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Accelerator Applications
The division was organized to promote the advancement of knowledge of the use of particle accelerator technologies for nuclear and other applications. It focuses on production of neutrons and other particles, utilization of these particles for scientific or industrial purposes, such as the production or destruction of radionuclides significant to energy, medicine, defense or other endeavors, as well as imaging and diagnostics.
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ANS Student Conference 2025
April 3–5, 2025
Albuquerque, NM|The University of New Mexico
Standards Program
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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Latest News
First astatine-labeled compound shipped in the U.S.
The Department of Energy’s National Isotope Development Center (NIDC) on March 31 announced the successful long-distance shipment in the United States of a biologically active compound labeled with the medical radioisotope astatine-211 (At-211). Because previous shipments have included only the “bare” isotope, the NIDC has described the development as “unleashing medical innovation.”
A. L. Kaplan
Nuclear Science and Engineering | Volume 27 | Number 2 | February 1967 | Pages 388-393
Technical Paper | doi.org/10.13182/NSE67-A18277
Articles are hosted by Taylor and Francis Online.
Attenuation by a floor barrier of fallout gamma radiation scattered into a basement has been studied experimentally with cylindrical steel structures. These structures were 2-ft high, 2-ft in diameter, with a 4-ft-deep basement. Wall thicknesses varied between 5 and 60 psf, with floor thicknesses of 0, 10, 20, and 40 psf. Detectors in the basement were located between 0.25 and 3 ft below ground. Cobalt-60 point sources were used to simulate the fallout field. Basement reduction factors predicted by structure shielding theory were lower than the experimental results by a factor of between 1.5 and 8. This discrepancy was attributed to the theoretical floor-barrier reduction factor. A new theoretical floor-barrier reduction factor, which is a function of both the floor thickness and the solid-angle fraction subtended at the detector by the floor, was constructed within the formalism of the existing structure shielding theory. This new function agreed quite well with both experimental results and Monte Carlo calculations, over the entire range of wall and floor thicknesses used in the experiment.