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Center for Used Fuel Research: Building confidence in storage and transport
Used nuclear fuel storage and transportation have reached a critical juncture.
Dozens of utilities need reliable data on how used nuclear fuel performs in dry storage casks and canisters to extend regulatory licenses at sites across the United States. Likewise, the Department of Energy expects to take ownership of the used nuclear fuel—termed “spent nuclear fuel” in the laws and regulations governing its stewardship—and transfer it to one or more federal staging facilities for management and disposition.
Meanwhile, dozens of reactor companies are testing prototypes of advanced reactors and advanced reactor fuels. Eventually, regulators and industry must also verify the safety and security of storage methods for these advanced fuel types.
To help address these challenges, the DOE established the Center for Used Fuel Research (CUFR) in January 2026 for work related to the long-term storage and transport of used nuclear fuel.
Xiangpeng Meng, Yuanyuan Liu, Bin Wu, Jianping Cheng, Li Wang, Yu Wang, Ning Su
Nuclear Technology | Volume 208 | Number 4 | April 2022 | Pages 753-760
Technical Note | doi.org/10.1080/00295450.2021.1945358
Articles are hosted by Taylor and Francis Online.
Detecting the activity of 210Pb in the human skull by counting its 46.5-keV gamma rays in vivo is a promising method to reconstruct one’s cumulative radon intake, based on which associated lung cancer risk can be evaluated. However, this technique is strongly challenged by the background radiation level, which can be largely categorized as room background and subject background. In this work, we quantitatively assess the performance of the phoswich detector in suppressing background radiation resulting from 40K ubiquitously present in human subjects under in vivo measurements using Monte Carlo simulations. We first determined the region of interest for 210Pb gamma-ray detection to be 31 to 61 keV and focused on the background level inside this region caused by two 40K decay processes. It is found that the 1.46-MeV gamma-ray–led background can be reduced by 40% by the phoswich detector operating in anticoincidence mode whereas the 1.31-MeV beta-particle–led background is almost unaffected. This observation is understood through the dependence of the anticoincidence efficiency on the incident gamma-ray energies. Our results suggest that the 1.31-MeV beta-particle–led background is much larger and harder to suppress than the 1.46-MeV gamma-ray–led background, and they call for more investigations in the background reduction techniques for 210Pb in vivo measurement.