Atomistic Simulations of Cation Distribution and Defect Effects on the Performance of Substituted Ferrites

TL;DR

This study uses atomistic simulations to explore how various ion substitutions affect the structural, electronic, magnetic, and thermoelectric properties of Mn-Zn ferrites, revealing stability trends and property modifications due to doping.

Contribution

It provides a comprehensive computational analysis of how different cation substitutions influence the stability and multifunctional properties of ferrites, offering insights for material design.

Findings

Si^{4+}, Ca^{2+}, Mg^{2+} enhance stability

Substitutions retain semiconducting band gaps

Doping reduces conductivity but increases Seebeck coefficient

Abstract

This study investigates Mn-Zn ferrites (nominal composition \ce{Mn_{0.5}Zn_{0.5}Fe2O4}, MZF) substituted with tetravalent (\ce{Si^{4+}}), trivalent (\ce{Co^{3+}}), and divalent (\ce{Ca^{2+}}, \ce{Mg^{2+}}, \ce{Sn^{2+}}) ions. We comprehensively analyze how substitutions at specific tetrahedral and octahedral crystallographic sites modulate the spinel lattice's structural stability, electronic band structure, magnetic anisotropy, and electrical conductivity. Density functional theory (DFT) combined with Boltzmann transport theory is employed to probe the thermoelectric and phonon transport properties of pristine and doped MZF systems. Formation energy calculations indicate that substitutions with \ce{Si^{4+}}, \ce{Ca^{2+}}, and \ce{Mg^{2+}} enhance the thermodynamic stability of MZF, while \ce{Co^{3+}} and \ce{Sn^{2+}} substitutions exhibit slightly higher formation energies, indicating relatively lower stability. Electronic structure analyses confirm all substituted variants retain a finite band gap, preserving their semiconducting nature. Magnetic anisotropy energy (MAE) calculations reveal that ferrites with mixed octahedral/tetrahedral substitutions display a narrower MAE distribution, signifying more uniform magnetic anisotropy. Thermoelectric property analysis at 300 K demonstrates that multivalent ion doping at either crystallographic site reduces electrical conductivity ($\sigma$) while concurrently enhancing the Seebeck coefficient ($S$). This inverse correlation highlights a doping-induced trade-off, likely driven by increased carrier scattering at defect sites and modifications to the electronic density of states near the Fermi level.