J Pranesh Shubha1, Syed F Adil2, Mujeeb Khan2, Mohammad R Hatshan2, Aslam Khan3. 1. Department of Chemistry, Don Bosco Institute of Technology, Mysore Road, Bangalore 560 074, India. 2. Department of Chemistry, College of Science, King Saud University, P.O. Box 2455, Riyadh 11451, Saudi Arabia. 3. King Abdullah Institute for Nanotechnology, King Saud University, Riyadh 11451, Kingdom of Saudi Arabia.
Abstract
The ZnO-based ternary heterostructure ZnO/Eu2O3/NiO nanoparticles are synthesized using waste curd as fuel by a simple one-pot combustion method. The as-synthesized heterostructure is characterized by using various spectroscopic and microscopic techniques including X-ray diffraction, UV-vis, FTIR, SEM, and TEM analyses. The photocatalytic activity of the ternary nanocomposite was tested for the photodegradation of methylene blue (MB) under solar light irradiation. The results have revealed that the ternary ZnO/Eu2O3/NiO photocatalyst exhibits excellent performance toward the photocatalytic degradation of the studied dye. Optimization studies revealed that the synthesized heterostructure exhibited a pH-dependent photocatalytic activity, and better results are obtained for specific concentrations of dye and catalysts. Among the different light sources employed during the study, the catalyst was found to possess the best degradation efficiency in visible light.
The ZnO-based ternary heterostructure ZnO/Eu2O3/NiO nanoparticles are synthesized using waste curd as fuel by a simple one-pot combustion method. The as-synthesized heterostructure is characterized by using various spectroscopic and microscopic techniques including X-ray diffraction, UV-vis, FTIR, SEM, and TEM analyses. The photocatalytic activity of the ternary nanocomposite was tested for the photodegradation of methylene blue (MB) under solar light irradiation. The results have revealed that the ternary ZnO/Eu2O3/NiO photocatalyst exhibits excellent performance toward the photocatalytic degradation of the studied dye. Optimization studies revealed that the synthesized heterostructure exhibited a pH-dependent photocatalytic activity, and better results are obtained for specific concentrations of dye and catalysts. Among the different light sources employed during the study, the catalyst was found to possess the best degradation efficiency in visible light.
Semiconductor-based photocatalytic degradation of hazardous dyes
has attracted significant attention of researchers as a potential
tool to solve the rapidly evolving problem of environmental pollution.[1] Particularly, hazardous organic dyes used in
textile industry are considered as dangerous environmental pollutants
due to their strong persistent color and their ability to absorb dissolved
oxygen from water bodies.[2] These types
of synthetic dyes seriously disturb the normal penetration of sunlight
in rivers, which has significant effect on the aquatic organisms due
to reduced photosynthetic activities.[3] Besides,
due to the strong stability, organic pollutants usually survive for
longer time in the environment, which possibly makes them xenobiotic.[4,5] Therefore, untreated textile effluent is potentially hazardous to
both terrestrial and aquatic life by adversely affecting the natural
ecosystem and causing long-term health effects.[6] Hence, a variety of physicochemical and biological processes
have been applied for the degradation of organic dyes, and additionally,
various other methods have also been increasingly explored.[7−12] Still, cost-effective removal of these dyes from effluents remains
a major problem.[13]Recently, advanced oxidation processes have drawn considerable
attention of researchers for the degradation of dyes from effluents.[14] These processes are cost-effective, environmental
friendly, and possess strong ability to degrade a variety of complex
dyes from wastewater. Typically, advanced oxidation processes are
performed by irradiation using solar or ultraviolet light in the presence
of photocatalysts. Further, in many cases, ultrasonication and H2O2 are also used to enhance the rate of degradation
or adsorption of dyes on photocatalysts.[15] Among various catalysts, semiconductor materials, such as Fe2O3, CdS, V2O5, ZnO, TiO2, and so forth, have been prominently used as photocatalysts
for the degradation of organic dyes.[16−18] Particularly, ZnO-based
photocatalysts have drawn considerable attention due to their extensive
usage in the field of environmental remediation.[19,20]Zinc oxide (ZnO) offers excellent benefits including high chemical
