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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
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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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Latest News
Moltex demonstrates its WATSS fuel recycling process
Advanced reactor company Moltex Energy Canada said it has successfully validated its waste to stable salt (WATSS) process on used nuclear fuel bundles from an unnamed Canadian commercial reactor through hot cell experiments conducted by Canadian Nuclear Laboratories.
Eric Hellstrand, Jakob Weitman
Nuclear Science and Engineering | Volume 9 | Number 4 | April 1961 | Pages 507-518
Technical Paper | doi.org/10.13182/NSE61-A25915
Articles are hosted by Taylor and Francis Online.
The resonance integral for thorium metal rods of different diameters has been determined by the activation method. The irradiations took place in the central channel of the reactor R1, where the energy dependence of the neutron flux had earlier been investigated with a fast chopper up to several kev. The absolute calibration was made with gold as a standard. The true resonance integral for gold was taken from the literature as 1500 ± 35 b. The experimental values for thorium were fitted to two alternative expressions with the following results: The measurements were made for S/M values in the range 0.14–0.87 cm2/g. The main contribution to the margin of error arises from the uncertainties in the cross sections used and in the correction for the departure of the neutron energy distribution from the 1/E form.