Estudo de sistemas magnéticos modeláveis mediante sub-redes

Detalhes bibliográficos
Ano de defesa: 2014
Autor(a) principal: Rodrigues, Aline do Nascimento lattes
Orientador(a): Plaza, Edison Jesús Ramírez
Banca de defesa: Não Informado pela instituição
Tipo de documento: Dissertação
Tipo de acesso: Acesso aberto
Idioma: por
Instituição de defesa: Universidade Federal de Sergipe
Programa de Pós-Graduação: Pós-Graduação em Física
Departamento: Não Informado pela instituição
País: Brasil
Palavras-chave em Português:
Palavras-chave em Inglês:
Área do conhecimento CNPq:
Link de acesso: https://ri.ufs.br/handle/riufs/5362
Resumo: We have modeled some magnetic systems, which consists of a number of sublattices, in the mean field approximation. This is possible in crystalline systems formed by two or more magnetic ions coupled by specific interactions such as the crystal field, exchange, among others. The main idea is to solve the microscopic Hamiltonian that models a given magnetic system in order to obtain their magnetic equation of state: M (H, T). For this, we use the appropriate arrangements to different magnetic (ferro-, ferri- and antiferro- magnetic) scheme sublattices. From the solutions of the Hamiltonian (eigenvalues and eigenvectors), physical quantities of interest were determined. In principle we consider systems with localized magnetism due to 3d and 4f electrons with the participation of non-magnetic ligands including 3d-4f systems with the presence of crystal field. In this dissertation we use the model of two-and three sublattices in order to obtain the equation of state for the following systems: RKKY exchange in RNi2B2C, superexchange in (Y3-zRz)(T1xFe1-x)(T2yFe3-y)O12, LixFe3- xO4 and (NixMn1-x)1.5[Cr(CN)6]. In these formulas, R represents a rare earth ion, T1 and T2 represent non-magnetic ions. Some representative cases are presented to illustrate the different equations of state and behavior of sublattices, metamagnetism, temperature compensation, etc. The extension to other similar systems can be direct or need to incorporate additional phenomenological parameters.