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DOE OSTI · 3012295

Microturbulence Suppression by Alfvén Eigenmodes in the DIII-D Tokamak

Du, X. D. [General Atomics, San Diego, CA (United States)] (ORCID:0000000161272825)·Heidbrink, W. W. [University of California, Irvine, CA (United States)] (ORCID:0000000269428043)·Yan, Z. [University of Wisconsin-Madison, WI (United States)]·Diamond, P. H. [University of California San Diego, La Jolla, CA (United States)] (ORCID:0000000332732604)·McKee, G. R. [University of Wisconsin-Madison, WI (United States)] (ORCID:0000000227549816)·Schmitz, L. [University of California-Los Angeles, CA (United States)] (ORCID:0000000313460914)·Van Zeeland, M. A. [General Atomics, San Diego, CA (United States)] (ORCID:0000000279112739)·Wang, H. Q. [General Atomics, San Diego, CA (United States)]·Austin, M. E. [University of Texas-Austin, TX (United States)] (ORCID:0000000200178605)·Liu, L. [University of Texas-Austin, TX (United States)] (ORCID:0009000879344848)·Callahan, K. J. [University of California, Irvine, CA (United States); Oak Ridge Institute for Science and Education (ORISE), Oak Ridge, TN (United States)] (ORCID:0000000152682590)·Shi, N. [General Atomics, San Diego, CA (United States)]
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Abstract

Mitigation and suppression of low-𝑘 turbulence are observed during the nonlinear evolution of toroidicity-induced Alfvén eigenmodes (TAEs) in DIII-D experiments. Turbulence mitigation begins when the dominant TAE starts to depart from the typical shear Alfvén wave polarization. TAE activity then evolves into a new state, characterized by more discrete coherent modes, increased total amplitude, and more localized radial structures. During this transition, a narrow shear flow layer forms, driven by an enhanced Reynolds stress force, with a shearing rate that exceeds the local turbulence decorrelation rate, leading to a full turbulence suppression. Furthermore, these observations indicate the imbalance between Reynolds and Maxwell stress forces during the nonlinear evolution of the TAE and their important roles in shear flow generation and turbulence reduction.

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Du, X. D. [General Atomics, San Diego, CA (United States)] (ORCID:0000000161272825), Heidbrink, W. W. [University of California, Irvine, CA (United States)] (ORCID:0000000269428043), Yan, Z. [University of Wisconsin-Madison, WI (United States)], Diamond, P. H. [University of California San Diego, La Jolla, CA (United States)] (ORCID:0000000332732604), McKee, G. R. [University of Wisconsin-Madison, WI (United States)] (ORCID:0000000227549816), Schmitz, L. [University of California-Los Angeles, CA (United States)] (ORCID:0000000313460914), Van Zeeland, M. A. [General Atomics, San Diego, CA (United States)] (ORCID:0000000279112739), Wang, H. Q. [General Atomics, San Diego, CA (United States)], Austin, M. E. [University of Texas-Austin, TX (United States)] (ORCID:0000000200178605), Liu, L. [University of Texas-Austin, TX (United States)] (ORCID:0009000879344848), Callahan, K. J. [University of California, Irvine, CA (United States); Oak Ridge Institute for Science and Education (ORISE), Oak Ridge, TN (United States)] (ORCID:0000000152682590), Shi, N. [General Atomics, San Diego, CA (United States)]. 2025-12-22. Microturbulence Suppression by Alfvén Eigenmodes in the DIII-D Tokamak. https://doi.org/10.1103/fdnb-ycz7

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