Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 6-10 of 15
Page 32
... beam . TARGET WHERE K ° ARE CREATED ~ 50 % of Ko DECAY FASTER ~ 50 % of Ko DISTANCE FROM THE TARGET ко DECAY SLOWER So , after some distance only the K1 ° beam is in existence . When we let the beam hit another target we can regenerate ...
... beam . TARGET WHERE K ° ARE CREATED ~ 50 % of Ko DECAY FASTER ~ 50 % of Ko DISTANCE FROM THE TARGET ко DECAY SLOWER So , after some distance only the K1 ° beam is in existence . When we let the beam hit another target we can regenerate ...
Page 45
... beam experiments . So , it is un- likely that one should reduce it by a factor of almost 2 ! ( Unless there is a strong dependence on the invariant mass of a virtual photon ) . One can also get the correct answer when one accepts that ...
... beam experiments . So , it is un- likely that one should reduce it by a factor of almost 2 ! ( Unless there is a strong dependence on the invariant mass of a virtual photon ) . One can also get the correct answer when one accepts that ...
Page 49
... beam is different . So , in the last two expressions for M ( y → V ) our Mr → V ( q ) depend on the position of all the other nucleons . These formulae are now adapted to take care of nonnegligible A. They are being used in all ...
... beam is different . So , in the last two expressions for M ( y → V ) our Mr → V ( q ) depend on the position of all the other nucleons . These formulae are now adapted to take care of nonnegligible A. They are being used in all ...
Page 50
... beams available due to their short lifetime . Here such indirect " measurement " is possible because the vector mesons interact with nucleons before they decay . The differential photoproduction cross sections look very much like ...
... beams available due to their short lifetime . Here such indirect " measurement " is possible because the vector mesons interact with nucleons before they decay . The differential photoproduction cross sections look very much like ...
Page 54
... photoproduction of vector mesons on nuclear targets we can easily remedy this situation . So , the only change we should introduce into the formulae given for vector meson photoproduction is an attenuation of the incident beam of 54.
... photoproduction of vector mesons on nuclear targets we can easily remedy this situation . So , the only change we should introduce into the formulae given for vector meson photoproduction is an attenuation of the incident beam of 54.
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