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Program - Brookhaven National Laboratory

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Target Characterization of Large Area Minor Actinide Layers for Fast Neutron Induced<br />

Fission Cross Section Experiments at nELBE<br />

T. Kögler, R. Hannaske, R. Massarczyk, Helmholtz-Zentrum Dresden-Rossendorf, Postfach 510 119,<br />

01324 Dresden, Germany, Technische Universität Dresden, Postfach 100 920, 01076 Dresden, Germany.<br />

R. Beyer, Z. Elekes, A.R. Junghans, R. Schwengner, A. Wagner, Helmholtz-Zentrum Dresden-Rossendorf,<br />

Postfach 510 119, 01324 Dresden, Germany. K. Eberhardt, A. Vascon, Johannes Gutenberg Universität<br />

Mainz, 55099 Mainz, Germany.<br />

The development of Accelerator Driven Systems (ADS) requires accurate nuclear data. Especially neutron<br />

induced fission cross sections of Plutonium and minor actinides in part show high uncertainties in the fast<br />

energy range. For 242 Pu current uncertainties are of around 21 %, the target uncertainties in the order of<br />

7 %. Sensitivity studies ([1], [2]) show that the total uncertainty has to be reduced below 5 %, to enable<br />

reliable neutron physical simulations. This challenging task will be performed at the neutron time-offlight<br />

facility of the new German <strong>National</strong> Center for High Power Radiation Sources at HZDR, Dresden.<br />

Improved experimental conditions (low scattering environment) and beam power, paired with the right<br />

spectral shape of the nELBE neutron source will provide excellent conditions to achieve this aim. A parallel<br />

plate ionization chamber with it’s approximately 100 % intrinsic detection efficiency will measure fission<br />

fragments from thin minor actinide layers (areal density: 580 and 220 microgram per centimeter 2 ; total<br />

mass: 200 milligram of 235 U and 75 milligram of 242 Pu). These very homogeneous targets are produced<br />

by the institute of radiochemistry of the University of Mainz. To handle the high specific alpha activity<br />

of the Pu targets, a combination of fast preamplifiers and digital signal processing has been developed to<br />

suppress pile-up effects. It is planned to determine the homogeneity of the minor actinide targets by two<br />

different methods. Due to their high specific activity the number of fissionable Pu atoms per unit area will<br />

be determined by a spatially resolved alpha spectroscopy. The required setup was optimized using Geant<br />

4 simulations. Results of this simulations and first experimental approaches will be presented. For the<br />

uranium targets it is planned to determine the homogeneity in a fission chamber with a collimated neutron<br />

beam at PTB Braunschweig. Physical properties (distance between anodes and cathodes, counting gas<br />

etc.) of the chamber have also been optimized using the Geant 4 framework. The work is embedded in the<br />

TRAKULA project (BMBF 02NUK13A) supported by the Federal Ministry for Education and Research<br />

of Germany.<br />

[1] OECD/NEA, Nuclear Data High Priority Request List, (2011), http://www.nea.fr/html/dbdata/hprl/<br />

[2] Working Party on International Evaluation Co-operation of the NEA Nuclear Science Committee, Uncertainty<br />

and Target Accuracy Assessment for Innovative Systems Using Recent Covariance Data Evaluations,<br />

(2008), http://www.nea.fr/html/science/wpec/volume26/volume26.pdf<br />

PR 69<br />

Monte Carlo Simulation of Prompt Fission Neutron Observables for the Spontaneous<br />

Fission of 236 Pu, 238 Pu,<br />

O. Serot , O. Litaize, C. Manailescu, D. Regnier, CEA, DEN-Cadarache, F-13108<br />

Saint-Paul-lez-Durance, France.<br />

Recently, a Monte Carlo code which simulates the fission fragment deexcitation process has been developed<br />

at CEA-Cadarache. Our aim is to get a tool capable to predict spectra and multiplicities of prompt particles<br />

and to investigate possible correlations between fission observables. One of the main challenges is to define<br />

properly the share of the available excitation energy at scission between the two nascent fission fragments.<br />

In a previous work [1], these excitation energies were treated within a Fermi-gas approximation in aT 2<br />

(where a and T stand for the level density parameter and the nuclear temperature) and a mass dependent<br />

297

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