Bilayer odd-parity coplanar magnets constructed from altermagnets realize tunable nonrelativistic SOC spin textures equivalent to relativistic counterparts.
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Cr7Se8 hosts mirror-protected Weyl nodal loops near the Fermi level arising from its coplanar triangular altermagnetic order.
Collinear altermagnets can exhibit tunable mixed-parity spin textures and new dissipationless spin Hall responses when driven by two-color light or coupled to P-odd loop-current order, creating (P,T)=(-,-) or (+,+) states.
Odd-parity altermagnetism reconstructs local topology in the Chern-insulating phase of the Haldane-Hubbard model without changing the total Chern number.
P-wave orbital magnetism protected by combined translation and time-reversal symmetry is proposed to originate from loop-current-induced orbital textures in a 2D Dirac lattice model, measurable via orbital Hall conductivity.
A J1-J2-J3 Heisenberg model plus DFT yields a global phase diagram for NiAs-type compounds that includes new g-wave altermagnets, f-wave OPMs, and mixed-parity states dominated by f-wave in CrSe and CrTe1-xSex.
Second-order nonlinear response to a temperature gradient induces magnetization in d′, g′, and i′ altermagnets (and in d-wave for arbitrary gradient direction), but not in the corresponding unprimed g- and i-wave cases.
citing papers explorer
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Nonrelativistic Spin-Orbit-Coupling Effects in Odd-Parity Coplanar Magnets
Bilayer odd-parity coplanar magnets constructed from altermagnets realize tunable nonrelativistic SOC spin textures equivalent to relativistic counterparts.
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Symmetry-Protected Weyl Nodal Loops in a Triangular Altermagnet
Cr7Se8 hosts mirror-protected Weyl nodal loops near the Fermi level arising from its coplanar triangular altermagnetic order.
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Tunable Odd-Parity Spin Splittings in Altermagnets
Collinear altermagnets can exhibit tunable mixed-parity spin textures and new dissipationless spin Hall responses when driven by two-color light or coupled to P-odd loop-current order, creating (P,T)=(-,-) or (+,+) states.
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The odd-parity altermagnetism induced reconstruction of the Chern-insulating phase in Haldane-Hubbard model
Odd-parity altermagnetism reconstructs local topology in the Chern-insulating phase of the Haldane-Hubbard model without changing the total Chern number.
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$P$-wave Orbital Magnetism
P-wave orbital magnetism protected by combined translation and time-reversal symmetry is proposed to originate from loop-current-induced orbital textures in a 2D Dirac lattice model, measurable via orbital Hall conductivity.
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Global magnetic phase diagram and multiple unconventional magnets in NiAs-type compounds
A J1-J2-J3 Heisenberg model plus DFT yields a global phase diagram for NiAs-type compounds that includes new g-wave altermagnets, f-wave OPMs, and mixed-parity states dominated by f-wave in CrSe and CrTe1-xSex.
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Magnetization induced by a nonlinear response to temperature gradient in $d^{\prime }$, $g^{\prime }$ and $i^{\prime }$ altermagnets
Second-order nonlinear response to a temperature gradient induces magnetization in d′, g′, and i′ altermagnets (and in d-wave for arbitrary gradient direction), but not in the corresponding unprimed g- and i-wave cases.