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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In anisotropic disordered 2D metals, altermagnetism emerges at zero temperature for larger anisotropy and coupling strengths, competing with ferromagnetism at zero spin-orbit coupling and with a paramagnetic phase at finite spin-orbit coupling via a quantum critical point.
A new equivariant space group framework constructs magnetic Hamiltonians with explicit dependence on magnetic order orientation n, enabling analysis of dynamics-driven topological pumping and ab-initio modeling of real materials.
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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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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Quantum Altermagnetic Instability in Disordered Metals
In anisotropic disordered 2D metals, altermagnetism emerges at zero temperature for larger anisotropy and coupling strengths, competing with ferromagnetism at zero spin-orbit coupling and with a paramagnetic phase at finite spin-orbit coupling via a quantum critical point.
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Equivariant Space Group and Hamiltonian for Collinear Magnetic Systems
A new equivariant space group framework constructs magnetic Hamiltonians with explicit dependence on magnetic order orientation n, enabling analysis of dynamics-driven topological pumping and ab-initio modeling of real materials.
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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.