Program - Brookhaven National Laboratory
Program - Brookhaven National Laboratory
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