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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.
M. S. Ash, G. Yanow
Nuclear Science and Engineering | Volume 55 | Number 3 | November 1974 | Pages 342-344
Technical Note | doi.org/10.13182/NSE74-A23460
Articles are hosted by Taylor and Francis Online.
In certain atomic physics experiments performed in conjunction with underground nuclear-weapon testing, it is desired that radiation energy converter plates be irradiated so as to reemit a maximum amount of radiation. The plates, composed of thin layers of materials of differing atomic number, are to be designed by choosing the material atomic number for each layer so that the plate, in toto, produces minimum photoelectron kinetic energy. Minimum photoelectron kinetic energy implies maximum energy reradiated, in the context of the radiation energy spectral regime of interest. The optimum choice of layer atomic numbers involves the solution of a novel variational problem where the minimizing function, the atomic numbers, take on integer values only. A comparison is made between the optimally designed plate and the corresponding homogeneous plate in terms of photoelectron kinetic energy produced. The homogeneous plate produces more than two orders of magnitude more photoelectric kinetic energy than does the optimally designed plate.