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The Radiation Protection and Shielding Division is developing and promoting radiation protection and shielding aspects of nuclear science and technology — including interaction of nuclear radiation with materials and biological systems, instruments and techniques for the measurement of nuclear radiation fields, and radiation shield design and evaluation.
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2025 ANS Annual Conference
June 15–18, 2025
Chicago, IL|Chicago Marriott Downtown
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The Standards Committee is responsible for the development and maintenance of voluntary consensus standards that address the design, analysis, and operation of components, systems, and facilities related to the application of nuclear science and technology. Find out What’s New, check out the Standards Store, or Get Involved today!
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BREAKING NEWS: Trump issues executive orders to overhaul nuclear industry
The Trump administration issued four executive orders today aimed at boosting domestic nuclear deployment ahead of significant growth in projected energy demand in the coming decades.
During a live signing in the Oval Office, President Donald Trump called nuclear “a hot industry,” adding, “It’s a brilliant industry. [But] you’ve got to do it right. It’s become very safe and environmental.”
Maria Do Carmo Lopes, Jorge Molina Avila
Nuclear Science and Engineering | Volume 96 | Number 4 | August 1987 | Pages 303-309
Technical Paper | doi.org/10.13182/NSE87-A16393
Articles are hosted by Taylor and Francis Online.
A simple, physically transparent method is developed to calculate the electric charge per neutron captured in prompt response self-powered neutron detectors (SPNDs), which contributes to the emitter-collector current. This charge is written as the energy integral of the product of two functions: the spectral function S(E), which is the energy spectrum of all electrons resulting from prompt gamma interactions with the atoms of the emitter, and the electron spectral contribution ∈ f(E), which is the probability that an electron released with energy E reaches the collector. The function ∈ f(E) is given an analytical approximate expression derived from an analytical approximation obtained for the path length probability distribution function. The exact expression of ∈ f(E) is also obtained analytically for infinitely long emitters in terms of special functions. The method allowed the creation of an extremely fast algorithm to calculate the effective charge and was applied to cobalt prompt response SPNDs.