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Structural, optical, magnetic and photoelectrochemical properties of (BiFeO3)1−x(Fe3O4)x nanocomposites
(BiFeO 3 ) 1 −x (Fe 3 O 4 ) x nanocomposites were prepared by dispersion of Fe 3 O 4 nanoparticles (NP) into sol–gel synthesised BiFeO 3 (BFO) matrix followed by calcination at 500 °C. Samples with x = 0.0, 0.2, 0.33 and 0.5 were investigated using X-ray diffractions (XRD), UV–vis spectroscopy, pho...
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Published in: | Journal of sol-gel science and technology 2019-09, Vol.91 (3), p.624-633 |
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Main Authors: | , , , , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | (BiFeO
3
)
1
−x
(Fe
3
O
4
)
x
nanocomposites were prepared by dispersion of Fe
3
O
4
nanoparticles (NP) into sol–gel synthesised BiFeO
3
(BFO) matrix followed by calcination at 500 °C. Samples with
x
= 0.0, 0.2, 0.33 and 0.5 were investigated using X-ray diffractions (XRD), UV–vis spectroscopy, photoluminescence spectroscopy (PL), transmissions electron microscopes (TEM), electron spin resonance (ESR), vibrating sample magnetometer (VSM) and photoelectrochemical (PEC) measurements. Formation of nanocomposites was confirmed by XRD and TEM. The XRD patterns showed presence of both BFO and Fe
3
O
4
phases without any secondary phases. The crystallite size of BFO (39.1–51.1 nm) is much bigger than that of Fe
3
O
4
(10.1–12 nm). Microstrain of BFO decreased for sample
x
= 0.2 and 0.33 and then increased for
x
= 0.5. Optical band gap of samples decreased from 2.5 eV for
x
= 0.0–1.96 eV for sample
x
= 0.5. The PL emission which centred at 428.1 eV for
x
= 0.0 increased gradually for samples
x
= 0.2 and 0.33 and then decreased for
x
= 0.5. Exchange bias (
H
EB
) was observed for hysteresis loops of all samples, and the highest value of
H
EB
was 38.4 Oe for
x
= 0.5. The
g
-values of the nanocomposites, ranged between 2.23 and 2.20, were higher than that of the BFO and Fe
3
O
4
components. The PEC measurement showed the photocurrent density increased with
x
. Finally, modulations of the physical properties of BFO/Fe
3
O
4
system were analysed and discussed in detail.
(a) Low magnification TEM image of (BiFeO
3
)
x
(Fe
3
O
4
)
x
composites showing dispersion of Fe
3
O
4
small particles (some was indicated by white arrow) into BiFeO
3
matrix. (b) PL spectra of sample
x
= 0.5, (c) Top view of PEC setup (where 1 : PC, 2 : Autolab system and 3: halogen lamp) (d) side view of PEC setup (4: PEC cell and 5 : manual chopper) and (e) Photocurrent against voltage under chopped illumination of
x
= 0.5.
Highlights
(BiFeO
3
)
1−
x
(Fe
3
O
4
)
x
composites were successfully synthesised.
Lattice parameter
c
of BFO decreased with increasing Fe
3
O
4
content,
x
.
(BiFeO
3
)
1−
x
(Fe
3
O
4
)
x
composites shows fascinating physical properties, such as exchange bias.
The (BiFeO
3
)
1−
x
(Fe
3
O
4
)
x
composites exhibited reduced optical band gap.
PEC measurement showed the photocurrent density increased with
x
.
The study showed a presence of interaction between the BiFeO
3
and Fe
3
O
4
resulting in modulated physical properties. |
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ISSN: | 0928-0707 1573-4846 |
DOI: | 10.1007/s10971-019-05053-9 |