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    Tunable magnetic transition and electronic structure in monolayer iron trihalides FeX3 (X=F, Cl, Br, I)

    Yuchen Lei1, Wenting Wu2, Qian Wan1, Hongwei Bao1, Jia Wu3, Fei Ma1,*, and Yan Li1,†

    • 1State Key Laboratory for Mechanical Behavior of Materials, Xi'an Jiaotong University, Xi'an 710049, China
    • 2North West Electric Power Design Institute, Xi'an, Shaanxi 710075, China
    • 3Xi'an Taijin Industrial Electrochemical Technology Co., Ltd., Xi'an 710016, China

    • *Contact author: mafei@mail.xjtu.edu.cn
    • †Contact author: liyan0802@xjtu.edu.cn

    Phys. Rev. Materials 10, 034415 – Published 31 March, 2026

    DOI: https://doi.org/10.1103/ynbm-hkrp

    Abstract

    Two-dimensional (2D) iron trihalides (FeX3, X=F, Cl, Br, I) are an emerging family of van der Waals magnets whose fundamental physical properties are not yet fully understood. In this work, we present a systematic first-principles study incorporating hybrid functional (HSE06) calculations and Hubbard U corrections to unravel the spin state, magnetic order, electronic structure, and doping response in monolayer FeX3. The high-spin (S=5/2) state is unequivocally established as the universal local ground state across the series. A chemical tuned magnetic transition is identified: FeF3 adopts Néel-type antiferromagnetic (AFM) order, while FeCl3, FeBr3, and FeI3 are ferromagnetic (FM) semiconductors with Curie temperatures (TC) monotonically increasing from 154 K to 238 K. This trend is driven by the competition between direct AFM exchange and halogen-mediated FM superexchange. Electronically, FeCl3 and FeBr3 are identified as bipolar magnetic semiconductors, exhibiting a perfect linear scaling of the band gap with halogen electronegativity. An effective tight-binding model derived from maximally Wannier functions reveals a progressive increase in crystal-field splitting (Δoct) from 3.36 eV to 4.22 eV, underpinning the evolving orbital hierarchy across iron trihalides. Crucially, electron doping induces a nonmonotonic magnetic evolution, from FM to geometrically frustrated AFM (zigzag/stripy), culminating in a reentrant FM state, driven by the competition between kinetic energy minimization and orbital-selective electron correlations. Finally, bilayer systems exhibit a universally robust interlayer AFM coupling driven by pz orbital-mediated superexchange across the van der Waals gap. Our work provides a complete microscopic picture of the basic magnetic and electronic properties of the 2D FeX3, establishing them as a highly versatile material platform for tunable magnetism and spintronics.

    Physics Subject Headings (PhySH)

    Corrections

    8 May, 2026

    Correction: Typographical errors in the coefficients of Eq. (5) have been fixed.

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