b ; Si ... SA ) | Yo ) , and we can write the same relations as before : σTOT = d2b | ( T ) | 2 + ...
Page 18
... scattering from nuclei of charged hadrons , and ( ii ) the corrections for the c.m. motion which are important for light nuclei but unimportant for heavy ones . Let us consider first the Coulomb corrections for heavy nuclei 18.
... scattering from nuclei of charged hadrons , and ( ii ) the corrections for the c.m. motion which are important for light nuclei but unimportant for heavy ones . Let us consider first the Coulomb corrections for heavy nuclei 18.
Page 19
... consider the effects produced by the average Coulomb potential produced by the whole nucleus [ 15 ] which produces almost identical results [ 16 , 17 ] . We shall assume that , in the high energy limit , the total phase shift is the sum ...
... consider the effects produced by the average Coulomb potential produced by the whole nucleus [ 15 ] which produces almost identical results [ 16 , 17 ] . We shall assume that , in the high energy limit , the total phase shift is the sum ...
Page 22
... consider a collection of neutrons and protons which do not screen each other . Then , we would have do DT do One may suspect the following : ≈ N \ ƒn ( A ) | 2 + Z | ƒ „ ( A ) | 2 . no screening If we introduce screening there will be ...
... consider a collection of neutrons and protons which do not screen each other . Then , we would have do DT do One may suspect the following : ≈ N \ ƒn ( A ) | 2 + Z | ƒ „ ( A ) | 2 . no screening If we introduce screening there will be ...
Page 23
... consider carefully the motion of the center of mass . Take , for example , a deuteron : here taking into account the c.m. motion is trivially accom- plished by using the wave functions of the relative motion , ø ( r ) . + R For example ...
... consider carefully the motion of the center of mass . Take , for example , a deuteron : here taking into account the c.m. motion is trivially accom- plished by using the wave functions of the relative motion , ø ( r ) . + R For example ...
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