MHD activity induced coherent mode excitation in the edge plasma region of ADITYA-U Tokamak

TL;DR

This study investigates how MHD activity in the ADITYA-U Tokamak's edge plasma excites coherent density and potential fluctuations, revealing mode structures and their dependence on magnetic fluctuation amplitudes.

Contribution

It demonstrates the excitation of specific coherent modes in edge plasma due to MHD activity and analyzes their mode structures and scaling behavior.

Findings

Coherent modes have mode structures m/n=2/1 in potential and m/n=1/1 in density.

Coupled power fraction scales linearly with magnetic fluctuation magnitude.

Rise rates of coupled power are dependent on magnetic fluctuation growth rates.

Abstract

In this paper, we report the excitation of coherent density and potential fluctuations induced by magnetohydrodynamic (MHD) activity in the edge plasma region of ADITYA-U Tokamak. When the amplitude of the MHD mode, mainly the m/n = 2/1, increases beyond a threshold value of 0.3-0.4 %, coherent oscillations in the density and potential fluctuations are observed having the same frequency as that of the MHD mode. The mode numbers of these MHD induced density and potential fluctuations are obtained by Langmuir probes placed at different radial, poloidal, and toroidal locations in the edge plasma region. Detailed analyses of these Langmuir probe measurements reveal that the coherent mode in edge potential fluctuation has a mode structure of m/n = 2/1 whereas the edge density fluctuation has an m/n = 1/1 structure. It is further observed that beyond the threshold, the coupled power fraction scales almost linearly with the magnitude of magnetic fluctuations. Furthermore, the rise rates of the coupled power fraction for coherent modes in density and potential fluctuations are also found to be dependent on the growth rate of magnetic fluctuations. The disparate mode structures of the excited modes in density and plasma potential fluctuations suggest that the underlying mechanism for their existence is most likely due to the excitation of the global high-frequency branch of zonal flows occurring through the coupling of even harmonics of potential to the odd harmonics of pressure due to 1/R dependence of the toroidal magnetic field.