stability, excellent biocompatibility, unique electronic structure,
and lower cost.[21] However, the large band
gap and fast recombination of photoinduced charge carriers have mainly
inhibited the practical applications of ZnO. Therefore, to enhance
the charge separation and to extend the response of ZnO toward the
visible light, it is commonly modified by structural doping with both
metallic and nonmetallic elements and also by the formation of heterojunctions
with a second semiconductor component.[22] Especially, the formation of a heterojunction offers promising opportunities
to enhance the separation efficiency of photoinduced charge carriers.[23] So far, a variety of ZnO-based binary and ternary
heterojunctions have been fabricated, such as 2D ZnO/ZnS binary heterostructures,
ternary ZnO/Cu2O/Si nanowire arrays, ternary ZnO–ZnS–Gd2S3 nanostructural arrays, and so on.[24−28]Therefore, for the purpose of photocatalytic degradation of organic
dyes, rationally designed ZnO-based ternary heterojunctions offer
great potential by facilitating the migration of electrons due to
the presence of multicomponent photosystems.[29] These systems effectively extend the lifetime of photogenerated
charge carriers and enhance the scope of light absorption.[23] Due to this, there is continued urge for the
controlled fabrication of ternary heterojunctions. Typically, these
types of systems are prepared by various physical and chemical methods
including sol–gel, chemical vapor deposition, microwave heating,
coprecipitation, and hydrothermal and solvothermal methods.[30] Often, these techniques need high-tech instruments,
long reaction times, and higher temperature; therefore, development
of other facile methods is highly required. Contrarily, solution combustion
is a facile technique, which is low cost, time and energy efficient,
and easy to perform and scale up.[31] In
addition, eco-friendly starting materials can also be effectively
applied in this technique.[32] These benefits
persuaded us to explore the synthesis of ZnO-based ternary heterojunctions
using another photoactive metal oxide and lanthanide element.Our group has been working toward the synthesis of various nanomaterials
and its applications toward catalysis and removal of pollutants.[33−35] In continuation of these efforts, we herein demonstrate the preparation
of ZnO-based ternary ZnO/Eu2O3/NiO heterostructure
nanoparticles (NPs) via a single-step combustion method. The as-prepared
heterostructure NPs have been tested as a photocatalyst for the degradation
of methylene blue (MB) under sunlight (cf. Scheme ). The results indicate that the as-prepared
ternary system demonstrated an improved photocatalytic activity. This
work offers new insights into designing a multicomponent ZnO-based
photocatalyst toward environmental remediation.
Scheme 1
(A) Schematic representation
of the preparation of ZnO/Eu2O3/NiO ternary
heterostructure NPs and (B) scheme illustrating the degradation of
organic dyes (MB).a
(A) Schematic representation
of the preparation of ZnO/Eu2O3/NiO ternary
heterostructure NPs and (B) scheme illustrating the degradation of
organic dyes (MB).a
Results and Discussion
UV–Vis Spectrum
Figure a shows the UV–vis absorption spectrum
of the as-prepared ZnO/Eu2O3/NiO NPs scanned
in the absorption range from 800 to 200 nm. The as-prepared ZnO/Eu2O3/NiO NPs absorption spectrum yields two absorption
bands, one in the UV region at ∼242 nm, which can be ascribed
to the transitions (LMCT) from O2– (2p) to M (3d),[36,37] while another
absorption edge is observed in the visible region at 350 to 370 nm,
which can be assigned to 6A1 + 6A1 to 4T1 + 4T1 transition, termed
as “double-excitation process.”[38−41] This suggests that the prepared
sample is photolytically active in the UV region as well as in the
visible region; moreover, it also indicates the crystalline nature
of the as-prepared oxides.[42] Further, the
band gap energy of NPs has been calculated from the UV–vis
spectra (Figure b)
using Tauc’s equation (eq ) and is found to be 3.69 eV.[36]where Eg is the
band gap energy in eV, α is the absorbance value, ν is
the frequency, h is Planck’s constant, b is a constant, and n is equal to 1/2
and 2 for a direct and indirect transition, respectively. A wide range
of absorption of light helps in effective photocatalytic degradation
and enhances the efficiency.
Figure 1
(a) UV–vis spectrum of ZnO/Eu2O3/NiO.
(b) Band gap calculation graph.
(a) UV–vis spectrum of ZnO/Eu2O3/NiO.
(b) Band gap calculation graph.
