Abstract

The study of fission yields has a major impact on the characterization and understanding of the fission process and is mandatory for reactor applications. The mass and isotopic yields of the fission fragments have a direct influence on the amount of neutron poisons that limit the fuel burnup and on the evaluation of the residual power of the reactor after shutdown. The fission yields of the plutonium nuclides are also mandatory for the studies on the fuel multi-recycling. In order to significantly improve the precision of nuclear data, more and more fundamental fission models are used in the evaluation processing. Therefore, tests of fission models become a central issue to achieve a coherent libraries of nuclear data. In this framework, an important investigation in the experimental limits of facilities is required to provide complete sets of data with their coherent variance-covariance matrices. In the past with the LOHENGRIN spectrometer of the ILL, priority has been given for the studies in the light fission fragment mass range. The LPSC in collaboration with ILL and CEA has developed a measurement program on symmetric and heavy mass fission fragment distributions. The combination of measurements with ionisation chamber and Ge detectors is necessary to describe precisely the heavy fission fragment region in mass and charge. Recently, new measurements of fission yields and kinetic energy distributions, with different fissioning systems, were performed with this facility. The focus has been done on the selfnormalization of the data to provide new absolute measurements, independently of any libraries, and the experimental covariance matrix. To reach precise measurements, a new experimental procedure was developed along with a new analysis method based on metadata. Because of the complex correction scheme from count rates to yields, a classical propagation uncertainty is not possible. The new analysis path gives the mean value of mass yields, its probability density function and the associated experimental variance-covariance matrices. All this information is a first step to bring nuclear data into statistical tests of the underlying hypothesis of fission models.

Highlights

  • Recent measurements from [1,2,3] of 233U fission yields in the heavy region with the Lohengrin spectrometer showed an important discrepancy near the symmetry region in comparison with the evaluations

  • Fission fragments emerge from the target with an ionic charge distributed around an average ionic charge of about 21

  • Measurements of fission yields with the Lohengrin spectrometer are in principle simple

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Summary

Experimental setup

The accurate knowledge of fission data in the actinide region is important for studies of innovative nuclear reactor concepts. Fission yield measurements supply experimental data to put constraints on fission models and improve their predictive power In this context, since 2007, various experiments from our collaboration have been performed to investigate fission yields at the Lohengrin spectrometer of the ILL with a special focus on the heavy and symmetry mass region, where there are inconsistencies between models (or evaluations) and the few experimental data. The Lohengrin mass spectrometer [4] is a nuclear physics instrument of the ILL research reactor facility which allows the study of fragment distributions from thermal neutron induced fission with a very good resolution. Fission fragments emerge from the target with an ionic charge distributed around an average ionic charge of about 21 Those fragments are emitted along the beam tube axis undergo a horizontal deflection in a magnetic field, directly followed by a vertical deflection in an electric field.

Relative and absolute experimental mass yields
Contamination highlighting
Analysis method for the contamination correction
Experimental fission yields covariance
Experimental mass yield covariance
Pure experimental evaluation and covariance
Findings
Conclusion and perspectives
Full Text
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