Abstract

The prompt γ-ray spectrum of fission fragments is important in understanding the dynamics of the fission process, as well as for nuclear engineering in terms of predicting the γ-ray heating in nuclear reactors. The γ-ray spectrum measured from the fission fragments of the spontaneous fission of 242Pu will be presented here. A fission chamber containing in total 37mg of 242Pu was used as active sample. The γ-quanta were detected with high time- and energy-resolution using LaBr3 and HPGe detectors, respectively, in coincidence with spontaneous fission events detected by the fission chamber. The acquired γ-ray spectra were corrected for the detector response using the spectrum stripping method. About 70 million fission events were detected which results in a very low statistical uncertainty and a wider energy range covered compared to previous measurements. The prompt fission γ-ray spectrum measured with the HPGe detectors shows structures that allow conclusions about the nature of γ-ray transitions in the fission fragments. The average photon multiplicity of 8.2 and the average total energy release by prompt photons per fission event of about 6.8 MeV were determined for both detector types.

Highlights

  • The emission of γ-quanta after nuclear fission plays an important role for the design of future nuclear power plants

  • The γ-quanta were detected with high time- and energy-resolution using LaBr3 and high purity germanium (HPGe) detectors, respectively, in coincidence with spontaneous fission events detected by the fission chamber

  • The prompt fission γ-ray spectrum measured with the HPGe detectors shows structures that allow conclusions about the nature of γ-ray transitions in the fission fragments

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Summary

Introduction

The emission of γ-quanta after nuclear fission plays an important role for the design of future nuclear power plants. In order to create the correlation between fission event and γ-ray emission a gate was set for all charge spectra in a way that the defined FF regions contain channel values greater than their corresponding local minima. This region is depicted here for the first deposit as hatched area. Two different types of detecors were used to measure the photons in coincidence with a detected fission fragment These are named in the following as γ-ray detector.

Separation of prompt- and delayed γ-rays and Slow rise time correction
Isomeric states from FF
Findings
Conclusion
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