Symmetry classification framework for unconventional magnetism identifies hybrid-parity and unconstrained-parity classes beyond altermagnets and odd-parity magnets, with computational example of combined spintronic effects.
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Cs1-δV2Te2O hosts hidden altermagnetism consisting of spatially alternating altermagnetic layers whose local spin polarizations are verified by spin-resolved ARPES.
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.
Slave-boson calculations on the checkerboard Hubbard model show altermagnons crossing from chirality-selective dissipation to coherent but deformed chiral branches at the metal-insulator transition.
citing papers explorer
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Unconventional Magnetism: Symmetry Classification, Hybrid-parity and Unconstrained-parity Classes
Symmetry classification framework for unconventional magnetism identifies hybrid-parity and unconstrained-parity classes beyond altermagnets and odd-parity magnets, with computational example of combined spintronic effects.
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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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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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Altermagnons at the metal-insulator transition
Slave-boson calculations on the checkerboard Hubbard model show altermagnons crossing from chirality-selective dissipation to coherent but deformed chiral branches at the metal-insulator transition.