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    Magnetic fluctuations near the Van Hove singularity in the kagome-lattice Hubbard model at finite doping

    Jingyao Wang1,*, Zixuan Jia2,*, Zenghui Fan2, Qingzhuo Duan2, and Tianxing Ma2,†

    • 1Key Laboratory for Microstructural Material Physics of Hebei Province, School of Science, Yanshan University, Qinhuangdao 066004, China
    • 2School of Physics and Astronomy, and Key Laboratory of Multiscale Spin Physics (Ministry of Education), Beijing Normal University, Beijing 100875, China

    • *These authors contributed equally to this work.
    • †Contact author: txma@bnu.edu.cn

    Phys. Rev. B 113, 085128 – Published 17 February, 2026

    DOI: https://doi.org/10.1103/yfwy-q6y9

    Abstract

    The kagome-lattice Hubbard model attracts widespread interest due to its flat-band and Van Hove singularity features, which can give rise to unconventional magnetism. We employ determinant quantum Monte Carlo simulations to systematically investigate the uniform magnetic susceptibility across a range of on-site interactions and electron fillings on a two-dimensional kagome lattice. Beyond the Van Hove singularity, dominant ferromagnetic fluctuations emerge. Magnetic susceptibility grows markedly with increasing interaction strength and decreasing temperature, indicating that the Van Hove singularity acts as a critical point for the crossover of dominant magnetic fluctuations. Finite-size analysis further suggests the potential stabilization of a finite-temperature ferromagnetic phase. We also examine the sign problem to identify numerically reliable parameter regimes. These results provide valuable insights into controlling magnetic fluctuations in kagome systems and establish a computational framework for exploring flat-band physics in regimes characterized by novel quantum phases and competing orders.

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