Abstract

The role of self-generated zonal flows in the collisionless trapped-electron-mode (CTEM) turbulence is a long-standing open issue in tokamak plasmas. Here, we show, for the first time, that the zonal flow excitation in the CTEM turbulence is formally isomorphic to that in the ion temperature gradient turbulence. Trapped electrons contribute implicitly only via linear dynamics. Theoretical analyses further suggest that, for short wavelength CTEMs, the zonal flow excitation is weak and, more importantly, not an effective saturation mechanism. Corresponding controlling parameters are also identified theoretically. These findings not only offer a plausible explanation for previous seemingly contradictory simulation results, but can also facilitate controlling the CTEM instability and transport with experimentally accessible parameters.

Highlights

  • Zonal flows (ZFs) are azimuthally symmetric sheared flows spontaneously excited by small scale fluctuations

  • Studies have shown that the role of ZF in collisionless trapped-electron-mode (CTEM) turbulence is parameter sensitive, with different controlling parameters identified from different simulations [5–14]

  • The turbulence is driven by trapped electrons, the nonlinear CTEM ZF interplay is governed by ions and circulating electrons

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Summary

Introduction

Zonal flows (ZFs) are azimuthally symmetric sheared flows spontaneously excited by small scale fluctuations. The role of self-generated zonal flows in the collisionless trapped-electron-mode (CTEM) turbulence is a long-standing open issue in tokamak plasmas. We show, for the first time, that the zonal flow excitation in the CTEM turbulence is formally isomorphic to that in the ion temperature gradient turbulence.

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