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Nuclear Nonproliferation Policy
The mission of the Nuclear Nonproliferation Policy Division (NNPD) is to promote the peaceful use of nuclear technology while simultaneously preventing the diversion and misuse of nuclear material and technology through appropriate safeguards and security, and promotion of nuclear nonproliferation policies. To achieve this mission, the objectives of the NNPD are to: Promote policy that discourages the proliferation of nuclear technology and material to inappropriate entities. Provide information to ANS members, the technical community at large, opinion leaders, and decision makers to improve their understanding of nuclear nonproliferation issues. Become a recognized technical resource on nuclear nonproliferation, safeguards, and security issues. Serve as the integration and coordination body for nuclear nonproliferation activities for the ANS. Work cooperatively with other ANS divisions to achieve these objective nonproliferation policies.
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2024 ANS Winter Conference and Expo
November 17–21, 2024
Orlando, FL|Renaissance Orlando at SeaWorld
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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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New laws offer nuclear industry incentives for existing power plant uprates
This year, the U.S. nuclear industry received a much-needed economic boost that could help preserve operating nuclear power plants and incentivize upgrades that extend their lifespan and power output.
Signed into law in 2022, the Inflation Reduction Act offers production tax credits (PTCs) for existing nuclear power plants and either PTCs or investment tax credits (ITCs) for new carbon-free generation. These credits could make power uprates—increasing the maximum power level at which a commercial plant may operate—a much more appealing option for utilities.
Janet S. Merritt, J. G. V. Taylor, A. W. Boyd
Nuclear Science and Engineering | Volume 28 | Number 2 | May 1967 | Pages 286-292
Technical Paper | doi.org/10.13182/NSE67-A17479
Articles are hosted by Taylor and Francis Online.
The 2200 m/sec neutron cross section for deuterium has been determined relative to that for 59Co by absolute counting of the 3H and 80Co produced by neutron irradiation. The result, expressed in terms of the 2200 m/sec cross section for 59Co in b, and of the tritium half-life in years, is (1.104 ± 0.014 × 10-3) [σ0(59Co)] [t1/2(3H)] mb. Assuming σ0(59Co) = 37.4 ± 0.3 b and t1/2(3H) = 12.262 ± 0.004 years, gives σ0 (D) = 0.506 ± 0.010 mb. The standard deviation of the mean value from 8 irradiations was ± 0.2%.
