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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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ANS Student Conference 2025
April 3–5, 2025
Albuquerque, NM|The University of New Mexico
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Latest News
First astatine-labeled compound shipped in the U.S.
The Department of Energy’s National Isotope Development Center (NIDC) on March 31 announced the successful long-distance shipment in the United States of a biologically active compound labeled with the medical radioisotope astatine-211 (At-211). Because previous shipments have included only the “bare” isotope, the NIDC has described the development as “unleashing medical innovation.”
V. J. Orphan, C. G. Hoot, Joseph John
Nuclear Science and Engineering | Volume 42 | Number 3 | December 1970 | Pages 352-366
Technical Paper | doi.org/10.13182/NSE70-A21223
Articles are hosted by Taylor and Francis Online.
Gamma-ray production cross sections were measured for the 16O(n, xγ) reaction from 6.35- to 16.52-MeV neutron energy. The Gulf General Atomic LINAC was used to produce a pulsed source of neutrons having a continuous distribution of neutron energies. A 30-cm3 Ge(Li) detector, placed at 125 deg to the incident neutron beam, was used to measure the γ-ray spectra. The corresponding neutron energy was determined by the time-of-flight technique. The two-parameter data (γ-ray energy, neutron energy) were processed with an on-line computer and sorted into 10 γ-ray spectra spanning the range 6.35 MeV ≤ En ≤ 16.52 MeV. From these data we obtained average differential gamma-ray production cross sections for 9 gamma rays from the 16O(n, xγ) reaction. The cross sections are in good agreement with other recent measurements, but show rather large disagreement with some earlier measurements. The total nonelastic cross section obtained by summing the partial cross sections is consistent with the nonelastic cross section obtained from the difference between the total cross section and the total elastic cross section for En < H MeV. However, in the range 11 MeV ≤ En ≤ 16.5 MeV, there is a serious discrepancy for which a possible explanation is discussed.