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Conference on Nuclear Training and Education: A Biennial International Forum (CONTE 2025)
February 3–6, 2025
Amelia Island, FL|Omni Amelia Island Resort
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Fermilab center renamed after late particle physicist Helen Edwards
Fermi National Accelerator Laboratory’s Integrated Engineering Research Center, which officially opened in January 2024, is now known as the Helen Edwards Engineering Center. The name was changed to honor the late particle physicist who led the design, construction, commissioning, and operation of the lab’s Tevatron accelerator and was part of the Water Resources Development Act signed by President Biden in December 2024, according to a Fermilab press release.
G. T. Hoang
Fusion Science and Technology | Volume 56 | Number 3 | October 2009 | Pages 1417-1431
Technical Papers | Tore Supra Special Issue | doi.org/10.13182/FST09-A9185
Articles are hosted by Taylor and Francis Online.
From both simulation and theoretical perspectives, the current density profile of magnetized plasma is expected to play an important role in turbulence. Optimization of both the safety factor q and the magnetic shear s can reduce turbulence, and therefore heat transport.Experimentally, external sources of heating and/or noninductive current drive have been used in Tore Supra to modify the current profile. In these experiments, electron heat diffusivity and turbulence level were found to be reduced when increasing s or reversing the q profile (i.e., negative s). As a consequence, confinement was improved.Core electron heat transport has been investigated. A critical threshold temperature gradient, above which turbulence strongly increases, has been experimentally determined. A parametric dependence study of this threshold pointed out the role of the ratio s/q, as expected by turbulence theory and simulations, thus explaining improved confinement regimes.Finally, thanks to the unique Tore Supra experimental conditions, the role of the q profile on turbulent particle transport was investigated. We have demonstrated that the electron density profile peaking is strongly governed by the q profile in low collisionality plasmas with dominant trapped electron modes.