Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 6-10 of 25
Page 19
... high energy limit , the total phase shift is the sum of the Coulomb phase shift ( xe , the phase shift one would get if the strong interactions were switched off ) and the strong interaction phase shift ( x , the phase shift we would ...
... high energy limit , the total phase shift is the sum of the Coulomb phase shift ( xe , the phase shift one would get if the strong interactions were switched off ) and the strong interaction phase shift ( x , the phase shift we would ...
Page 20
... limiting procedure A → ∞ , one should keep eix ) under the integral sign of the expression for M [ 12 ] ... limit our- selves to forward scattering processes ) we can approximate y ( b ) ≈y ( 0 ) d ‹ 2 ) ( b ) , hence ik f ...
... limiting procedure A → ∞ , one should keep eix ) under the integral sign of the expression for M [ 12 ] ... limit our- selves to forward scattering processes ) we can approximate y ( b ) ≈y ( 0 ) d ‹ 2 ) ( b ) , hence ik f ...
Page 21
... limit , determined by the size and sign of an and a ,. Some calculations were done [ 15 ] with p ( r ) : Po ( 1 - exp [ ( r - R ) / c ] ) . For 208 Pb , R - 6.5 fm and c = 0.523 fm . The densities pa ( b ) , pp ( b ) were obtained by ...
... limit , determined by the size and sign of an and a ,. Some calculations were done [ 15 ] with p ( r ) : Po ( 1 - exp [ ( r - R ) / c ] ) . For 208 Pb , R - 6.5 fm and c = 0.523 fm . The densities pa ( b ) , pp ( b ) were obtained by ...
Page 28
... limit E → ∞ ( ii ) the target plays a passive role ( except in double diffraction , but in any case : no quantum numbers are exchanged ) . Examples : in QED ; elastic electron ( positron ) scattering from a Coulomb field , Delbrück ...
... limit E → ∞ ( ii ) the target plays a passive role ( except in double diffraction , but in any case : no quantum numbers are exchanged ) . Examples : in QED ; elastic electron ( positron ) scattering from a Coulomb field , Delbrück ...
Page 35
... energies . But in the limit of very high energies and small momentum transfer , all such effects dis- appear . Let us take , e.g. , two such states and give them the same momentum p . Then their energies differ : E - E * = √p2 + M2 ...
... energies . But in the limit of very high energies and small momentum transfer , all such effects dis- appear . Let us take , e.g. , two such states and give them the same momentum p . Then their energies differ : E - E * = √p2 + M2 ...
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