https://www.cns.s.u-tokyo.ac.jp/~shimoura/research/nuc_data/pdf/19.pdf

Energy levels of light nuclei A=11☆

Energy levels of light nuclei A = 12

We report the results of a theoretical study of quasielastic electron and neutrino interactions with carbon. Our approach takes into account the effects of final-state interactions between the struck nucleon and the residual nucleus, neglected in the impulse approximation, through a generalization of the spectral function formalism. The calculated electron-scattering cross sections turn out to be in very good agreement with the available data over a broad kinematical region. The impact of nuclear effects on the reconstruction of neutrino energy in charged-current quasielastic processes is also studied, and the results of our approach are compared to the predictions of the relativistic Fermi gas model, routinely employed in most Monte Carlo simulations. Finally, we discuss the limitations of the existing procedure for energy reconstruction and propose a new, improved, one. At energy ~600 MeV, we observe a sizable difference between neutrino and antineutrino scattering, important for the measurements of charge-parity symmetry violation. Our analysis suggests that a reliable determination of neutrino energy can only be obtained from models validated by a systematic comparison to the available electron-scattering data.

Improving the accuracy of neutrino energy reconstruction in charged-current quasielastic scattering off nuclear targets

Proton-induced knockout reactions with polarized and unpolarized beams

Alpha-cluster preformation factor within cluster-formation model for odd-A and odd–odd heavy nuclei

A complete set of Wolfenstein parameters (${D}_{{i}^{'}j}$), induced polarizations ($P$), and analyzing powers (${A}_{y}$) have been measured for ($p,2p$) reactions on $^{6}\mathrm{Li}$, $^{12}\mathrm{C}$, and $^{40}\mathrm{Ca}$ targets in order to investigate possible nuclear medium effects on the nucleon-nucleon ($\mathit{NN}$) interaction. Most of these observables show significant reductions from the values for proton-proton scattering as monotonic functions of the nuclear density relevant to these reactions. The reductions of these ${D}_{{i}^{'}j}$ are reasonably reproduced by nonrelativistic plane-wave and distorted-wave calculations based on the impulse approximation, demonstrating that these suppressions are attributed to changes of the two body kinematics due to the finite separation energies of these reactions, while the reductions of ${A}_{y}$ and $P$ are much more prominent than the calculations. The relativistic calculations, which partly explain the ${A}_{y}$ and $P$ reductions, cannot reproduce the ${D}_{{i}^{'}j}$ data, but all the data are consistently reproduced when the parameters of the $\mathit{NN}$ interaction in a meson exchange model are renormalized, suggesting possible modifications of the $\mathit{NN}$ interaction by the surrounding nuclear medium.

Wolfenstein parameters for s1/2 proton knockout (p,2p) reactions

s 1/2 陽子ノックアウト(p,2p)反応に対するWolfensteinパラメータ

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Wolfenstein parameters for s1/2 proton knockout (p,2p) reactions

s 1/2 陽子ノックアウト(p,2p)反応に対するWolfensteinパラメータ