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Calculation of exchange integrals and Curie temperature for La-substituted barium hexaferrites

As the macro behavior of the strength of exchange interaction, state of the art of Curie temperature T(c), which is directly proportional to the exchange integrals, makes sense to the high-frequency and high-reliability microwave devices. Challenge remains as finding a quantitative way to reveal the...

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Detalles Bibliográficos
Autores principales: Wu, Chuanjian, Yu, Zhong, Sun, Ke, Nie, Jinlan, Guo, Rongdi, Liu, Hai, Jiang, Xiaona, Lan, Zhongwen
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5086983/
https://www.ncbi.nlm.nih.gov/pubmed/27796361
http://dx.doi.org/10.1038/srep36200
Descripción
Sumario:As the macro behavior of the strength of exchange interaction, state of the art of Curie temperature T(c), which is directly proportional to the exchange integrals, makes sense to the high-frequency and high-reliability microwave devices. Challenge remains as finding a quantitative way to reveal the relationship between the Curie temperature and the exchange integrals for doped barium hexaferrites. Here in this report, for La-substituted barium hexaferrites, the electronic structure has been determined by the density functional theory (DFT) and generalized gradient approximation (GGA). By means of the comparison between the ground and relative state, thirteen exchange integrals have been calculated as a function of the effective value U(eff). Furthermore, based on the Heisenberg model, the molecular field approximation (MFA) and random phase approximation (RPA), which provide an upper and lower bound of the Curie temperature T(c), have been adopted to deduce the Curie temperature T(c). In addition, the Curie temperature T(c) derived from the MFA are coincided well with the experimental data. Finally, the strength of superexchange interaction mainly depends on 2b-4f(1), 4f(2)-12k, 2a-4f(1), and 4f(1)-12k interactions.