Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 6-10 of 14
Page 45
... measuring σr ( y , nucleon ) one can determine ( do / d ) ( yp → pp ) |。 for which one gets much too high a value . One may get agreement if one reduces Y2 / 4 from 0.62 to 0.37 ! But y , 2 / 4π is well known from colliding beam ...
... measuring σr ( y , nucleon ) one can determine ( do / d ) ( yp → pp ) |。 for which one gets much too high a value . One may get agreement if one reduces Y2 / 4 from 0.62 to 0.37 ! But y , 2 / 4π is well known from colliding beam ...
Page 50
... measurement " is possible because the vector mesons interact with nucleons before they decay . The differential photoproduction cross sections look very much like elastic hadron - nucleus cross sections . They exhibit a steep slope at ...
... measurement " is possible because the vector mesons interact with nucleons before they decay . The differential photoproduction cross sections look very much like elastic hadron - nucleus cross sections . They exhibit a steep slope at ...
Page 51
... measured looks as follows : double scattering contributions do ( mb Gev2 ) 10 SINGLE SCATTERING D COMPONENT OF THE ... measuring the amplitudes for photoproduction of po on neutrons and protons , modulated by the deuteron form factor F ...
... measured looks as follows : double scattering contributions do ( mb Gev2 ) 10 SINGLE SCATTERING D COMPONENT OF THE ... measuring the amplitudes for photoproduction of po on neutrons and protons , modulated by the deuteron form factor F ...
Page 52
... measuring the cross section at large momentum transfers we can extract fnucleon because we know fynucleon quite well ... measurement of the elastic p - nucleon cross section in existence . ( ii ) If one wants to extract on or y , 2 / 4π ...
... measuring the cross section at large momentum transfers we can extract fnucleon because we know fynucleon quite well ... measurement of the elastic p - nucleon cross section in existence . ( ii ) If one wants to extract on or y , 2 / 4π ...
Page 53
... measured was Y + A → po + A _ +++ 00 The following targets were used : H2 , Be , C , Al , Ti , Cu , Ag , Cd , In , Ta , W , Au , Pb , U. The parameters obtained from fitting the differential cross sections to their very extensive ...
... measured was Y + A → po + A _ +++ 00 The following targets were used : H2 , Be , C , Al , Ti , Cu , Ag , Cd , In , Ta , W , Au , Pb , U. The parameters obtained from fitting the differential cross sections to their very extensive ...
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