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Fusion Science and Technology
August 2026
Latest News
Uranium prices steady as EIA releases annual market report
The end-of-July spot price for uranium was $86.36 per pound, as reported by Cameco—roughly the same as it has been since February. Analytics firm Trading Economics reported a uranium futures price of $86.60 per pound, a figure that also has been holding steady since early April.
These updates come as the U.S. Energy Information Administration has released its 2025 Uranium Marketing Annual Report, which examines in detail multiple aspects of the U.S. uranium market. Data are derived from answers given in the Uranium Marketing Annual Survey, which collects information on contracts, deliveries (during the past year and projected for the next 10 years), purchased enrichment services, inventories, fuel assembly usage, and market requirements.
T. Morisaki, S. Masuzaki, M. Kobayashi, R. Sakamoto, K. Tanaka, K. Narihara, H. Funaba, Y. Feng, F. Sardei, N. Ohyabu, A. Komori, O. Motojima, LHD Experimental Group, Y. Feng, F. Sardei
Fusion Science and Technology | Volume 50 | Number 2 | August 2006 | Pages 216-221
Technical Paper | Stellarators | doi.org/10.13182/FST06-A1238
Articles are hosted by Taylor and Francis Online.
Confinement improvement of ~20% from the ISS95 scaling law has been observed in the outwardly shifted configuration on the local island divertor (LID) experiment. In the configuration, highly peaked electron density profiles, together with peaked electron temperature profiles, are established with hydrogen pellet injection. A steep density gradient is formed in the internal region near the rational surface of q = 2 in the density decay phase after pellet injection. The plasma stored energy or central beta value increases and reaches its maximum as the density decreases, which is typical behavior of the reheat mode. Because of the increase in the central pressure, a large Shafranov shift is observed in the electron temperature and density profiles measured with a Thomson scattering system, suggesting the formation of the internal transport barrier during the LID discharge. Such better confinement has never been seen in inwardly shifted configurations. The reason for that is discussed taking the energy and particle transport into consideration. Recent results from a modeling study with the EMC3-EIRENE code are also presented.