Characterization of the I-phase regime at TCV

Abstract The I-phase is an H-mode confinement regime of tokamaks characterized by limit cycle oscillations, the so-called LCOs or bursts. These bursts are the manifestation of a periodic flattening of the plasma edge pressure profile. The profile flattening is caused by increased radial transport, driven by a high-frequency plasma edge mode that periodically appears. This short-living mode is intrinsically connected to each burst. It vanishes once the profiles are fully flattened, and it reestablishes during profile recovery once critical gradients are reached and a new cycle begins. In this paper, we describe for the first time the unambiguous presence of the I-phase at the tokamak à configuration variable (TCV). As the I-phase confinement regime is found in the parameter regime between the L-mode and the fully developed H-mode, it is often confused with dithers between H-mode and L-mode. Therefore, we are highlighting the differences between these two phenomena. Furthermore, we show the two-dimensional dynamics of the I-phase mode and bursts and the associated filamentary transport, enabled by the outstanding capabilities of the 2D TCV Gas Puff Imaging diagnostics.

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Publication Details

Journal
Nuclear Fusion
Published
2024-11-25
DOI
https://doi.org/10.1088/1741-4326/ad96cb
Citations
3
Primary Topic
Magnetic confinement fusion research
Type
article
Field-Weighted Citation Impact
1.98

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Characterization of the I-phase regime at TCV

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3 citations
Nuclear Fusion
Magnetic confinement fusion research
1.98
article

Characterization of the I-phase regime at TCV

D. Brida, M. Griener, M. Faitsch, Y.S. Wang, N. Offeddu, C. Theiler, C. Wüthrich
article en
3 citations

Abstract

Abstract The I-phase is an H-mode confinement regime of tokamaks characterized by limit cycle oscillations, the so-called LCOs or bursts. These bursts are the manifestation of a periodic flattening of the plasma edge pressure profile. The profile flattening is caused by increased radial transport, driven by a high-frequency plasma edge mode that periodically appears. This short-living mode is intrinsically connected to each burst. It vanishes once the profiles are fully flattened, and it reestablishes during profile recovery once critical gradients are reached and a new cycle begins. In this paper, we describe for the first time the unambiguous presence of the I-phase at the tokamak à configuration variable (TCV). As the I-phase confinement regime is found in the parameter regime between the L-mode and the fully developed H-mode, it is often confused with dithers between H-mode and L-mode. Therefore, we are highlighting the differences between these two phenomena. Furthermore, we show the two-dimensional dynamics of the I-phase mode and bursts and the associated filamentary transport, enabled by the outstanding capabilities of the 2D TCV Gas Puff Imaging diagnostics.

Nuclear FusionVol. 65(1)
Max Planck Institute for Plasma Physics (DE), École Polytechnique Fédérale de Lausanne (CH)
EUROfusion, European Commission, Euratom Research and Training Programme, Staatssekretariat für Bildung, Forschung und Innovation
Openalex Percentile: Top 8%
Magnetic confinement fusion research
1.98
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