X-ray Diffraction
The prepared mixed metal oxides are
subjected to X-ray diffraction (XRD), and the obtained diffractograms
are shown in Figure . A comparative XRD of NiO, ZnO, and Eu2O3 is
also included in this figure. The evaluation of the diffraction pattern
obtained for ZnO/Eu2O3/NiO NPs provides evidence
that the as-prepared heterostructures are crystalline in nature. The
pattern obtained corresponds to the mixture comprising hexagonal and
cubic structures of ZnO, NiO, and Eu2O3. NiO
shows the powder diffraction pattern of NiO with cubic structures
(JCPDS no: 2-1216) with a lattice parameter a = 4.172
Å and with a space group Fm3̅m (no. 225). Cubic Eu2O3 NPs are shown with
a heterostructure (JCPDS no 86-2476), a lattice parameter a = 10.859, and a space group Ia3̅
(no. 206). Moreover, Figure also shows that diffraction pattern obtained for ZnO is similar
to the reference XRD pattern of ZnO obtained from ICSD, which is hexagonal
with the heterostructure (JCPDS no 1-1136) and lattice parameters a = 3.242 Å and c = 5.176 Å,
while the space group is P63mc (no. 186).
Figure 2
XRD patterns of ZnO/Eu2O3/NiO nanostructure
and a comparative ZnO, Eu2O3, NiO, and diffraction
patterns.
XRD patterns of ZnO/Eu2O3/NiO nanostructure
and a comparative ZnO, Eu2O3, NiO, and diffraction
patterns.
FTIR Spectrum
The FTIR spectrum of ZnO/Eu2O3/NiO NPs is displayed in Figure . The FTIR spectrum of a CuO NP shows broad
absorption bands between 2800 and 4000 cm–1, mainly
ascribed to OH– from the hydroxyl group, which is probably
attributed to the adsorbed water on the surface of the nanocrystals
and also to the C–O groups on the surface of the ZnO/Eu2O3/NiO NPs.[43] A peak
at 3614 cm–1 is characteristic to the formation
of the Eu2O3 phase.[44] A peak at ∼1063 cm–1 is due to C=O
stretching of acetate. The characteristic peaks less than 1000 cm–1, that is, 567 and 621 cm–1, can
be attributed to the M–O and M–O–M stretching
modes of vibrational frequencies of metals interlinked by common oxygen
atoms, which are also observed in the FTIR spectrum of ZnO (Figure S2).[45]
Figure 3
FTIR spectrum of ZnO/Eu2O3/NiO.
FTIR spectrum of ZnO/Eu2O3/NiO.
Microscopic Analysis
SEM Analysis
The morphological features of the as-prepared
heterostructure, that is, ZnO/Eu2O3/NiO, are
obtained by field emission scanning electron microscopy (FESEM) analysis,
and the achievement of the nanostructured heterostructure is confirmed
by TEM analysis, and the results obtained are given in Figure . The low-magnification FESEM
image shown in Figure a reveals that ZnO/Eu2O3/NiO is composed of
clusters of particles as well as flakes. Figure b is the high-magnification FESEM image which
shows that part of the material is in the form of flakes in which
all the flakes are interconnected and form a net-like structure with
large pores. Based on the previously reported literature, it can be
assumed that the flake-like morphology could belong to the NiO component
of the heterostructure, while the clusters could be the ZnO and Eu2O3 NPs in the heterostructure.[46]
Figure 4
FESEM images of ZnO/Eu2O3/NiO particles with
(a) low magnification (scale bar of 200 nm) and (b) high magnification
(scale bar of 100 nm).
FESEM images of ZnO/Eu2O3/NiO particles with
(a) low magnification (scale bar of 200 nm) and (b) high magnification
(scale bar of 100 nm).Elemental mappings of bulk ZnO/Eu2O3/NiO
have been collected and displayed in Figure . It shows that the as-prepared heterostructure
contains the desired elemental composition, and the elements are well
dispersed throughout the composition, which can play a synergetic
role in the enhancement of the catalytic performance. Moreover, the
ED spectrum of ZnO/Eu2O3/NiO heterostructure
is given in Figure S1, which designates
that all the expected elements such as Zn, Mn, Eu, and O are present
and the percentage of elemental compositions is displayed in the inset
table, which is in accordance with the stoichiometric amount taken
for the preparation of ZnO/Eu2O3/NiO heterostructure
NPs.
Figure 5
Elemental mappings of the prepared mixed metal oxide NiO/Eu2O3/ZnO indicating the presence of (a) Zn, (b) Eu,
(c) Ni, (d) O, and (e) bulk.
