Abstract
The differential cross sections and the analyzing powers were measured for the $^{24}\mathrm{Mg}(\stackrel{\ensuremath{\rightarrow}}{\mathrm{p}},\mathrm{d})^{23}\mathrm{Mg}$ reaction at 65 and 80 MeV. Adiabatic model and distorted-wave Born approximation calculations were performed for the transitions to the ${\frac{5}{2}}^{+}$, 0.45 MeV, the ${\frac{1}{2}}^{+}$, 2.36 MeV, and the ${\mathrm{\textonehalf{}}}^{+}$, 4.36 MeV states. Analyses were also performed for the published data at incident energies of 33.6 and 94.8 MeV. The adiabatic approximation with the nonlocal correction could reproduce the experimental data with the same quality over the whole energy region investigated. The nonlocal correction was important to reproduce the pronounced oscillation of the experimental $l=0$ analyzing powers. The extracted spectroscopic factors are consistent with the theoretical predictions for both the ${\frac{5}{2}}^{+}$ and the ${\frac{1}{2}}^{+}$ states.[NUCLEAR REACTIONS $^{24}\mathrm{Mg}(\stackrel{\ensuremath{\rightarrow}}{\mathrm{p}},\mathrm{d})$, $E=65,80$ MeV; measured $\ensuremath{\sigma}(\ensuremath{\theta})$, $A(\ensuremath{\theta})$. Enriched target. Adiabatic model and DWBA analyses.]
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