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Conference Spotlight
2025 ANS Winter Conference & Expo
November 8–12, 2025
Washington, DC|Washington Hilton
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The Standards Committee is responsible for the development and maintenance of voluntary consensus standards that address the design, analysis, and operation of components, systems, and facilities related to the application of nuclear science and technology. Find out What’s New, check out the Standards Store, or Get Involved today!
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Japan gets new U for enrichment as global power and fuel plans grow
President Trump is in Japan today, with a visit with new Prime Minister Sanae Takaichi on the agenda. Takaichi, who took office just last week as Japan’s first female prime minister, has already spoken in favor of nuclear energy and of accelerating the restart of Japan’s long-shuttered power reactors, as Reuters and others have reported. Much of the uranium to power those reactors will be enriched at Japan’s lone enrichment facility—part of Japan Nuclear Fuel Ltd.’s Rokkasho fuel complex—which accepted its first delivery of fresh uranium hexafluoride (UF₆) in 11 years earlier this month.
R. D. Werner, T. A. Eastwood
Nuclear Science and Engineering | Volume 21 | Number 1 | January 1965 | Pages 20-25
Technical Paper | doi.org/10.13182/NSE65-A21010
Articles are hosted by Taylor and Francis Online.
The thermal neutron-capture cross section of 1.0-year Ru106 has been determined from the yield of 22-min Rh107 formed in reactor irradiations. The average of four measurements is 0.146 barns. The experimental error is about ±7% but when systematic errors are included, largely in gamma-ray abundances from Ru106 and Rh107 decay, the uncertainty is about 30%. Cadmium-ratio measurements were made and the resonance-capture integral, including the 1/υ part, was found to be 2.0 ± 0.6 barns for an effective cadmium cutoff of 0.54 eV. These results are relative to a cobalt thermal neutron-capture cross section of 37.5 barns and total resonance integral of 72.7 barns. It has been assumed that neutron capture by Rh106, Ru107 and Rh107 is negligible, that the cross section of Ru106 in the thermal region has a 1/υ dependence and that the neutron spectrum is 1/E in the resonance region.