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    Electron spin resonance signatures of Dirac spinons in the Gd-substituted kagome antiferromagnet Gd0.015Y0.985Cu3(OD)6.5Br2.5

    T. Y. Kim1, C. Koo1,*, K. Yu. Povarov2, U. Jena3, P. Khunita3,4, S. A. Zvyagin2, J. Wosnitza2,5, and K.-Y. Choi1,†

    • *Contact author: chkoo@skku.edu
    • †Contact author: choisky99@skku.edu

    Phys. Rev. B 113, 094429 – Published 13 March, 2026

    DOI: https://doi.org/10.1103/wz8f-2dxk

    Abstract

    External stimuli offer a route to realize exotic states with nontrivial excitations in highly frustrated kagome antiferromagnets. Here, 1.5% Gd3+ ions are substituted for Y3+ ions in YCu3(OD)6.5Br2.5 (abbreviated as YCu3), yielding Gd0.015Y0.985Cu3(OD)6.5Br2.5, where the Gd3+ ions act as a local probe to investigate fractionalized excitations in the S=1/2 kagome Heisenberg antiferromagnet YCu3. The Gd substitution level is confirmed through detailed x-ray diffraction analyses, while magnetization and magnetic-susceptibility measurements disclose the interaction between the substituted Gd ions and the Cu-spin kagome network. Specific-heat measurements in magnetic fields up to 14 T and down to dilution-refrigerator temperatures reveal an enhanced density of low-energy states, indicative of spinon-impurity coupling, yet higher-energy excitations are hardly affected. Furthermore, high-frequency electron spin resonance (ESR) measurements, enabled by the presence of Gd as a local probe, present the resonance associated with Gd ions coupled with the kagome spins. In particular, the temperature dependence of the ESR linewidth exhibits a near-quadratic power-law behavior, revealing the presence of Dirac spinon dynamics in the finite-temperature regime above 2 K.

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