期刊
PHYSICA B-CONDENSED MATTER
卷 627, 期 -, 页码 -出版社
ELSEVIER
DOI: 10.1016/j.physb.2021.413548
关键词
Magnetic force theorem (MFT); Superexchange; Monte Carlo simulation; Curie temperature; Ferrite spinel; Nanoparticles; GGA plus U-PBE; Monte Carlo methods; Spin channels
The sub-magnetic ordering of CoFe2O4 spinel was elaborated through ab-initio calculations, revealing different band gaps and magnetic features for different magnetic states. The Co-O hybridization was found to be stronger than Fe-O, and the magnetocrystalline anisotropy showed values consistent with previous studies. Using the Monte Carlo method, Curie temperatures were obtained for different magnetic orders, with the FM sub-order state having the highest temperature.
Sub-magnetic ordering of CoFe2O4 spinel was elaborated through the electronic structure via ab-initio calculations. PBE-GGA was preferred to obtain band structure and density of states applying Hubbard correction. Considered magnetic states, including distinctive sub-orders, exhibited several band gaps and magnetic features. Applying the magnetic force theorem to the ground state solution, exchange coupling energies were obtained. We double-checked O(p)-Fe/Co(d) hybridizations and exchange energies of considered magnetic states contributing to FM/FiM phases. Co-O hybridizations were stronger than Fe-O. Rest couples, obviously overshadowed the contribution of oxygen-connected ions, herewith, assuring different strengths of exchange energy. Initially, FM coupled Co-Co and Fe-Fe pairs had the strongest values. Magnetocrystalline anisotropy had close-set values consistent with previous studies (0.09210385eV for Co-Co, AFM, and Fe-Fe, FM). Curie temperatures (T-c) were obtained from temperature-dependent normalized magnetization and magnetic susceptibility curves using the Monte Carlo method on a classical Heisenberg model. Exchange energies, magnetocrystalline anisotropy, and magnetic moments obtained from DFT calculations were implemented as inputs to the simulation process. The highest Tc was found to be 725 K for the FM sub-order state. Other states undergo a phase transition under 500 K and 445 K temperatures, respectively. Considered magnetic orders can occur concerning experimental conditions and production method/procedure of CoFe2O4 spinel ferrites.
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