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. 2020 Mar 20;10(3):563.
doi: 10.3390/nano10030563.

Synthesis, Characterization, and Optimization of Magnetoelectric BaTiO3-Iron Oxide Core-Shell Nanoparticles

Affiliations

Synthesis, Characterization, and Optimization of Magnetoelectric BaTiO3-Iron Oxide Core-Shell Nanoparticles

Mahmud Reaz et al. Nanomaterials (Basel). .

Abstract

Improvement of magnetic, electronic, optical, and catalytic properties in cutting-edge technologies including drug delivery, energy storage, magnetic transistor, and spintronics requires novel nanomaterials. This article discusses the unique, clean, and homogeneous physiochemical synthesis of BaTiO3/iron oxide core-shell nanoparticles with interfaces between ferroelectric and ferromagnetic materials. High-resolution transmission electron microscopy displayed the distinguished disparity between the core and shell of the synthesized nanoparticles. Elemental mapping and line scan confirmed the formation of the core-shell structure. Energy-dispersive X-ray spectroscopy and X-ray photoelectron spectroscopy detected the surface iron oxide phase as maghemite. Rietveld analysis of the X-ray diffraction data labeled the crystallinity and phase purity. This study provides a promising platform for the desirable property development of the futuristic multifunctional nanodevices.

Keywords: core–shell; energy-dispersive X-ray spectroscopy; magnetic iron-oxides; nanoparticles; oxide-nanomaterials synthesis; perovskite oxide; superparamagnetism.

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Conflict of interest statement

The authors declare no conflict of interest. The funders had no role in the design of the study; in the collection, analyses, or interpretation of data; in the writing of the manuscript, or in the decision to publish the results.

Figures

Figure 1
Figure 1
Schematic illustration of the synthesis of perovskite oxide/ferrite core–shell nanostructures.
Figure 2
Figure 2
Elemental distributions in core–shell nanoparticles (CSNP) via TEM color map show (a) sample area for high-angle annular dark-field (HAADF) imaging. Elemental mapping of (b) only Ba atoms, (c) only Fe atoms, and (d) both Fe and Ba atoms.
Figure 3
Figure 3
(a) TEM-EDX showing Fe and Ba intensities at the region of interest for the quantitative analysis (yellow line) and (b) normalized intensity along the yellow line.
Figure 4
Figure 4
XRD diffraction data of oxidized CSNP that were synthesized from low (s1) and high (s2) initial concentration of FeCl3·6H2O. (a) Bragg peak from crystalline BaTiO3, references were shifted in vertical scale, (b) zoomed in near (220) peak of maghemite, and (c) zoomed in near (311) peak of maghemite.
Figure 5
Figure 5
(a) Background-subtracted XPS scan of the BaTiO3/iron oxide CSNP. (b) Sherley background-subtracted high-resolution scan data of the Fe 2p3/2 orbital deconvoluted without surface peaks.
Figure 6
Figure 6
Field dependence of magnetization for the CSNP at (a) 300 K and (b) 5 K. Inset in the figure shows the low field fragment of the hysteresis loop. Scaling of the vertical axis is different (micro vs. milli) in (a) and (b).

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