A symmetry-based stacking strategy with layer-flip realizes odd-parity altermagnetism from nonrelativistic orbital orders, hosting quantum spin Hall phases with helical edge states.
Salehi,Transverse Spin Supercurrent at p-wave magnetic Josephson Junctions, arXiv:2507.11397 (2025)
3 Pith papers cite this work. Polarity classification is still indexing.
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Low-field domain selection in CeNiAsO enables giant reversible in-plane resistivity anisotropy up to 35 percent in both Néel and spin-density-wave phases.
Self-consistent BdG calculations on a p-wave magnet model show magnetic coupling drives transitions from dominant s-wave to mixed p_x-wave and then to equal-spin p_y-wave superconductivity with coexistence and competition regimes.
citing papers explorer
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Odd-Parity Altermagnetism Originated from Orbital Orders
A symmetry-based stacking strategy with layer-flip realizes odd-parity altermagnetism from nonrelativistic orbital orders, hosting quantum spin Hall phases with helical edge states.
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Sub-spin-flop switching of a fully compensated antiferromagnet by magnetic field
Low-field domain selection in CeNiAsO enables giant reversible in-plane resistivity anisotropy up to 35 percent in both Néel and spin-density-wave phases.
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Competition and coexistence of superconducting symmetries in $p$-wave magnets
Self-consistent BdG calculations on a p-wave magnet model show magnetic coupling drives transitions from dominant s-wave to mixed p_x-wave and then to equal-spin p_y-wave superconductivity with coexistence and competition regimes.