Chemical Magic: How a Hydrogen Layer Creates Altermagnetism and Record Magnetoresistance ✛ ✦

Original: "Surface Functionalization Enables Two-Dimensional Altermagnetism and Giant Tunnel Magnetoresistance"
arXiv:2607.03908 · 2026-07-04 · CC BY 4.0 · 2 min
Chemical modification of a FeSe monolayer turns an ordinary antiferromagnet into an altermagnet with record tunneling magnetoresistance.

In the grand symphony of magnetism, a duo long reigned: boisterous ferromagnetism and silent antiferromagnetism, where spin-soloists cancel each other out. But recently, a third voice joined the ensemble — altermagnetism. Imagine a conductor making the orchestra play soundlessly, yet each instrument carries its own part: an altermagnet separates electrons by spin without creating magnetization. The trouble is that in the flat world of two-dimensional materials, such a talent was almost unheard of — until chemists stepped in, wielding the tool of surface functionalization.

The FeSe monolayer, known for its record superconductivity above 100 K, proved to be an ideal platform. Simply attaching hydrogen atoms to just one side shatters the strict symmetry like a cracked mirror.

Numerical simulations show: a single surface hydrogenation, oxidation, or fluorination breaks inversion and mirror symmetries, transforming mundane spin degeneracy into exquisite d-wave splitting. In the hydrogenated iron-selenide monolayer (Fe₂Se₂H), pairs of Weyl point-antipodes with opposite Chern numbers are born, and spin-orbit coupling opens a topological gap. Thus begins the subtle dance of quantum fields: the wave-particle duality of electrons acquires precise spin polarization: they are not just particles, but waves with perfectly tuned orientation.

Transport calculations in structures like Au/Fe₂Se₂H/barrier/Fe₂Se₂H/Au revealed giant tunneling magnetoresistance—1870%. That’s almost 20 times higher than modern commercial magnetic tunnel junctions. When the Néel vectors in the two layers are parallel, the spin filters are aligned, and current flows freely; when antiparallel, the channel is blocked. Like a lock obedient to a chemical key, the device controls the flow of spin-polarized electrons. The Pauli principle, forbidding two electrons from occupying the same state, here turns into selective transmission: one channel is a high-speed freeway, the other a solid wall.

Looking ahead, chemical engineering can be extended to other antiferromagnetic monolayers. Moreover, combining with FeSe’s innate superconductivity opens a path to hybrid devices where altermagnetic and superconducting correlations intertwine in novel quantum states. This discovery is already changing the rules of the game: instead of passively searching for altermagnets, scientists gain an active method to construct them, and the record magnetoresistance promises spintronic memory and logic with previously unattainable density and speed.

The FeSe monolayer is a record-holder among chalcogenides: its superconducting temperature surpasses 100 K. Altermagnets, theoretically described just a few years ago, had until now eluded direct observation in two-dimensional form due to intricate symmetry requirements.

\mathrm{TMR} = \frac{G_{\mathrm{PC}} - G_{\mathrm{APC}}}{G_{\mathrm{APC}}} \times 100\%
G_PC and G_APC are the total conductances (summed over spin channels) in the state with parallel and antiparallel Néel vectors, respectively.
G^{\sigma} = \frac{e^2}{h} \frac{1}{N} \sum_{\mathbf{k}} T^{\sigma}_{\mathbf{k}}(E)
G^σ is the conductance for spin σ, e²/h is the conductance quantum, T^σ_k(E) is the transmission coefficient for wave vector k at energy E.
Scientists
Wolfgang PauliMax PlanckAlbert EinsteinEnrico FermiPaul DiracJohn Henry Poynting
Concepts
d wave altermagnet altermagnetism antiferromagnetic order domain wall Fermi surface antiferromagnet