Crystalline antiunitary symmetry in altermagnets selects pairing that produces robust nodal topological superconducting phases with Majorana flat bands and chiral edge states.
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Altermagnets host a purely intrinsic orbital-splitter current that is strongly anisotropic, exceeds the spin-splitter current by up to a factor of four in some directions, and generates damping-like torque to speed up magnetization switching.
Altermagnets host a giant nonperturbative magnetic orbital Hall effect that generates collinear orbital currents capable of switching perpendicular magnetization without external fields.
Checkerboard-lattice Hubbard electrons are unstable to weak-coupling altermagnetism whose magnons display alternating chirality splitting.
A weak crystal potential in d-wave altermagnets induces real-space spin quadrupolar order without unit cell enlargement.
citing papers explorer
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Nodal Topological Superconductivity Driven by Crystalline Antiunitary Symmetry in Altermagnets
Crystalline antiunitary symmetry in altermagnets selects pairing that produces robust nodal topological superconducting phases with Majorana flat bands and chiral edge states.
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Orbital-Splitter Current in Altermagnets
Altermagnets host a purely intrinsic orbital-splitter current that is strongly anisotropic, exceeds the spin-splitter current by up to a factor of four in some directions, and generates damping-like torque to speed up magnetization switching.
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Nonperturbative Magnetic Orbital Hall Effect in Altermagnets
Altermagnets host a giant nonperturbative magnetic orbital Hall effect that generates collinear orbital currents capable of switching perpendicular magnetization without external fields.
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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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Spin Quadrupolar orders in $d$-wave Unconventional Magnetism
A weak crystal potential in d-wave altermagnets induces real-space spin quadrupolar order without unit cell enlargement.