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Nuclear Energy Conference & Expo (NECX)
September 8–11, 2025
Atlanta, GA|Atlanta Marriott Marquis
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Ho Nieh nominated to the NRC
Nieh
President Trump recently nominated Ho Nieh for the role of commissioner in the Nuclear Regulatory Commission through the remainder of a term that will expire June 30, 2029.
Nieh has been the vice president of regulatory affairs at Southern Nuclear since 2021, though he is currently working as a loaned executive at the Institute of Nuclear Power Operations, where he has been for more than a year.
Nieh’s experience: Nieh started his career at the Knolls Atomic Power Laboratory, where he worked primarily as a nuclear plant engineer and contributed as a civilian instructor in the U.S. Navy’s Nuclear Power Program.
From there, he joined the NRC in 1997 as a project engineer. In more than 19 years of service at the organization, he served in a variety of key leadership roles, including division director of Reactor Projects, division director of Inspection and Regional Support, and director of the Office of Nuclear Reactor Regulation.
Samuel Carmona, Shimon Yiftah
Nuclear Technology | Volume 71 | Number 1 | October 1985 | Pages 289-295
Technical Paper | Material | doi.org/10.13182/NT85-A33727
Articles are hosted by Taylor and Francis Online.
Complete evaluations of the (n,2n) and (n,3n) reaction cross sections were carried out for the stable isotopes of lead and for natural lead, that element being a potential neutron amplifier for fusion blankets. The method of computation used is based on the Segev simple formalism for compound nucleus decay without branching. This method, which was already checked for 204Pb, was used for cross-section computation for all other stable lead isotopes. From these results, evaluated cross sections could be derived for natural lead. The results of the evaluations were in good agreement with experimental data. Small discrepancies with the measured data for 204Pb, 207Pb, and 208Pb at low excitation energies above threshold are overcome through the introduction of an “effective” threshold energy slightly higher than the real one. This single correction is sufficient for matching the shape of the evaluated curves to the measured data over the entire energy range for the second neutron emission.