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Program - Brookhaven National Laboratory

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Neutron capture measurements of dysprosium were performed at the electron linear accelerator facility of<br />

the Rensselaer Polytechnic Institute by using the time-of-flight technique in the energy region from 10 eV<br />

to 1 keV. The neutron capture experiments were made with a 16-section NaI multiplicity detector at a<br />

flight path length of 25.5 m. High purity isotopic samples of 161Dy, 162Dy, 163Dy, 164Dy as well as one<br />

natural dysprosium sample with thickness of 0.508 mm were prepared for this measurement. Resonance<br />

parameters were extracted from the data using simultaneous fit with the multilevel R-matrix Bayesian code<br />

SAMMY 8.0. New resonances are proposed, and other resonances previously identified in the literature<br />

have been revised. The resonance Integral (RI) was calculated for each dysprosium isotope using the codes<br />

NJOY and INTER. The resonance integrals calculated for both present and ENDF/B-VII.0 parameters<br />

within the energy region of 0.5 to 20 MeV. The present results are compared with other evaluated values<br />

of ENDF/B-VII.0 and JENDL 4.0.<br />

PR 53<br />

Neutron Yields from the Thick Targets Bombarded with Deuterons Above 20 MeV<br />

Changlin Lan, School of Nuclear Science and Technology, Lanzhou University, Lanzhou 730000, China.<br />

Tao Ye, Institute of Applied Physics and Computational Mathematics, Beijing 100094, China. Yukinobu<br />

Watanabe, Department of Advanced Energy Engineering Science, Kyushu University, Kasuga, Fukuoka<br />

816-8580, Japan. Weili Sun, Institute of Applied Physics and Computational Mathematics, Beijing<br />

100094, China. Kazuyuki Ogata, Research Center of Nuclear Physics (RCNP), Osaka University, Ibaraki<br />

567-0047, Japan.<br />

The reliable thick target neutron yields (TTNYs) data of the deuteron incident nuclear reactions are<br />

important for various applications, especially for the deuteron-energy range of 20-40 MeV, which will be<br />

used in the safety design of the IFMIF. From the literatures, the data on these subjects have been measured<br />

and simulated by some laboratories in the past years. But the data are still scarce such as the outgoing<br />

neutron angles and the kinds of target materials. Meanwhile, there are discrepancies between the measured<br />

and calculated results which used the Monte Carlo code directly. To improve the understanding of the<br />

experimental data, a hybrid method is proposed to estimate the TTNYs bombarded with deuterons above<br />

20 MeV, by including the nuclear models for deuteron breakup reactions. To estimate completely the thick<br />

target yield of deuteron induced reaction, it is necessary to incorporate the theoretical studies between<br />

the nuclear models and the particle transportation methods. At first, a model calculation is employed<br />

to produce the data file, which analyzes the nucleon production from deuteron breakup reaction by the<br />

continuum discretized coupled-channels method and the Glauber model. Next, we simulate the deuteron<br />

and neutron transport processes in the thick samples, and give the output neutron flux.<br />

PR 54<br />

Transmission and Capture Yield Calculations in the Nuclear Data Evaluation Code Conrad<br />

O. Litaize, P. Archier, CEA, DEN, DER, Physics Studies <strong>Laboratory</strong>, F-13108 Saint-Paul-lez-Durance,<br />

France. B. Becker, P. Schillebeeckx, EC-JRC-IRMM, Retieseweg 111, B-2440 Geel, Belgium.<br />

This paper deals with the verification and validation of the nuclear reaction models developed in the Conrad<br />

code [1] for the modelling of the neutron induced reactions in the Resolved Resonance energy Range (RRR).<br />

First, this work demonstrates the capability of CONRAD code to calculate cross sections compared with<br />

NJOY [2] code (release 99-259). For both Multi-Level-Breit-Wigner and Reich-Moore approximations of<br />

the R-Matrix theory the average discrepancies between the two codes is lower than 0.003% if the precision<br />

290

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