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2025 ANS Winter Conference & Expo
November 9–12, 2025
Washington, DC|Washington Hilton
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Researchers use one-of-a-kind expertise and capabilities to test fuels of tomorrow
At the Idaho National Laboratory Hot Fuel Examination Facility, containment box operator Jake Maupin moves a manipulator arm into position around a pencil-thin nuclear fuel rod. He is preparing for a procedure that he and his colleagues have practiced repeatedly in anticipation of this moment in the hot cell.
O. Auciello, A. A. Haasz, P. C. Stangeby
Fusion Science and Technology | Volume 6 | Number 2 | September 1984 | Pages 411-413
Technical Paper | Selected papers from the Ninth International Vacuum Congress and the Fifth International Conference on Solid Surfaces (Madrid, Spain, September 26-October 1, 1983) | doi.org/10.13182/FST84-A23214
Articles are hosted by Taylor and Francis Online.
Methane production yields due to sub-eV H° impact on carbon are in the 10−3 – 10−4 CH4/H° range, i.e., about two orders of magnitude less than CH4/H+ yields for 0.1 – 100 keV H+ ions. Two macroscopic states of “reactivity” were identified for carbon: an “activated” state characterized by a CH4 yield vs. sample temperature curve with a maximum at 700–850K, and a “deactivated” state characterized by a monotonically decreasing yield as a function of temperature. Regarding the retention of sub-eV H° and D° in carbon, our results differ from previously published results. We have observed lower levels of trapped H° (∼1015 H°/cm2), with an apparent trend for saturation, at incident fluences of >2×1019 H°/cm2. Strong synergistic effects have been reported for combined sub-eV H°/5 keV Ar+ impact, while it appears that “insignificant” synergism exists for combined sub-eV H°/e− impact.