6533b7dafe1ef96bd126ee1e
RESEARCH PRODUCT
Quasielastic proton knockout from 16O.
J. R. CalarcoG. Van Der SteenhovenM. LeuschnerL. LapikásH. P. BlokE. JansNasser Kalantar-nayestanakiF. W. HersmanGert Jan KramerP.k.a. De Witt HubertsJ.m. Friedrichsubject
Nuclear reactionPhysicsNuclear and High Energy PhysicsProtonExcited stateBound stateHadronSum rule in quantum mechanicsAtomic physicsNucleonGround statedescription
The spectral function of the $^{16}\mathrm{O}$(e,e'p${)}^{15}$N reaction has been measured in quasielastic parallel kinematics. Momentum distributions are extracted for transitions to several discrete states, with emphasis on the low-lying positive parity states of $^{15}\mathrm{N}$. Spectroscopic factors and bound state wave functions are deduced from a DWIA analysis employing five different optical potentials. Coupled channels effects are investigated for the first four states of $^{15}\mathrm{N}$ and are found to be minimal. The spectroscopic results of the 1/${2}^{\mathrm{\ensuremath{-}}}$ ground state and the first 3/${2}^{\mathrm{\ensuremath{-}}}$ excited state indicate a 28%\ifmmode\pm\else\textpm\fi{}5.4% reduction of the valence 1p shell strength with respect to the IPSM sum rule limit for $^{16}\mathrm{O}$. The spectroscopic strength for knockout of protons from the 2s1d shell, integrated up to a missing energy of 40 MeV, is found to be 0.269\ifmmode\pm\else\textpm\fi{}0.033. The distribution of proton spectroscopic strength is determined from a multipole decomposition of the $^{16}\mathrm{O}$ spectral function.
year | journal | country | edition | language |
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1994-02-01 | Physical review. C, Nuclear physics |