Altermagnetic order turns circular Abrikosov vortices into elliptical ones whose orientation follows the magnetic field direction relative to the Néel vector, producing nonreciprocal magnetization curves in pinned superconducting films.
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6 Pith papers cite this work. Polarity classification is still indexing.
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cond-mat.str-el 2 cond-mat.mes-hall 1 cond-mat.mtrl-sci 1 cond-mat.supr-con 1 physics.comp-ph 1verdicts
UNVERDICTED 6representative citing papers
Dirac quadrupole altermagnets in 2D exhibit a topological orbital piezomagnetic effect from strain altering their quadrupole Dirac points.
Introduces chiral altermagnetic magnetoelectrics in nonpolar chiral systems and identifies K[Co(HCOO)3] as a platform with Néel-vector and chirality-controlled switchable polarization.
Floquet driving with CPL creates an odd-parity altermagnetic HOTI in Cr₂CH₂ monolayer with preserved C₃-protected corner states over a range of driving strengths.
TbPt6Al3 shows a linear piezomagnetic effect with Q11 = 9.1 × 10^{-3} μ_B/(f.u. MPa) at 2 K, more than two orders of magnitude larger than prior altermagnets, attributed to strong 4f spin-orbit coupling in Tb^{3+}.
A honeycomb lattice of Aza-3-Triangulene and 2-Triangulene molecules is predicted to form a half-metallic ferrimagnet with fully spin-polarized flat-band conduction, zero net magnetization, and 50 meV exchange couplings for room-temperature stability.
citing papers explorer
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Abrikosov vortices in altermagnetic superconductors
Altermagnetic order turns circular Abrikosov vortices into elliptical ones whose orientation follows the magnetic field direction relative to the Néel vector, producing nonreciprocal magnetization curves in pinned superconducting films.
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Topological piezomagnetic effect in two-dimensional Dirac quadrupole altermagnets
Dirac quadrupole altermagnets in 2D exhibit a topological orbital piezomagnetic effect from strain altering their quadrupole Dirac points.
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Chiral Altermagnetic Magnetoelectrics
Introduces chiral altermagnetic magnetoelectrics in nonpolar chiral systems and identifies K[Co(HCOO)3] as a platform with Néel-vector and chirality-controlled switchable polarization.
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Floquet-Engineered Odd-Parity Altermagnetic Higher-Order Topology in a Two-Dimensional Antiferromagnet Cr$_2$CH$_2$
Floquet driving with CPL creates an odd-parity altermagnetic HOTI in Cr₂CH₂ monolayer with preserved C₃-protected corner states over a range of driving strengths.
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Piezomagnetic effect of a rare-earth-based altermagnet TbPt6Al3
TbPt6Al3 shows a linear piezomagnetic effect with Q11 = 9.1 × 10^{-3} μ_B/(f.u. MPa) at 2 K, more than two orders of magnitude larger than prior altermagnets, attributed to strong 4f spin-orbit coupling in Tb^{3+}.
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Prediction of room-temperature two-dimensional $\pi$-electron half-metallic ferrimagnets
A honeycomb lattice of Aza-3-Triangulene and 2-Triangulene molecules is predicted to form a half-metallic ferrimagnet with fully spin-polarized flat-band conduction, zero net magnetization, and 50 meV exchange couplings for room-temperature stability.