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Conference Spotlight
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.
C. H. Reed, C. N. Henry, A. A. Usner
Nuclear Science and Engineering | Volume 30 | Number 3 | December 1967 | Pages 362-373
Technical Paper | doi.org/10.13182/NSE67-A18399
Articles are hosted by Taylor and Francis Online.
Asymptotic decay constants for pulse-induced “thermalized” neutron fields have been measured for graphite cubical assemblies having geometric bucklings varying from 9.30 × 10–4 cm–2 to 13.44 × 10–3 cm–2. A value of 700 μ sec was observed to be a sufficient time after the neutron pulse to identify and evaluate fundamental-mode decay in the smallest system included in the above interval of buckling. Values of the infinite-medium neutron lifetime –1 “Fick’slaw” diffusion coefficient D0, as well as the so-called “diffusion-cooling” coefficient C, were obtained from least-squares fits to the experimental α/ρ vs B2/ρ2 data and are mutually consistent and stable over a large interval of B2 and in good agreement with theory. The existence of a well-defined negative FB6 term has been verified. An “effective” higher-mode decay of (3570 ± 80)sec–1, independent of system buckling, was obtained and is consistent with the concept of a continuum lying above a critical limit for fundamental-mode decay. An apparent critical limit (v ∑ t)min has been identified in the interval 2392 sec–1 < (v ∑ t)min < 2648 sec–1 which corresponds to the interval of buckling 13.44 × 10–3 cm–2 to 16.53 × 10–3 cm–2.