Cold Plasma Dispersion Tensor
\[\mathbf{n}\times(\mathbf{n}\times\mathbf{E}) + \mathbf{K}\cdot\mathbf{E} = 0\]
Source lecture(s): pc368_lec13_magnetized_wave
Physical Meaning
The cold-plasma wave equation describes electromagnetic wave propagation in a magnetized, collisionless plasma. The refractive index tensor \(\mathbf{K}\) determines cutoff, resonance, and mode polarization.
Variable Definitions
| Symbol | Definition | SI Units |
|---|---|---|
| \(\mathbf{n} = c\mathbf{k}/\omega\) | Refractive-index vector | dimless |
| \(\mathbf{K}\) | Dielectric (Stix) tensor | dimless |
| \(S, D, P\) | Stix parameters | dimless |
| \(\omega_{ps}, \Omega_{cs}\) | Species plasma/cyclotron frequencies | rad s\(^{-1}\) |
Assumptions
- Uniform \(\mathbf{B}_0\).
- Cold fluid species (finite temperature adds kinetic corrections).
- Linear waves.
Derivation
Linearize the cold-fluid momentum equation for each species, include Lorentz force, and couple to Maxwell’s equations. The susceptibility tensor is:
\[\chi_{ij} = -\sum_s \frac{\omega_{ps}^2}{\omega^2} \Bigl[ \mathbf{I} + \frac{\omega}{\Omega_{cs}}\mathbf{M} + \Bigl(\frac{\omega}{\Omega_{cs}}\Bigr)^2 \mathbf{b}\mathbf{b} \Bigr]\]
where \(\mathbf{M}\) encodes the magnetization. In their standard form this yields the \(S, D, P\) tensor.
Applications
- RF heating: Ion cyclotron range of frequencies (ICRF).
- Ionospheric propagation: HF radio windows and cuts.
- ECRH: Electron cyclotron resonance heating.
Connections to Other Equations
- Magnetized Waves: The physical modes.
- Plasma Frequency: Enters \(P\) and \(S\).
- Alfvén Speed: Related to \(\Omega_{ci}\).