TbB4 hosts component-resolved mixed-parity spin textures in a 3D compensated magnet, with p/f-wave odd parity in-plane and d-wave even parity out-of-plane, driven by staggered Berry phase from scalar spin chirality.
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8 Pith papers cite this work. Polarity classification is still indexing.
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Bichromatic Floquet driving activates giant perpendicular Edelstein polarizations in 2D altermagnets by breaking rotational symmetry.
Spin accumulation electrically injects a vector magnon spin current into altermagnets with a transverse component enhanced by two orders of magnitude due to broken PT symmetry, providing a transport signature to distinguish them from conventional antiferromagnets.
Cs1-δV2Te2O hosts hidden altermagnetism consisting of spatially alternating altermagnetic layers whose local spin polarizations are verified by spin-resolved ARPES.
Altermagnetic sublattice order imposes momentum-dependent nodes in the superconducting gap for local pairing interactions and favors nonunitary equal-spin triplet superconductivity at large spin splitting.
Checkerboard-lattice Hubbard electrons are unstable to weak-coupling altermagnetism whose magnons display alternating chirality splitting.
Cobalt doping converts FeSb2 into a metallic altermagnet with infrared-visible spin-split bands persisting to room temperature.
Multipole analysis of α-MnTe shows that distinct altermagnetic configurations induce spin-momentum locking with different parities and magnetic spin Hall effects with up to 16% angle, enabling identification of order parameters via anisotropy.
citing papers explorer
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Unconventional Mixed-Parity Magnetism in Rare-Earth Tetraborides
TbB4 hosts component-resolved mixed-parity spin textures in a 3D compensated magnet, with p/f-wave odd parity in-plane and d-wave even parity out-of-plane, driven by staggered Berry phase from scalar spin chirality.
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Giant perpendicular Edelstein polarization in 2D compensated magnets via bichromatic Floquet driving
Bichromatic Floquet driving activates giant perpendicular Edelstein polarizations in 2D altermagnets by breaking rotational symmetry.
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Vector Magnonics: Electrical Injection and Control of Spin Flow in Altermagnets
Spin accumulation electrically injects a vector magnon spin current into altermagnets with a transverse component enhanced by two orders of magnitude due to broken PT symmetry, providing a transport signature to distinguish them from conventional antiferromagnets.
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Observation of hidden altermagnetism in Cs$_{1-\delta}$V$_2$Te$_2$O
Cs1-δV2Te2O hosts hidden altermagnetism consisting of spatially alternating altermagnetic layers whose local spin polarizations are verified by spin-resolved ARPES.
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Inherent momentum-dependent gap structure of altermagnetic superconductors
Altermagnetic sublattice order imposes momentum-dependent nodes in the superconducting gap for local pairing interactions and favors nonunitary equal-spin triplet superconductivity at large spin splitting.
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Weak-coupling altermagnetism and chiral magnetic excitations in a checkerboard lattice
Checkerboard-lattice Hubbard electrons are unstable to weak-coupling altermagnetism whose magnons display alternating chirality splitting.
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From Narrow-gap Semiconductor to Metallic Altermagnet: Optical Fingerprints of Co-Doped FeSb2
Cobalt doping converts FeSb2 into a metallic altermagnet with infrared-visible spin-split bands persisting to room temperature.
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Multipole analysis of spin currents in altermagnetic MnTe
Multipole analysis of α-MnTe shows that distinct altermagnetic configurations induce spin-momentum locking with different parities and magnetic spin Hall effects with up to 16% angle, enabling identification of order parameters via anisotropy.