4.5 Article

Various edge low-frequency fluctuations during transition to a detached divertor in Experimental Advanced Superconducting Tokamak

Journal

NUCLEAR FUSION
Volume 63, Issue 6, Pages -

Publisher

IOP Publishing Ltd
DOI: 10.1088/1741-4326/acc4dd

Keywords

divertor detachment; low-frequency fluctuations; EAST

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Different types of edge low-frequency fluctuations with distinct characteristics are observed in various detached divertor states. The characteristics of three specific types of fluctuations, namely low-frequency quasi-coherent fluctuation (LFCF), low-frequency broadband frequency fluctuation (LFBF), and low -n X-point mode (LNXM), on the Experimental Advanced Superconducting Tokamak (EAST) are examined. The occurrence of LFCF is related to the energy detachment and a large electron temperature gap between the inner and outer strike points, while LFBF occurs when the inner strike point is energy detached and the outer strike point is nearly energy detached or attached. The underlying physical mechanisms of these fluctuations are proposed. Rating: 8/10.
Various edge low-frequency fluctuations with distinct characteristics exist in different detached divertor states. Three edge low-frequency fluctuations (f < 10 kHz), namely low-frequency quasi-coherent fluctuation (LFCF), low-frequency broadband frequency fluctuation (LFBF), and low -n X-point mode (LNXM) on Experimental Advanced Superconducting Tokamak (EAST), are systematically assessed. The basic features of these fluctuations, such as spectral width, location, mode number, propagating direction, and particle transport capacities, are examined. LFCF occurs when the inner strike point is energy detached or nearly energy detached with T-et,T-inner similar to 8-15 eV (T-et,T-inner is the electron temperature of the inner strike point), and a large electron temperature gap between the inner and outer strike points with Delta T-et > 25 eV (Delta T-et is the electron temperature gap between the inner and outer strike points) is essential for the occurrence of LFCF. By contrast, LFBF occurs when the inner strike point is energy detached with Tet,inner < 8 eV, while the outer strike point is nearly energy detached or attached. The Delta T-et of LFBF is generally lower than that of LFCF, which is <25 eV. LNXM is related only to the radiative divertor with impurity seeding and considered to be excited by the geodesic acoustic mode proposed in earlier work (Sun 2021 Nucl. Fusion 61 014002; Diallo 2020 28th IAEA Fusion Energy Conf.), or the coupling of impurity radiation condensation instability and drift waves proposed in a previous work (Ye 2021 Nucl. Fusion 61 116032). In addition, the possible physical mechanisms of LFBF and LFCF are proposed, with LFBF being the purely growing rippling mode and LFCF being the mode formed by the coupling of the rippling mode to the drift waves. Related research may be beneficial to better clarify the various low-frequency fluctuations that occur during different divertor states.

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