2009
DOI: 10.1103/physrevc.80.044602
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Cross sections of theNd143(n,α)Ce140

Abstract: Cross sections and forward/backward ratios in the laboratory reference system were measured for the 143 Nd(n,α) 140 Ce reaction at 4.0, 5.0, and 6.0 MeV and for the 147 Sm(n,α) 144 Nd reaction at 5.0 and 6.0 MeV. A twin-gridded ionization chamber and large-area back-to-back 143 Nd 2 O 3 samples and 147 Sm 2 O 3 samples were employed. Experiments were performed at the 4.5 MV Van de Graaff accelerator of Peking University, China. Fast neutrons were produced through the 2 H(d,n) 3 He reaction by using a deuterium… Show more

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Cited by 16 publications
(13 citation statements)
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“…However, above 1 MeV surprisingly significant differences up to a factor of two appear. Interestingly, the Smaragd calculation shows a similar energy dependence as the experimental data points [33,34] but it underestimates the abolute scale significantly. It is beyond the scope of the present paper to provide a detailed comparison of the Talys and Smaragd codes.…”
Section: Ce Reactionsupporting
confidence: 54%
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“…However, above 1 MeV surprisingly significant differences up to a factor of two appear. Interestingly, the Smaragd calculation shows a similar energy dependence as the experimental data points [33,34] but it underestimates the abolute scale significantly. It is beyond the scope of the present paper to provide a detailed comparison of the Talys and Smaragd codes.…”
Section: Ce Reactionsupporting
confidence: 54%
“…7. The agreement with the experimental data above 1 MeV [33,34] is reasonable although the energy dependence of the data points is not perfectly reproduced. At energies below 1 MeV the experimental data of [32,35] The calculations have been repeated using the code Smaragd [37] with its default parameters (here the MCF potential is used in the α channel by default), see Fig.…”
Section: Ce Reactionmentioning
confidence: 61%
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