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    Spin order and excitations in the collinear kagome antiferromagnet Y0.5Fe3Sn3

    Jin Ding1,2,*, Yang Liu1,2,*, Feihao Pan3, Yinghao Zhu3, Yixi Su3, Stanislav E. Nikitin4, Ursula B. Hansen5, Mechthild Enderle5, Zhilun Lu6 et al.

    Linxuan Song1, Yong-Chang Lau1,2, Xiaoyan Ma1,2, Enke Liu1,†, and Huiqian Luo1,‡

    • *These authors contributed equally to this work.
    • †Contact author: ekliu@iphy.ac.cn
    • ‡Contact author: hqluo@iphy.ac.cn

    Phys. Rev. B 114, 204418 – Published 19 October, 2026

    DOI: https://doi.org/10.1103/mjd4-ylmx

    Abstract

    Kagome lattices host rich magnetic, topological, and transport phenomena owing to their geometric frustration and strong spin correlations. Here we present a systematic neutron scattering study of the kagome metal Y0.5Fe3Sn3, which orders into a collinear c-axis antiferromagnetic (AF) state below TN= 551 K. An additional anomalous Hall effect (AHE) contribution beyond the conventional magnetization-scaling response is observed well below TN under an in-plane magnetic field B∥ab. Elastic neutron scattering demonstrates that the Fe moments preserve their collinear c-axis AF alignment down to 1.5 K at zero field. Inelastic neutron scattering reveals a distinctive Y-shape spin excitation dispersion exhibiting a two-gap structure below 10 meV, likely arising from two nondegenerate spin-wave branches. Polarized neutron measurements further show that the low-temperature spin excitations are strongly anisotropic: the in-plane component Mab dominates while the c-axis component Mc is nearly absent. Upon warming, Mc gradually grows markedly but remains much weaker than Mab even at 300 K. We propose that the unconventional AHE originates from a nonzero scalar spin chirality induced by field-driven spin canting either in the static or dynamic configurations due to gapless excitations. These findings establish the collinear AF kagome metal Y0.5Fe3Sn3 as a platform for chirality-driven AHE without spontaneous spin reorientation.

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