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Conference Spotlight
2026 Annual Conference
May 31–June 3, 2026
Denver, CO|Sheraton Denver
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Latest News
The progress so far: An update on the Reactor Pilot Program
It has been about three months since the Department of Energy named 10 companies for its new Reactor Pilot Program, which maps out how the DOE would meet the goal announced by executive order in May of having three reactors achieve criticality by July 4, 2026.
H. Naik, Meghna Karkera, Vibha Vansola, Santhi Sheela Yeraguntla, Mayur Mehta, S. V. Suryanarayana, R. Makwana, S. C. Sharma
Nuclear Science and Engineering | Volume 199 | Number 9 | September 2025 | Pages 1406-1424
Research Article | doi.org/10.1080/00295639.2025.2455888
Articles are hosted by Taylor and Francis Online.
Fission product cumulative yields within the mass ranges of 83 to 117 and 123 to 153 have been measured in the 4.93- and 8.31-MeV quasi-mono-energetic neutron-induced fission of 238U by using an off-line gamma-ray spectrometric technique. From the cumulative yields, the mass chain yields were obtained by applying charge distribution correction. From the mass yield data, the peak-to-valley (P/V) ratio, the average values of light mass <AL> and heavy mass <AH>, and the average number of neutrons <υ> were obtained. The data from the present work and literature in the 238U(n,f) reaction at various energies were compared with similar data in the 238U(γ,f) reaction. In both the reactions, the mass yield distributions are asymmetric and double humped. The yields of fission products for A = 133 to 134, A = 138 to 140, and A = 143 to 144 and their complementary products are higher than those of other fission products because of the nuclear structure effect. With the increase of excitation energy, the yield of the symmetric product increases, which causes a decrease of the P/V ratio. The <υ> value also increases with excitation energy in a similar way in both the reactions. However, it is surprising to see a different changing trend of <AL> and <AH> values with an increase of excitation energy between the 238U(n,f) and 238U(γ,f) reactions.