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Axisymmetric global Alfvén eigenmodes in the TCV tokamak

M. DrevalInstitute of Plasma Physics, National Science Center, Kharkov Institute of Physics and TechnologyS. E. SharapovUKAEA, Culham CampusH. J. C. OliverUKAEA, Culham CampusM FitzgeraldUKAEA, Culham CampusA. KarpushovEcole Polytechnique Fédérale de Lausanne (EPFL), Swiss Plasma Center (SPC)A. Jansen van VuurenEcole Polytechnique Fédérale de Lausanne (EPFL), Swiss Plasma Center (SPC)J. Poley-SanjuánEcole Polytechnique Fédérale de Lausanne (EPFL), Swiss Plasma Center (SPC)M. PodestáEcole Polytechnique Fédérale de Lausanne (EPFL), Swiss Plasma Center (SPC)F. PorcelliTurin Polytechnic Universitythe TCV Teamthe EUROfusion Tokamak Exploitation Team
2026en
ABI

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Abstract Global Alfvén eigenmodes (GAEs) with toroidal mode number n = 0 (i.e. axisymmetric) have been observed in the toroidicity-induced, ellipticity-induced, and above non-circularity-induced frequency ranges in the TCV tokamak. Observation of n = 0 GAEs at multiple frequencies, caused by the periodic structure of the Alfvén continuum in frequency, demonstrates the fundamental nature of these modes. A radial splitting of the n = 0 GAEs has been predicted by linear MHD calculation. This calculation is consistent with the recently observed radial splitting of GAEs in the sub-cyclotron frequency range. Linear MHD codes were used to compute the n = 0 Alfvén continuum and the corresponding eigenmode structures. The modeling confirms that the n = 0 GAEs are located mainly below the minima of the Alfvén continuum, although some modes are observed above the continuum maxima, similar to the sub-cyclotron-frequency GAEs, for which modes above the continuum maxima have also been reported. The n = 0 GAEs have been observed in a variety of discharge types, including low- and high-density plasmas, positive- and negative-triangularity configurations, and discharges with neutral beam injection in both co-current and counter-current directions. A key factor for the appearance of n = 0 GAEs is a positive gradient in the particle energy distribution function, ∂ f /∂ E > 0 (bump-on-tail), which has been confirmed by TRANSP calculations for all discharges.

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