Tailoring Structural, Electronic, and Magnetic Properties of Fe₃O₄ and MnZn-Ferrites through Metal/Non-metal Doping: A DFT+U Study

Abstract

Nanoscale spinel-structured ferrites, especially when doped with metal or nonmetal ions, have attracted significant attention due to their tunable functional properties, making them indispensable for advanced applications in high-frequency electronics and energy conversion systems. Among these, manganese–zinc (MnZn) ferrites exhibit remarkable versatility, driving extensive theoretical and experimental research. This study presents a systematic investigation utilizing spin-polarized density functional theory with Hubbard correction (DFT+U) within the generalized gradient approximation (GGA+U), employing the Perdew–Burke–Ernzerhof (PBE) functional, to analyze the electronic, magnetic, and structural properties of Fe 3 O 4 and doped MnZn-ferrites of the form (Zn x 2+ Mn y 2+ Fe 1– x – y 3+ ) A (M x Fe 2 x –1 3+ ) B O 4 2– and (M x Fe 1– x 3+ ) A (Zn x 2+ Mn x 2+ Fe 2– x – y 3+ ) B O 4 2–, where M represents transition metals (Ti, V, Co, Mo, La) and nonmetals (Ca, Si, Sn, Bi). The findings demonstrate that Mn/Zn doping exerts a pronounced influence on lattice distortions, with crystallographic deformation minimized and structural stability maximized under equimolar Mn:Zn substitution, as evidenced in the Mn 4 Zn 4 Fe 2 O 4 composition. Formation energy calculations further suggest that transition-metal doping enhances the stability of the ferrite structures. Electronic structure analysis demonstrates that dopant selection critically governs band gap characteristics. Specifically, Ca-, Si-, V-, and Sn-doped systems exhibit half-metallic properties, whereas Mn 4 Zn 4 and Mn 8 Zn 8 -ferrites configurations retain their semiconducting nature. Computational analysis of magnetocrystalline anisotropy energy (MAE) reveals a preferential alignment of the easy magnetization axis (EMA) along the crystallographic [001] direction ( Z -axis) across all doped Mn 4 Zn 4 Fe 2 O 4 systems with the exception of Ca-doped configurations. Notably, transition-metal dopants (V, Co, Ti, and Mo) in Mn 8 Zn 8 Fe 8 O 4 exhibit robust uniaxial anisotropy, as evidenced by positive MAE values (0.25–3.5 meV/atom). This anisotropy arises from spin–orbit coupling-enhanced orbital polarization and asymmetric d-electron redistribution at dopant sites, which stabilizes the [001]-oriented magnetization.

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