Pressure-gradient-induced Alfven eigenmodes: I. Ideal MHD and finite ion Larmor radius effects

Abstract

In the second magnetohydrodynamic (MHD) ballooning stable domain of a high-beta tokamak plasma, the Schroedinger equation for ideal MHD shear Alfven waves has discrete solutions corresponding to standing waves trapped between pressure-gradient-induced potential wells. Our goal is to understand how these so-called alpha-induced toroidal Alfven eigenmodes alpha-TAE are modified by the effects of finite Larmor radii (FLR) and kinetic compression of thermal ions in the limit of massless electrons. In the present paper, we neglect kinetic compression in order to isolate and examine in detail the effect of FLR terms. After a review of the physics of ideal MHD alpha-TAE, the effect of FLR on the Schroedinger potential, eigenfunctions and eigenvalues are described with the use of parameter scans. The results are used in a companion paper to identify instabilities driven by wave-particle resonances in the second stable domain.

24 pages, 10 figures

References in corpus (2)

• Pressure-gradient-induced Alfven eigenmodes: II. Kinetic excitation with ion temperature gradient
• AWECS: A Linear Gyrokinetic Delta-f Particle-in-Cell Simulation Code for the Study of Alfvenic Instabilities in High-Beta Tokamak Plasmas

Cited by in corpus (3)

• Pressure-gradient-induced Alfven eigenmodes: II. Kinetic excitation with ion temperature gradient
• Testing the conservative character of particle simulations: I. Canonical and noncanonical guiding center model in Boozer coordinates
• Resonant theory of kinetic ballooning modes in general toroidal geometry