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Program - Brookhaven National Laboratory

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Community’s 7th Framework <strong>Program</strong>me in the ANDES project under grant agreement No. 249671. It<br />

has also been partially funded by the specific collaborative agreement between CIEMAT and UNED/UPM<br />

in the area of ”High level waste transmutation”.<br />

DE 3 4:20 PM<br />

Measurement of Gamma Energy Distributions and Multiplicities Using STEFF<br />

E. Murray, A. G. Smith, A. J. Pollitt<br />

Department of Physics and Astronomy, University of Manchester, M13 9PL, Manchester, UK<br />

J. Matarranz, I. Tsekhanovich<br />

Université de Bordeaux/CENBG, 33175 Gradignan Cedex, France<br />

T. Soldner, U. Koster<br />

Insitut Laue-Langevin, 6 rue J. Horowitz, 38012 Grenoble, France<br />

D.C Biswas<br />

Bhabha Atomic Research Centre, Trombay, 400085, Mumbai, India<br />

Prompt gamma ray energy distributions and multiplicities released during thermally induced fission of<br />

235 U are measured using STEFF (SpecTrometer for Exotic Fission Fragments). Thermal neutrons are<br />

provided by the high-flux reactor at the ILL, Grenoble. STEFF is a unique 2E2v device that uses a<br />

coincidence timing method to measure the emission of prompt gamma rays as a function of the fragment<br />

mass and energy. Following scission, the fission fragments contain excitation energy that is released via<br />

prompt neutron and gamma ray emission as the fragment decays to its ground state. STEFF contains<br />

an array of 11 NaI detectors around the uranium target providing a 6.8% photopeak detection efficiency<br />

for acceptance of gamma rays released within 1ns of the scission time. STEFF also consists of 7 NE213<br />

detectors, which detect the emission of prompt neutrons, the release of which is associated with reduction<br />

of fragment energy and, to a lesser extent, fragment spin. Using STEFF, the gamma ray energies and<br />

multiplicity have been measured as a function of mass, with a mass resolution of 4% and a gamma-ray<br />

energy range up to 8 MeV. This experiment acts as a direct response to the NEA high priority demand<br />

which requires more accurate knowledge of heating caused by gamma emission in the next generation of<br />

nuclear reactors.<br />

DE 4 4:40 PM<br />

Gamma Heat Rate Evaluation for Material Irradiation Test in The Experimental Fast<br />

Reactor Joyo<br />

S. Maeda, H. Naito, T. Soga, C. Ito, T. Aoyama<br />

Japan Atomic Energy Agency<br />

One of the primary missions of the experimental fast reactor Joyo is to perform irradiation tests of fuel<br />

and materials to support development of fast reactors. In a material irradiation test, it is essential to give<br />

a precise characterization of the irradiation field, considering not only neutron fluence and displacements<br />

per atom (dpa) but also temperature. The main heat source in a material irradiation test is the gamma<br />

heating of surrounding materials, such as stainless steels constituting the irradiation rig including the<br />

irradiation specimen and capsule. Accurate core and temperature calculation methods are required for<br />

predicting the gamma heat rate and other key performance parameters for irradiation tests in Joyo. In<br />

order to evaluate the gamma heating spatial distribution in fast reactors, it was needed to consider whole<br />

components of gamma intensity. However, delayed gamma ray yield data of all actinides are not prepared<br />

70

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