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
JAEA-Conf 2011-002 - 日本原子力研究開発機構
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<strong>JAEA</strong>-<strong>Conf</strong> <strong>2011</strong>-<strong>002</strong><br />
19. Measurement of Resonance Parameters of 155,156,157,158,160 Gd by using pulsed<br />
neutrons with energy ranges from 10 eV to 1 keV<br />
Yeong-Rok Kang*, Tae-Ik Ro<br />
Department of Physics, Dong-A University, Busan 604-714, Korea<br />
Email: tiro@donga.ac.kr<br />
Guinyun Kim, Manwoo Lee<br />
Department of Physics, Kyungpook National University, Daegu 702-701, Korea<br />
Y. Danon, M.J Rapp, D. Williams<br />
Department of Mechanical, Aerospace, and Nuclear Engineering, Rensselaer Polytechnic Institute<br />
Troy, New York 12180-3590<br />
G. Leinweber, D.P Barry, R.C. Block<br />
Bechtel Marine Propulsion Corporation, Knolls Atomic Power Laboratory<br />
P.O. Box 1072, Schenectady, New York 12301-1072<br />
We explored neutron interactions with Gadolinium isotopes in the energy region from 10 eV to 1 keV<br />
at the electron linear accelerator facility at the Rensselaer Polytechnic Institute (RPI). The neutron capture<br />
measurements were made at a flight path of 25 m with a 16-segment sodium iodide multiplicity detector by<br />
using the time-of-flight technique. Five high-purity gadolinium isotopes ( 155 Gd, 156 Gd, 157 Gd, 158 Gd, and 160 Gd)<br />
and two natural gadolinium samples were used for the neutron capture measurement. Resonance parameters for<br />
155,156,157,158,160<br />
Gd were obtained by using the multilevel R-matrix Bayesian code SAMMY. The samples are<br />
placed in the center of a cylindrical 16-segment thallium activated sodium iodide NaI(Tl) detector. Each NaI(Tl)<br />
piece is pie shaped and optically separated from each other. All of the NaI(Tl) pieces are housed within an<br />
aluminum can with photomultipliers attached to each pie shaped segment. Many new resonances of the<br />
epithermal region are proposed, and other resonances previously identified in the literature have been revised.<br />
The poor match of the ENDF/B-VII.0 parameters to the current data is significant, and substantial improvement<br />
to the understanding of gadolinium cross sections is presented, particularly above 180.4 eV where the ENDF/B-<br />
VII.0 resolved region for 155 Gd ends. As a result, fitting data above 180.4 eV was performed without initial<br />
estimates for resonance locations and widths as a challenging task. Also new fitting result of 157 Gd above<br />
306.4eV of the upper limit of ENDF/B-VII.0 was presented.<br />
1. Introduction<br />
The neutron capture cross-sections of gadolinium (Gd) isotopes are important in the design of reactors, as<br />
well as in nuclear-reaction and astrophysical studies. Since the major portion of the natural Gd capture crosssections<br />
is due to 155 Gd and 157 Gd, an accurate knowledge of the cross-sections for those isotopes is also of<br />
importance to calculate the reactor characteristics when Gd is used as a burnable poison in light water reactors.<br />
The purpose of the present work was to measure the neutron capture cross-sections and to determine resonance<br />
parameters for Gd isotopes that are an improvement over the current gadolinium evaluations. In addition, the<br />
data are important for examining the availability of Gd as a control material for fast reactors. 1<br />
In the region from 1.0 to 300.0 eV, most of the resonances occur in 155 Gd and 157 Gd. In these two isotopes,