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Nuclear Energy Conference & Expo (NECX)
September 8–11, 2025
Atlanta, GA|Atlanta Marriott Marquis
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Remembering ANS member Gil Brown
Brown
The nuclear community is mourning the loss of Gilbert Brown, who passed away on July 11 at the age of 77 following a battle with cancer.
Brown, an American Nuclear Society Fellow and an ANS member for nearly 50 years, joined the faculty at Lowell Technological Institute—now the University of Massachusetts–Lowell—in 1973 and remained there for the rest of his career. He eventually became director of the UMass Lowell nuclear engineering program. After his retirement, he remained an emeritus professor at the university.
Sukesh Aghara, chair of the Nuclear Engineering Department Heads Organization, noted in an email to NEDHO members and others that “Gil was a relentless advocate for nuclear energy and a deeply respected member of our professional community. He was also a kind and generous friend—and one of the reasons I ended up at UMass Lowell. He served the university with great dedication. . . . Within NEDHO, Gil was a steady presence and served for many years as our treasurer. His contributions to nuclear engineering education and to this community will be dearly missed.”
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.