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Magnetic structure of the kagome metal in view of Bragg diffraction
Phys. Rev. B 112, 144402 – Published 1 October, 2025
DOI: https://doi.org/10.1103/rn9y-6spg
Abstract
A material in possession of localized -electron magnetism and delocalized -electron or band magnetism can often present enigmatic physical phenomena, and there has been a longstanding interest in the kagome metal . More recently, because of an investigation of a so-called anomalous Hall effect, or topological Hall effect, and magnetic neutron Bragg diffraction [Yao et al., Phys. Rev. Lett. 134, 186501 (2025)]. Iron moments in the two-dimensional layers of a hexagonal nuclear structure undergo collinear antiferromagnetic order below a temperature K. The moments depart from the axis in a spontaneous transition at K to an orthorhombic structure. The magnetism of Yb ions appears to behave independently, which can be confirmed using resonant x-ray Bragg diffraction enhanced by a Fe atomic resonance. The inferred magnetic structure is P(parity)T(time)-symmetric (anti-inversion ) collinear antiferromagnetism that does not couple to circular polarization (helicity) in primary x-rays, unlike altermagnetism. A linear magnetoelectric effect is allowed, and Kerr rotation and the piezomagnetic effect are forbidden. Symmetry informed Bragg diffraction patterns for future x-ray and neutron experiments are shown to be rich in Fe magnetic properties of orthorhombic , including space-spin correlations, anapoles, and Dirac quadrupoles familiar in high- ceramic superconductors.
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