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
February 2026
Nuclear Technology
January 2026
Fusion Science and Technology
Latest News
The spark of the Super: Teller–Ulam and the birth of the H-bomb—rivalry, credit, and legacy at 75 years
In early 1951, Los Alamos scientists Edward Teller and Stanislaw Ulam devised a breakthrough that would lead to the hydrogen bomb [1]. Their design gave the United States an initial advantage in the Cold War, though comparable progress was soon achieved independently in the Soviet Union and the United Kingdom.
Watanabe Osamu (19P39)
Fusion Science and Technology | Volume 51 | Number 2 | February 2007 | Pages 322-324
Technical Paper | Open Magnetic Systems for Plasma Confinement | doi.org/10.13182/FST07-A1389
Articles are hosted by Taylor and Francis Online.
An electric field distribution of a surface normal wave on a corrugated metal plate used for a surface wave oscillator was calculated. The surface wave oscillator is formed by the corrugated metal plate and a sheet electron beam. The direction of the beam propagation is parallel to the metal plate and perpendicular to the corrugation. In the vicinity of the sinusoidal corrugated metal plate, the electromagnetic wave of the surface normal mode which propagates parallel to the plate exists. From the surface normal mode computation, it was confirmed that an electric field distribution had a periodic component to the traveling direction of the beam. Cherenkov interaction should be excited by the electron beam passing in this periodic electric field region. The surface normal wave always exists only in a slow wave region, and has backward wave with the periodic boundary condition. This interaction becomes absolute instability, because the interaction is on the backward wave of the surface normal mode in the slow wave region. A strong oscillation by the surface normal wave should be generated, because the wave can generate the absolute instability of the Cherenkov interaction.