Comment on "Plasma ionization by annularly bounded helicon waves" [Phys . Plasmas 13, 063501 (2006)]
Robert W. Johnson

TL;DR
This paper critiques the neoclassical helicon wave theory, highlighting a fundamental flaw in its derivation and emphasizing that only electromagnetic waves propagate in stationary, fully ionized plasmas.
Contribution
It identifies a key mathematical flaw in the existing helicon wave theory and clarifies the nature of wave propagation in fully ionized plasmas.
Findings
The proportional relationship used in the original derivation is flawed.
Only electromagnetic waves can propagate in stationary, fully ionized plasmas.
The fundamental theorem of Stokes invalidates the curl-based derivation.
Abstract
The neoclassical calculation of the helicon wave theory contains a fundamental flaw. Use is made of a proportional relationship between the magnetic field and its curl to derive the Helmholtz equation describing helicon wave propagation; however, by the fundamental theorem of Stokes, the curl of the magnetic field must be perpendicular to that portion of the field contributing to the local curl. Reexamination of the equations of motion indicates that only electromagnetic waves propagate through a stationary region of constant pressure in a fully ionized, neutral medium.
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