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10 Pith papers cite this work. Polarity classification is still indexing.

10 Pith papers citing it

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2026 6 2025 4

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UNVERDICTED 10

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representative citing papers

Abrikosov vortices in altermagnetic superconductors

cond-mat.supr-con · 2026-04-16 · unverdicted · novelty 7.0

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.

Chiral Altermagnetic Magnetoelectrics

cond-mat.mtrl-sci · 2025-08-18 · unverdicted · novelty 7.0

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.

Theory of Spin-splitter Magnetoresistance in Altermagnets

cond-mat.mes-hall · 2026-05-11 · unverdicted · novelty 6.0

Spin-splitter magnetoresistance depends only on the relative angle between ferromagnetic magnetization and altermagnetic Neel vector, shows opposite-sign longitudinal response, and has proportional longitudinal-transverse signals, unlike spin-Hall magnetoresistance.

Moire Control of Alterelectric Quadrupolar Order

cond-mat.mtrl-sci · 2026-04-20 · unverdicted · novelty 6.0

Moiré superlattices steer the orientation of alterelectric quadrupolar order from a weakly selected regime to a robust axial-dominated state via registry-phase control in a Bloch-periodic model.

Strain Engineering of Altermagnetic Symmetry in Epitaxial RuO$_2$ Films

cond-mat.mtrl-sci · 2025-10-30 · unverdicted · novelty 6.0

Compressive strain along [001] stabilizes altermagnetism in RuO2 films on (100) and (110) TiO2 substrates, tunable by film thickness, with (100) orientation yielding ideal altermagnetic order and (110) showing uncompensated ferrimagnetism.

Topological bands in metals

cond-mat.other · 2025-10-16 · unverdicted · novelty 6.0

The number of sheets and monodromy of the electron dispersion covering of the Brillouin zone in superstructured crystals are topological invariants, realized in three-sublattice helimagnet models as a spin-textured one-sheeted Fermi surface in a topological metal.

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