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Why should safeguards by design be a global effort?
Jeremy Whitlock
I can’t think of a more exciting time to be working in nuclear, with the diversity of advanced reactor development and increasing global support for nuclear in sustainable energy planning. But we can’t lose sight of the need to plan for efficient international safeguards at the same time.
Global nuclear deployment has been underpinned since 1970 by the Treaty on the Non-Proliferation of Nuclear Weapons (NPT), making it a key customer requirement for governments to demonstrate unequivocally that the technology is not being misused for weapons development.
The International Atomic Energy Agency (IAEA) has helped verify this commitment for more than 50 years, but it has never safeguarded many of the advanced reactors (and related fuel cycle processes) being developed today.
A. Borella, K. Volev, A. Brusegan, P. Schillebeeckx, F. Corvi, N. Koyumdjieva, N. Janeva, A. A. Lukyanov
Nuclear Science and Engineering | Volume 152 | Number 1 | January 2006 | Pages 1-14
Technical Paper | doi.org/10.13182/NSE06-A2557
Articles are hosted by Taylor and Francis Online.
The neutron capture cross section of thorium has been measured in the energy region between 4 and 140 keV at the GELINA time-of-flight facility of the Institute for Reference Materials and Measurements in Geel, Belgium. The gamma rays from capture events were detected by two C6D6 liquid scintillators, placed 14.37 m from the neutron source. The shape of the neutron flux was measured with a 10B-loaded ionization chamber. To obtain a detection efficiency independent of the gamma cascade and proportional to the total excitation energy, the pulse-height weighting technique was applied. The data have been normalized to the well-isolated and almost saturated 232Th resonance at 23.5 eV. The systematic uncertainties related to the normalization and weighting function, using an internal saturated resonance, are ~1.5%. An additional systematic uncertainty of 0.5% results from the self-shielding and multiple scattering corrections.Between 4 and 140 keV, our data are ~9 and 6.5% higher than the data of Kobayashi et al. and Macklin et al., respectively, and in good agreement with the data of Poenitz and Smith. Below 15 keV our data deviate by up to 30% from the data reported by Wisshak et al. Our data have been analyzed in terms of average level parameters. The resulting parameters are consistent with the resolved resonance parameters deduced from the transmission measurements of Olsen et al.