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
Feb 2026
Jul 2025
Latest Journal Issues
Nuclear Science and Engineering
March 2026
Nuclear Technology
February 2026
Fusion Science and Technology
January 2026
Latest News
Fusion energy: Progress, partnerships, and the path to deployment
Over the past decade, fusion energy has moved decisively from scientific aspiration toward a credible pathway to a new energy technology. Thanks to long-term federal support, we have significantly advanced our fundamental understanding of plasma physics—the behavior of the superheated gases at the heart of fusion devices. This knowledge will enable the creation and control of fusion fuel under conditions required for future power plants. Our progress is exemplified by breakthroughs at the National Ignition Facility and the Joint European Torus.
W.M. Shu, K. Okuno, Y. Hayashi, S. Ohira, Y. Naruse
Fusion Science and Technology | Volume 21 | Number 3 | May 1992 | Pages 1934-1938
Material and Tritium | doi.org/10.13182/FST92-A30002
Articles are hosted by Taylor and Francis Online.
Ion implantation driven permeation (IDP) behavior on pure molybdenum has been investigated using deuterium ion with low energy (200–2000 eV). The experimental results include measurements of the dependence of the permeation rate at the steady state upon the incident ion flux, temperature and incident ion energy. A good linear relationship was observed between the permeation rate and the incident ion flux. This suggests that the IDP process through pure molybdenum was controlled by diffusion of deuterium in both the front and back regions. The temperature dependence of the permeation rate varies with the incident ion energy. It is caused by the different mechanism of diffusion of the hydrogen isotope in the front region due to the trapping effect for incident ion energy ranging from 1.5 to 2 keV, or the formation of a short diffusion path (H-SIA) for incident ion energy ranging from 200 to 500 eV.