Theory and Simulations of Compressional and Global Alfven Eigenmode Stability in Spherical Tokamaks
J. B. Lestz

TL;DR
This paper combines analytic theory and simulations to understand the stability of compressional and global Alfven eigenmodes in spherical tokamaks, revealing their dependence on beam parameters and potential control methods.
Contribution
It develops new analytic instability conditions and validates them with simulations and experiments, advancing understanding of CAE/GAE behavior in spherical tokamaks.
Findings
CAE/GAE excitation depends on beam velocity and geometry
Simulations reveal a new high frequency energetic particle mode
Analytic theory explains experimental GAE stabilization techniques
Abstract
Neutral-beam-driven, sub-cyclotron compressional (CAE) and global (GAE) \Alfven eigenmodes are routinely excited in spherical tokamaks such as NSTX(-U) and MAST, have been observed on the conventional aspect ratio tokamak DIII-D, and may be unstable in ITER burning plasmas. Their presence has been experimentally linked to the anomalous flattening of electron temperature profiles at high beam power in NSTX, potentially limiting fusion performance. A detailed understanding of CAE/GAE excitation, therefore, is vital to predicting (and ultimately controlling) their effects on plasma confinement. To this end, hybrid kinetic-MHD simulations are complemented with an analytic study of the linear stability properties of CAEs and GAEs. Perturbative, local analytic theory has been used to derive new instability conditions for CAEs/GAEs driven by realistic neutral beam distributions. A…
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