Spin order and excitations in the collinear kagome antiferromagnet Y 0.5 Fe 3 Sn 3

arXiv:2610.29708 · cond-mat.str-el · Submitted 2026-10-21 · Read on arXiv

cond-mat.str-el

Submitted: 2026-10-21

Updated: 2026-10-21

Comments: 21 pages, 15 figures, Published on Physical Review B

Journal ref: Physical Review B 114, 204418 (2026)

DOI: 10.1103/mjd4-ylmx

License: http://creativecommons.org/licenses/by/4.0/

The gist: Kagome lattices host rich magnetic, topological, and transport phenomena owing to their geometric frustration and strong spin correlations.

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 Y 0.5 Fe 3 Sn 3, which orders into a collinear c-axis antiferromagnetic (AF) state below T N = 551 K. An additional anomalous Hall effect (AHE) contribution beyond the conventional magnetization-scaling response is observed well below T N 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 M ab dominates while the c-axis component M c is nearly absent. Upon warming, M c gradually grows markedly but remains much weaker than M ab 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 Y 0.5 Fe 3 Sn 3 as a platform for chirality-driven AHE without spontaneous spin reorientation.

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