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Synthesis and Study of Fe-Doped Bi(2)S(3) Semimagnetic Nanocrystals Embedded in a Glass Matrix

Iron-doped bismuth sulphide (Bi(2−x)Fe(x)S(3)) nanocrystals have been successfully synthesized in a glass matrix using the fusion method. Transmission electron microscopy images and energy dispersive spectroscopy data clearly show that nanocrystals are formed with an average diameter of 7–9 nm, depe...

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Detalles Bibliográficos
Autores principales: Silva, Ricardo S., Mikhail, Hanna D., Guimarães, Eder V., Gonçalves, Elis R., Cano, Nilo F., Dantas, Noelio O.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2017
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6152244/
https://www.ncbi.nlm.nih.gov/pubmed/28696350
http://dx.doi.org/10.3390/molecules22071142
Descripción
Sumario:Iron-doped bismuth sulphide (Bi(2−x)Fe(x)S(3)) nanocrystals have been successfully synthesized in a glass matrix using the fusion method. Transmission electron microscopy images and energy dispersive spectroscopy data clearly show that nanocrystals are formed with an average diameter of 7–9 nm, depending on the thermic treatment time, and contain Fe in their chemical composition. Magnetic force microscopy measurements show magnetic phase contrast patterns, providing further evidence of Fe incorporation in the nanocrystal structure. The electron paramagnetic resonance spectra displayed Fe(3+) typical characteristics, with spin of 5/2 in the 3d(5) electronic state, thereby confirming the expected trivalent state of Fe ions in the Bi(2)S(3) host structure. Results from the spin polarized density functional theory simulations, for the bulk Fe-doped Bi(2)S(3) counterpart, corroborate the experimental fact that the volume of the unit cell decreases with Fe substitutionally doping at Bi1 and Bi2 sites. The Bader charge analysis indicated a pseudo valency charge of 1.322|e| on Fe(Bi)(1) and 1.306|e| on Fe(Bi)(2) ions, and a spin contribution for the magnetic moment of 5.0 µ(B) per unit cell containing one Fe atom. Electronic band structures showed that the (indirect) band gap changes from 1.17 eV for Bi(2)S(3) bulk to 0.71 eV (0.74 eV) for Bi(2)S(3):Fe(Bi1) (Bi(2)S(3):Fe(Bi2)). These results are compatible with the 3d(5) high-spin state of Fe(3+), and are in agreement with the experimental results, within the density functional theory accuracy.