ANS is committed to advancing, fostering, and promoting the development and application of nuclear sciences and technologies to benefit society.
Explore the many uses for nuclear science and its impact on energy, the environment, healthcare, food, and more.
Explore membership for yourself or for your organization.
Conference Spotlight
2026 ANS Annual Conference
May 31–June 3, 2026
Denver, CO|Sheraton Denver
Latest Magazine Issues
Jan 2026
Jul 2025
Latest Journal Issues
Nuclear Science and Engineering
January 2026
Nuclear Technology
December 2025
Fusion Science and Technology
November 2025
Latest News
From Capitol Hill: Nuclear is back, critical for America’s energy future
The U.S. House Energy and Commerce Subcommittee on Energy convened its first hearing of the year, “American Energy Dominance: Dawn of the New Nuclear Era,” on January 7, where lawmakers and industry leaders discussed how nuclear energy can help meet surging electricity demand driven by artificial intelligence, data centers, advanced manufacturing, and national security needs.
John D. Sheliak, James K. Hoffer
Fusion Science and Technology | Volume 35 | Number 2 | March 1999 | Pages 234-243
Technical Paper | doi.org/10.13182/FST99-A11963930
Articles are hosted by Taylor and Francis Online.
Solid D-T layers are equilibrated inside a 2 mm diameter beryllium toroidal cell at temperatures ranging from 19.0 K to 19.6 K, using the beta-layering process. Each experimental run consisted of multiple cycles of rapid- or slow-freezing of the initially liquid D-T charge. Each of these freeze cycles was followed by a lengthy period of beta-layering equilibration, which was terminated by melting the layer. The temperature was changed in discrete steps at the end of some equilibration cycles in an attempt to simulate actual ICF target conditions. High-precision images of the D-T solid-vapor interface were analyzed to yield the surface roughness σrms as a sum of modal contributions. Results show an average σrms. of 1.3 ± 0.3 μm for layers equilibrated at 19.0 K and show an inverse dependence of σrms on equilibration temperature up to 19.525 K. Inducing sudden temperature perturbations lowered σrms to 1.0 ± 0.05 μm.