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2025 ANS Winter Conference & Expo
November 8–12, 2025
Washington, DC|Washington Hilton
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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. S. Booth, R. H. Hartley, R. B. Perez
Nuclear Science and Engineering | Volume 28 | Number 3 | June 1967 | Pages 404-414
Technical Paper | doi.org/10.13182/NSE67-A28955
Articles are hosted by Taylor and Francis Online.
A technique is presented for conducting neutron-wave experiments in thermal-neutron systems using either a sinusoidally modulated or a pulsed source of thermal neutrons. A neutron source suitable for this experiment is described, data-accumulation criteria are presented, and the electrical systems used for collection are discussed. A specific experiment with graphite is reported and the discussion of data analysis is carried through the experimental determination of this system's dispersion law. It is found that, in general, a pulsed source of thermal neutrons is more suitable for neutron-wave experimentation than a sinusoidally modulated source. Confirmation is given to the theoretical prediction that diffusion and thermalization parameters can be measured by this technique over a relatively wide range of frequency without significant higher space- and energy-mode contamination. The values we obtained for the diffusion and thermalization parameters for graphite of density 1.60 g/cm3 were α0 ± 91. ± 1 sec−1, D0 = (2.16 ± 0.01) × 105 (cm2 sec−1), C0 = (39. ± 2) × 105 (cm4 sec−1), and F0 = (12. ± 2) × 107 (cm6 sec−1).