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Study of the structural, electronic, magnetic and magnetocaloric properties of La(0.5)Ca(0.5)Mn(0.9)V(0.1)O(3) sample: first-principles calculation (DFT–MFT)

This paper presents a correlation between experimental and theoretical approaches to study the structural, electronic, magnetic, and magnetocaloric properties of La(0.5)Ca(0.5)Mn(0.9)V(0.1)O(3). The studied compound crystallizes in the Pbnm orthorhombic space group. The calculated DOS using the DFT...

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Detalles Bibliográficos
Autores principales: Mabrouki, A., Messaoudi, O., Mansouri, M., Elgharbi, S., Bardaoui, A.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society of Chemistry 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9043998/
https://www.ncbi.nlm.nih.gov/pubmed/35498110
http://dx.doi.org/10.1039/d1ra07177g
Descripción
Sumario:This paper presents a correlation between experimental and theoretical approaches to study the structural, electronic, magnetic, and magnetocaloric properties of La(0.5)Ca(0.5)Mn(0.9)V(0.1)O(3). The studied compound crystallizes in the Pbnm orthorhombic space group. The calculated DOS using the DFT + U method proves that La(0.5)Ca(0.5)Mn(0.9)V(0.1)O(3) sample exhibits semi-metallic behavior, which is preferred in spintronic applications. The calculated PDOS proves that the high hydration among Mn 3d, V 3d and O 2p at the Fermi energy level is responsible for the FM behavior of La(0.5)Ca(0.5)Mn(0.9)V(0.1)O(3). The magnetic moment has been calculated using DFT results by estimating the valence electron population. The optical properties show high light absorption in the UV region. By using the Bean–Rodbell method, the magnetic phase shows a second-order transition where η = 0.85, and the exchange parameter λ is found to be 1.19 T g(−1) emu(−1). Based on the mean-field theory, the saturation magnetization (M(0)), the Landé factor (g), and the total angular momentum (J) were determined. These parameters were used to simulate magnetization as a function of the magnetic field at different temperatures as well as the variation of the magnetic entropy change ΔS(M) (T).