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Radiation Protection & Shielding
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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Conference on Nuclear Training and Education: A Biennial International Forum (CONTE 2025)
February 3–6, 2025
Amelia Island, FL|Omni Amelia Island Resort
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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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Christmas Night
Twas the night before Christmas when all through the houseNo electrons were flowing through even my mouse.
All devices were plugged in by the chimney with careWith the hope that St. Nikola Tesla would share.
J.J. Ramirez, K.R. Prestwich, R.W. Stinnett, D.L. Johnson, C.L. Olson, G.O. Allshouse, M.J. Clauser, V.Harper-Slaboszewicz, T.W.L. Sanford, J.D. Boyes, T.A. Mehlhorn, L.J. Lorence, D.L. Hanson, M.E. Cuneo Sandia, R.R. Peterson, R.L. Engelstad, J.W. Powers, H.Y. Khater, M.E. Sawan, E.G. Lovell, G.A. Moses
Fusion Science and Technology | Volume 19 | Number 3 | May 1991 | Pages 664-668
Inertial Fusion | doi.org/10.13182/FST91-A29420
Articles are hosted by Taylor and Francis Online.
The Laboratory Microfusion Facility (LMF) is being planned to develop high-gain, high-yield (200 MJ-1000 MJ) ICF targets for applications to nuclear weapons effects simulation, thermonuclear weapons physics, and energy production. It is expected that a 1000-MJ yield will require ∼ 10–20 MJ input energy to the target. The light-ion beam driver concept for the LMF consists of 36 accelerator modules that drive independent Li+ ion diodes. Each ion beam is extracted from an annular ion diode and propagated to a solenoidal lens located near the wall of the target chamber. This magnetic lens focuses the beam on to the pellet located at the center of the target chamber. The temporal shape of the power pulse delivered to the target is controlled by the synchronized firing of the accelerator modules. This paper presents a status of the light-ion beam LMF driver concept.