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Updated: Jan 11, 2026

Optimization, Test and Diagnostics of Miniaturized Hall Thrusters
Published on: February 16, 2019
Wave topology in Hall magnetohydrodynamics.
Alejandro Mesa Dame1, Hong Qin1, Eric Palmerduca1
1Princeton University, Princeton University, Princeton Plasma Physics Laboratory, Princeton, New Jersey 08540, USA and Department of Astrophysical Sciences, Princeton, New Jersey 08540, USA.
Hall magnetohydrodynamics (HMHD) extends ideal magnetohydrodynamics (MHD) by including the Hall effect. This study details HMHD wave modes, finding they are topologically distinct from ideal MHD despite sharing the same spectrum.
Area of Science:
- Plasma physics
- Magnetohydrodynamics
- Wave phenomena
Background:
- Ideal magnetohydrodynamics (MHD) simplifies plasma behavior.
- Hall magnetohydrodynamics (HMHD) offers greater accuracy at smaller scales by including the Hall effect.
- A complete description of HMHD eigenmodes was previously lacking.
Purpose of the Study:
- To derive the complete spectrum and eigenvectors of Hall magnetohydrodynamics (HMHD) waves.
- To identify the topological structure of HMHD wave modes.
- To clarify the relationship between HMHD and ideal MHD wave spectra.
Main Methods:
- Derivation of HMHD wave spectrum and eigenvectors.
- Analysis of wave mode topology.
- Comparison with ideal MHD in the limit of vanishing Hall parameter.
Main Results:
- The HMHD wave spectrum consists of three branches: slow magnetosonic-Hall, shear Alfvén-Hall, and fast magnetosonic-Hall waves.
- These branches continuously reduce to ideal MHD counterparts as the Hall parameter approaches zero.
- HMHD wave structure exhibits nontrivial topology with a Weyl point and nonzero Chern numbers, unlike ideal MHD.
Conclusions:
- HMHD wave spectrum is homotopic to ideal MHD, with no additional branches.
- The key distinction lies in the topological properties of HMHD waves.
- The findings clarify the nature of wave propagation in Hall magnetohydrodynamics.
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