Far from being limited to a trivial generalization of their Hermitian counterparts, non-Hermitian topological phases have gained widespread interest due to their unique properties. One of the most striking non-Hermitian phenomena is the skin effect, i.e., the localization of a macroscopic fraction of bulk eigenstates at a boundary, which underlies the breakdown of the bulk-edge correspondence. Here we develop a generic phenomenological approach to describing magnetic dissipation within a lattice model and we introduce an “effective area law” to investigate the emergence of the skin effect in magnetic systems. As a testbed of our approach, we focus on a spin-orbit-coupled van der Waals (vdW) ferromagnet with spin-nonconserving magnon-phonon interactions, finding that the magnetic skin effect emerges in an appropriate temperature regime. Our results suggest that the interference between Dzyaloshinskii-Moriya interaction (DMI) and nonlocal magnetic dissipation plays a key role in the accumulation of bulk states at the boundaries.

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• Magnetism
• Skin effect
• Spintronics
• 2-dimensional systems
• Ferrimagnets
• Honeycomb lattice
• Magnetic systems
• Topological materials