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August 24–27, 2026
Dallas, TX|Hilton Anatole
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Breaking ground on a new approach to construction
The drive to Kairos Power’s reactor demonstration site in Oak Ridge, Tenn., is not only scenic—it’s historic. Nearly 85 years ago, roughly 30,000 construction workers transformed orchards and farmland into a key Manhattan Project site. Depending on your route, you may pass by one of the three gatehouses that were once military checkpoints controlling access to Atomic Energy Commission production facilities.
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.