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Education, Training & Workforce Development
The Education, Training & Workforce Development Division provides communication among the academic, industrial, and governmental communities through the exchange of views and information on matters related to education, training and workforce development in nuclear and radiological science, engineering, and technology. Industry leaders, education and training professionals, and interested students work together through Society-sponsored meetings and publications, to enrich their professional development, to educate the general public, and to advance nuclear and radiological science and engineering.
Meeting Spotlight
ANS Student Conference 2025
April 3–5, 2025
Albuquerque, NM|The University of New Mexico
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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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Candidates for leadership provide statements: ANS Board of Directors
With the annual ANS election right around the corner, American Nuclear Society members will be going to the polls to vote for a vice president/president-elect, treasurer, and members-at-large for the Board of Directors. In January, Nuclear News published statements from candidates for vice president/president-elect and treasurer. This month, we are featuring statements from each nominee for the Board of Directors.
R. E. Simpson
Nuclear Technology | Volume 3 | Number 8 | August 1967 | Pages 500-506
Technical Paper and Note | doi.org/10.13182/NT67-A27782
Articles are hosted by Taylor and Francis Online.
A study has been made of the response of normal lithium fluoride and that depleted of 6Li when exposed to pure gamma rays and to the mixed neutron-plus-gamma fields of reactors. Results from a study of the glow curves of the two materials after gamma-ray exposure are similar. However, after reactor exposures in a known field of thermal neutrons and gamma rays, significant differences were found in the 200 and 275°C glow peaks for approximately the same integrated area under the curves. Presumably these are principally due to differences in the specific ionization of recoil electrons from gamma rays relative to that of the alpha particles and 3H recoils from the 6Li(n,α)3H reaction. By using thermal-neutron shields of 6Li or cadmium, the pure gamma dose can be obtained from the usual gamma-ray glow curves from either material. The response (integrated light output) of the depleted LiF per 1010 n/cm2(th) equals that caused by 0.7 rad of 60Co gamma rays, while the corresponding response of the normal phosphor exceeds that from 200 rad of gamma rays. Having determined the response of these materials to thermal neutrons, and considering the relative independence of the response (per rad) upon gamma-ray energy, one may use the depleted phosphor to determine gamma-ray dose within a reactor environment and the normal material as an auxiliary thermal-neutron-plus-gamma-ray detector.