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Growth beyond megawatts
Hash Hashemianpresident@ans.org
When talking about growth in the nuclear sector, there can be a somewhat myopic focus on increasing capacity from year to year. Certainly, we all feel a degree of excitement when new projects are announced, and such announcements are undoubtedly a reflection of growth in the field, but it’s important to keep in mind that growth in nuclear has many metrics and takes many forms.
Nuclear growth—beyond megawatts—also takes the form of increasing international engagement. That engagement looks like newcomer countries building their nuclear sectors for the first time. It also looks like countries with established nuclear sectors deepening their connections and collaborations. This is one of the reasons I have been focused throughout my presidency on bringing more international members and organizations into the fold of the American Nuclear Society.
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.