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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. Takahashi
Nuclear Science and Engineering | Volume 87 | Number 4 | August 1984 | Pages 432-443
Technical Paper | doi.org/10.13182/NSE84-A18509
Articles are hosted by Taylor and Francis Online.
A high-energy fission model is incorporated into the nucleon-meson transport code, NMTC, which has been used for predicting high-energy neutron yields from high-energy nucleon and pion collisions with nuclei. The experiments of Vasil'kov et al., Russel et al., and Fraser et al. to measure fissile material production rates from fertile material and to determine neutron production rates, are analyzed. Evaluations are made of the plutonium production rate from the infinite medium uranium block. The calculation including the high-energy fission process gives a more reasonable agreement with the experiments, than the process without high-energy fission. A possible refinement of the model, taking into account the rotational motion in the excited state, is discussed.