Hyperspatial projections of decorated Ammann-Beenker and Penrose lattices host interaction-induced Néel order that realizes g-wave and h-wave altermagnetism compatible with quasicrystalline symmetries.
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P-wave magnets exhibit spontaneous parity breaking of spin-polarized Fermi surfaces in time-reversal symmetric crystals, demonstrated via symmetry analysis in CeNiAsO with a predicted large spontaneous resistivity anisotropy.
D-wave altermagnets host a robust finite-temperature pair-density-wave superconducting phase driven by momentum-dependent spin splitting.
Collinear altermagnets can exhibit tunable mixed-parity spin textures and new dissipationless spin Hall responses when driven by two-color light or coupled to P-odd loop-current order, creating (P,T)=(-,-) or (+,+) states.
Vacancy-driven reconstruction of V2X2 monolayers creates an inverse Lieb network that realizes d-wave altermagnetism with (cos kx - cos ky) spin splitting and zero net magnetization.
Ultrafast light induces momentum-dependent altermagnetic spin splitting in antiferromagnets via photoexcited charge redistribution and lattice distortion that breaks effective time-reversal symmetry.
Slow phonons suppress the spin Edelstein effect in strained Rashba d-wave altermagnets through energy renormalization that collapses the Fermi surface, producing tunable anisotropic depolarization.
Orbital altermagnetism is defined as a symmetry-protected order of orbital magnetic moments with d-wave-like momentum locking, shown via tight-binding models and DFT in materials such as CuBr2, VS2, MoO and CrO.
Graphene antidot superlattices develop interaction-induced i-wave altermagnetic spin splitting from their intrinsic magnetic instability.
Janus FeSeX monolayers host coexisting d-wave altermagnetism without SOC and a SOC-induced topological gap with quantized spin Hall conductivity and nontrivial invariants.
NV-center quantum relaxometry encodes momentum-space anisotropy of altermagnetic spin diffusion, enabling local distinction from antiferromagnets.
A review that classifies two-dimensional altermagnets via spin-group theory, lists materials with large spin splitting, and outlines design strategies for experimental realization.
citing papers explorer
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Unconventional Altermagnetism in Quasicrystals: A Hyperspatial Projective Construction
Hyperspatial projections of decorated Ammann-Beenker and Penrose lattices host interaction-induced Néel order that realizes g-wave and h-wave altermagnetism compatible with quasicrystalline symmetries.
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P-wave magnets
P-wave magnets exhibit spontaneous parity breaking of spin-polarized Fermi surfaces in time-reversal symmetric crystals, demonstrated via symmetry analysis in CeNiAsO with a predicted large spontaneous resistivity anisotropy.
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Finite temperature pair density wave superconductivity in $d$-wave altermagnets
D-wave altermagnets host a robust finite-temperature pair-density-wave superconducting phase driven by momentum-dependent spin splitting.
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Tunable Odd-Parity Spin Splittings in Altermagnets
Collinear altermagnets can exhibit tunable mixed-parity spin textures and new dissipationless spin Hall responses when driven by two-color light or coupled to P-odd loop-current order, creating (P,T)=(-,-) or (+,+) states.
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Vacancy-driven inverse Lieb geometry: A general route to $d$-wave altermagnetism in two dimensions
Vacancy-driven reconstruction of V2X2 monolayers creates an inverse Lieb network that realizes d-wave altermagnetism with (cos kx - cos ky) spin splitting and zero net magnetization.
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A Route to Nonrelativistic Altermagnetic Spin Splitting via Ultrafast Light
Ultrafast light induces momentum-dependent altermagnetic spin splitting in antiferromagnets via photoexcited charge redistribution and lattice distortion that breaks effective time-reversal symmetry.
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Slow-phonon control of spin Edelstein effect in Rashba $d$-wave altermagnets
Slow phonons suppress the spin Edelstein effect in strained Rashba d-wave altermagnets through energy renormalization that collapses the Fermi surface, producing tunable anisotropic depolarization.
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Orbital Altermagnetism
Orbital altermagnetism is defined as a symmetry-protected order of orbital magnetic moments with d-wave-like momentum locking, shown via tight-binding models and DFT in materials such as CuBr2, VS2, MoO and CrO.
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Intrinsic i-wave altermagnetism in 2D graphene superlattices
Graphene antidot superlattices develop interaction-induced i-wave altermagnetic spin splitting from their intrinsic magnetic instability.
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Coexistence of d-Wave Altermagnetism and Topological States in Janus FeSeX (X = S, Te) Monolayers
Janus FeSeX monolayers host coexisting d-wave altermagnetism without SOC and a SOC-induced topological gap with quantized spin Hall conductivity and nontrivial invariants.
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Quantum-impurity sensing of altermagnetic order
NV-center quantum relaxometry encodes momentum-space anisotropy of altermagnetic spin diffusion, enabling local distinction from antiferromagnets.
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Classification and design of two-dimensional altermagnets
A review that classifies two-dimensional altermagnets via spin-group theory, lists materials with large spin splitting, and outlines design strategies for experimental realization.