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Westinghouse, Nordion, and PSEG team up to produce Co‑60 in the United States
This past January, Westinghouse Electric Company, Nordion, and PSEG Nuclear formalized agreements to implement newly developed cobalt-60 production technology at Units 1 and 2 of PSEG’s Salem nuclear power plant in New Jersey, with the Co-60 to be supplied to Nordion. Through an ongoing joint initiative, the companies aim to harness U.S. pressurized water reactors to produce a key medical isotope and build the first commercial-scale Co-60 production platform in the United States.
L. E. Beghian, N. C. Rasmussen, R. Thews, J. Weber
Nuclear Science and Engineering | Volume 15 | Number 4 | April 1963 | Pages 375-381
Technical Paper | doi.org/10.13182/NSE63-A26453
Articles are hosted by Taylor and Francis Online.
Nanosecond bursts of monoenergetic neutrons in the range 0.8–1.6 Mev are injected into non-moderating assemblies of bismuth, lead, and natural uranium. The flux in these assmblies is observed to decay exponentially with characteristic nanosecond time constants in good agree-ment with one velocity transport theory, and the known inelastic scattering and absorption cross sections.These experiments serve as a check on the validity of the assumptions of transport theory. The technique also serves as a method for measuring macroscopic inelastic and absorption cross sections directly, without the necessity of making the corrections required in other methods e.g., for double scattering and for the angular distribution.Nanosecond bursts of monoenergetic neutrons in the range 0.8–1.6 Mev are injected into non-moderating assemblies of bismuth, lead, and natural uranium. The flux in these assmblies is observed to decay exponentially with characteristic nanosecond time constants in good agree-ment with one velocity transport theory, and the known inelastic scattering and absorption cross sections.These experiments serve as a check on the validity of the assumptions of transport theory. The technique also serves as a method for measuring macroscopic inelastic and absorption cross sections directly, without the necessity of making the corrections required in other methods e.g., for double scattering and for the angular distribution.