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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.
Y. Sentoku, W. Kruer, M. Matsuoka, A. Pukhov
Fusion Science and Technology | Volume 49 | Number 3 | April 2006 | Pages 278-296
Technical Paper | Fast Ignition | doi.org/10.13182/FST06-A1149
Articles are hosted by Taylor and Francis Online.
In the fast ignition scheme, the compressed core is surrounded by a 1-mm-scale coronal plasma. The critical density where the laser deposits energy is still more than 100 m away from the core. The distance is much longer than the laser focus radius or the core size. This situation raises an important question: How can we couple laser energy to the core from such a distance? One of the techniques that has been proposed to overcome this problem is hole boring by the ponderomotive pressure of the incident laser light. In this paper, the physics related to the laser hole boring, including the parametric instabilities, the channel formation, and the hot electron acceleration by ultraintense laser light, are discussed. The maximum density where the laser can propagate by hole boring is obtained as a function of the intensity. This agrees well with experimental observations, and it is confirmed by numerical simulations. The acceleration mechanism of hot electrons in the magnetic channel is also identified. The hot electrons are characterized by the numerical simulations. In summary, the critical issue of energy coupling in this scheme is raised and discussed.