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JAEA-Conf 2011-002 - 日本原子力研究開発機構

JAEA-Conf 2011-002 - 日本原子力研究開発機構

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Fig. 1 A conceptural picture of the surrogate reaction. This particular example shows<br />

a way to determine neutron cross sections of short-lived nucleus 239 U (T1/2=23 min.) by<br />

populating the same compound nucleus 240 U via 238 U( 18 O, 16 O) 240 U reaction.<br />

These problems are fundamental in nature, so reseach from the viewpoint of nuclear<br />

physics is necessary to understand the underlying physics and to really yield the desired<br />

neutron cross section data by the surrogate method.<br />

In this paper, a <strong>JAEA</strong>-based activity on the installation of equipments for the<br />

surrogate method and its physical justification will be explained briefly below.<br />

2. Strategy<br />

By using the surrogate method, we plan to determine primalily 1) fission cross<br />

sections, 2) capture cross sections, and subsequently 3) fission-fragment mass<br />

distributions and 4) number of prompt neutrons per fission, of minor actinides. Also,<br />

capture cross sections of LLFPs and some nuclei relevant to the s-process nucleosynthesis<br />

are in our scope. Therefore, our detection system must involve i) charged-particle<br />

detercters to identify the populated nuclear species and their excitation energies, ii)<br />

fission fragment detectors, iii) -ray detectors and iv) neutron counters. The system is<br />

Fig.2 A schematic layout of the surrogate<br />

detection system under plan<br />

<strong>JAEA</strong>-<strong>Conf</strong> <strong>2011</strong>-<strong>002</strong><br />

<br />

Fig.3 Charged-particle spectra obtained by a<br />

silicon E-E deterctor

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