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KC 2 2:00 PM<br />

R-matrix Analysis for n+ 16 O Cross-Sections up to En = 6.0 MeV with Covariance<br />

S. Kunieda, K. Shibata and T. Fukahori<br />

Japan Atomic Energy Agency, Tokai-mura Naka-gun, Ibaraki 319-1195, Japan<br />

T. Kawano, M. Paris, G. Hale<br />

Los Alamos <strong>National</strong> <strong>Laboratory</strong>, Los Alamos, NM 87545, U.S.A.<br />

Oxygen is one of the most important materials in nuclear applications such as reactors, in the form of<br />

water and oxide. Therefore, both experimental and theoretical studies have been devoted to know the<br />

accurate neutron cross sections for 16 O over the years. Nowadays, the oxygen data in the evaluated nuclear<br />

data libraries such as ENDF/B-VII.1, JENDL-4 and JEFF-3.1.2 are believed to be reasonable, since they<br />

well perform in criticality benchmarks. Since there are increasing demands for giving uncertainties in<br />

evaluated cross sections to estimate the margin of integral calculations, the covariance data are available in<br />

ENDF/B-VII.1 and JENDL-4 for 16 O cross sections. However these covariances are estimated in a simple<br />

way inferred only from experimental information. This situation is also true for many other light nuclei.<br />

Purpose of this work is to estimate n+ 16 O cross sections and their uncertainties by analysing experimental<br />

data with theoretical model. We carry out the R-matrix analysis for the 17 O system to deduce model<br />

parameters with uncertainties up to En = 6.0 MeV. Because the (n, α) reaction channel opens at about<br />

En = 2.4 MeV, two partitions of the 17 O system - 16 O+n and 13 C+α - are considered in the analysis.<br />

Measured data we use are neutron total cross section for 16 O and 13 C(α, n) 16 O reaction cross sections.<br />

The covariance matrix is obtained by propagating uncertainties of model parameters to the cross sections.<br />

The uncertainty we obtained is strongly dependent on the resonant behavior.<br />

KC 3 2:20 PM<br />

Progress in Developing Nuclear Reaction Calculation Code CCONE for Higher Energy<br />

Nuclear Data Evaluation<br />

O. Iwamoto<br />

Nuclear Science and Engineering Directorate, Japan Atomic Energy Agency<br />

The nuclear reaction calculation code CCONE [1] was developed and used for the nuclear data evaluation<br />

for JENDL/AC-2008 and JENDL-4.0. It is planned to extend the evaluated data in JENDL-4.0 toward<br />

higher energy. To adapt the CCONE code to the high energy nuclear data evaluation, the pre-equilibrium<br />

exciton model part has been extended to be able to calculate multiple particle emission. It is realized<br />

by sequential calculation of exciton states for all residual nuclei left by particle emissions. In addition,<br />

Iwamoto-Harada cluster coalescence model has been incorporated in the multiple-emission exciton model<br />

to improve calculation accuracies of cluster emission spectra such as alpha particles. The calculated results<br />

of light particle emission spectra are compared with experimental data and evaluated data.<br />

[1] O. Iwamoto, “Development of a Comprehensive Code for Nuclear Data Evaluation, CCONE, and<br />

Validation Using Neutron-Induced Cross Sections for Uranium Isotopes”, J. Nucl. Sci. Technol., 44, pp.<br />

687-697 (2007).<br />

KC 4 2:40 PM<br />

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