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    Electronic and magnetic properties of FeX4 (X=N,P) monolayer and bilayer structures under strain

    Fuat Bilican1,2, Fatih Ersan2,*, Zeynep Demir Vatansever3,†, Sevgi Ozdemir Kart1, and Erol Vatansever3

    • *Contact author: fatih.ersan@adu.edu.tr
    • †Contact author: zeynep.demir@deu.edu.tr

    Phys. Rev. Applied 25, 014037 – Published 15 January, 2026

    DOI: https://doi.org/10.1103/btqb-5vh2

    Abstract

    Two-dimensional magnetic materials are promising candidates for next-generation spintronic devices because their magnetic order can be tuned by external factors, such as strain. In this work, we study FeX4 (X=N,P) in monolayer and bilayer forms through density-functional-theory calculations combined with Monte Carlo simulations and present a comprehensive picture of their structural, electronic, and magnetic behavior under biaxial strain. With respect to the monolayer configurations, the FeN4 structure exhibits a planar geometry and semiconducting properties, whereas the FeP4 structure adopts a buckled morphology and demonstrates metallic behavior. Both ML-FeN4 and ML-FeP4 are characterized by dynamic and thermal stability. In contrast, other pnictogen-containing monolayers, including FeAs4, FeSb4, and FeBi4, display structural instability. Under applied biaxial strain, the electronic character of ML-FeP4 changes from metallic to semiconducting, while ML-FeN4 maintain their semiconducting nature. In the bilayer counterparts, interlayer interactions enhance magnetic moments and alter overall stability compared with those in the monolayers. Monte Carlo simulations reveal strain-driven magnetic phase transitions together with significant variations in transition temperatures. The Curie temperature reaches about 980 K in the ferromagnetic regime of FeN4 and around 300 K in the unstrained ferromagnetic state of FeP4. BL-FeN4 remains antiferromagnetic under strain but switches between different antiferromagnetic configurations with transition temperatures in the several-hundred-kelvin range, while BL-FeP4 exhibits a strain-induced ferromagnetic phase with a transition temperature close to 133 K. These findings demonstrate the potential of Fe-based two-dimensional systems for strain-controlled and thermally robust low-power spintronic applications.

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