l - th / 9 70 60 18 v 1 5 J un 1 99 7 Spin - Polarization Response Functions in High - Energy ( − → e , e ′ − → p ) Reactions
نویسنده
چکیده
Spin-polarization response functions are examined for high-energy (−→e , e′−→p ) reaction by computing the full 18 response functions for the proton kinetic energy Tp′ = 0.515 GeV and 3.179 GeV with an 16O target. The Dirac eikonal formalism is applied to account for the final-state interactions. The formalism is found to yield the response functions in good agreement with those calculated by the partial-wave expansion method at 0.515 GeV. We identify the response functions that depend on the spin-orbital potential in the final-state interactions, but not on the central potential. Dependence on the Diracor Pauli-type current of the nucleon is investigated in the helicitydependent response functions, and the normal-component polarization of the knocked-out proton, Pn, is computed. Also Department of Physics, the George Washington University, Washington, DC 20052 Also Department of Physics and Astronomy, California State University, Northridge, Northridge,
منابع مشابه
Spin-polarization response functions in high-energy „e¢ ,e8,p¢ ... reactions
Spin-polarization response functions for the high-energy (eW ,e8pW ) reaction are examined by computing all 18 response functions for proton kinetic energies of 0.515 and 3.170 GeV from an O target. The Dirac eikonal formalism is applied to account for the final-state interactions. It is found to yield the response functions in good agreement with those calculated by partial-wave expansion at 0...
متن کامل- th / 9 60 70 47 v 1 2 4 Ju l 1 99 6 Heavy Meson Production in Proton - Nucleus Reactions with Empirical Spectral Functions ∗
We study the production of K + , ρ, ω and φ mesons in p + 12 C reactions on the basis of empirical spectral functions. The high momentum, high removal energy part of the spectral function is found to be negligible in all cases close to the absolute threshold. Furthermore, the two-step process (pN → πN N ; πN → N + K + , ρ, ω, φ) dominates the cross section at threshold energies in line with ear...
متن کامل- th / 9 71 20 58 v 1 1 6 D ec 1 99 7 Charged current weak electroproduction of ∆ resonance
We study the weak production of ∆ (i.e. e − + p → ∆ 0 + ν e and e + + p → ∆ ++ + ¯ ν e) in the intermediate energy range corresponding to the Mainz and TJNAF electron accelerators. The differential cross sections σ(θ) are found to be of the order of 10 −39 cm 2 /sr, over a range of angles which increases with energy. The possibility of observing these reactions with the high luminosities availa...
متن کاملar X iv : n uc l - th / 9 80 90 90 v 2 1 6 M ar 1 99 9 Channel Coupling in A ( ~ e , e ′ ~ N ) B Reactions
The sensitivity of momentum distributions, recoil polarization observables, and response functions for nucleon knockout by polarized electron scattering to channel coupling in final-state interactions is investigated using a model in which both the distorting and the coupling potentials are constructed by folding density-dependent nucleon-nucleon effective interactions with nuclear transition d...
متن کاملar X iv : n uc l - th / 9 80 80 61 v 3 1 9 D ec 1 99 8 Longitudinal and Transverse Spin Responses in Relativistic Many Body Theory
We study theoretically the spin response functions using the relativistic many body theory. The spin response functions in the relativistic theory are reduced largely from the ones of the non-relativistic theory. This happens particularly to the longitudinal spin responses. This fact is able to remove the difficulty in reproducing the ratio of the longitudinal and transverse response functions ...
متن کاملذخیره در منابع من
با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید
عنوان ژورنال:
دوره شماره
صفحات -
تاریخ انتشار 1997