Elemental mappings of the prepared mixed metal oxideNiO/Eu2O3/ZnO indicating the presence of (a) Zn, (b) Eu,
(c) Ni, (d) O, and (e) bulk.
TEM Analysis
Figure shows the TEM images of ZnO/Eu2O3/NiO. Figure a–c
shows the low- and high-magnification images which demonstrate that
the spherical particles are distributed all over the sample as well
as some incidents of agglomerations can be observed. The sizes of
the particles are in the range between 20 and 60 nm. The selected
area electron diffraction pattern (Figure d) indicates the polycrystalline form of
the material, and the reflection planes obtained are very much in
alignment with the information deduced from the XRD pattern.
Figure 6
TEM images of ZnO/Eu2O3/NiO with (a) low
magnification, (b) high magnification showing particles, (c) HRTEM
showing lattice fringes, and (d) electron diffraction image.
TEM images of ZnO/Eu2O3/NiO with (a) low
magnification, (b) high magnification showing particles, (c) HRTEM
showing lattice fringes, and (d) electron diffraction image.
Photocatalytic Analysis
The theory of semiconductor
photocatalysis says that the morphology, band gap, surface area, particle
size, crystalline nature, and amount of hydroxyl ions on the surface
of the photocatalyst determine its strength.[47] The theory explains the formation of an electron and a hole on the
surface of the semiconductor by the absorption of light, and the generated
electrons and holes will take part in the reaction or they do recombine.
If the external surface is provided for the charge carriers, they
will relocate where the electrons are caught by the semiconductor
while the holes are trapped by hydroxyl radicals and form OH• and HO2•. In the case of a ternary
structure, more surface is available for relocation of charge carriers,
and hence, the formed hydroxyl ions are utilized effectively to degrade
MB.As per the results obtained from UV–vis spectroscopy,
it is evident that the heterostructure prepared is active in the UV–vis
region as well as in the visible region. Moreover, the band gap calculated
yielded Eg = 3.79 eV. In order to evaluate
the photocatalytic performance of the heterostructure, that is, NiO/Eu2O3/ZnO, various experiments such as effect of light
source, concentration of MB, load of catalyst, and pH are carried
out and MB is taken as the standard pollutant for photocatalytic degradation
in the study, and the variation of absorption peak intensity recorded
at 663 nm (λmax of MB) is monitored to deduce the
results obtained.For the study, 100 cm3 of an aqueous solution of varying
amounts of MB such as 5, 10, 15, and 20 ppm is taken for degradation
experiments. The amount of as-prepared heterostructure is also varied,
such as 5, 15, 30, and 45 mg of ZnO/Eu2O3/NiO.
The solution is mixed with mixed metal oxide and aerated for 40 min
while kept in the dark. The kinetics of the degradation is studied
by periodically collecting 3 cm3 of the aqueous mixture
as a sample from the solution at intervals of 30 min, which is then
subjected to centrifugation. From the absorbance spectra obtained
by employing UV–vis spectroscopy, the initial (Ci) and final (Cf) dye concentrations
in the system are confirmed and the % of degradation of the dye is
determined by substituting the values obtained in eq .Moreover, when the photocatalytic activity of the as-prepared catalyst,
that is, ZnO/Eu2O3/NiO, is compared with the
individual components of the catalyst, that is, ZnO, Eu2O3, and NiO, it is observed that the degradation of MB
obtained is 66, 40, and 72%, respectively, which is much lower than
the 97% obtained from the use of the as-prepared catalyst, indicating
the synergistic effect of all the three components of the catalyst
on the degradation of MB. The graphical illustration of the degradation
of MB using ZnO, Eu2O3, and NiO is given in Figure S2.
Effect of Light Source
Since the as-prepared heterostructure
is photolytically active in both the UV region and in the visible
region as confirmed from the UV–vis spectra, the first set
of study is designed to confirm the light source that can yield the
best performance of the as-prepared heterostructure. Hence, the photocatalytic
degradation of MB employing ZnO/Eu2O3/NiO NPs
is carried out in three different environments, that is, under sunlight,
UV ray irradiation (wavelength 254 nm), and in the dark. From the
results obtained, it is confirmed that the as-prepared mixed metal
oxide is active under UV irradiation as well as in visible light,
as realized by the UV–vis spectra obtained. However, in the
case of the experiment carried out in the dark, the degradation of
MB is found to be negligible. Moreover, when the degradation results
obtained from the experiments carried out in sunlight and under UV
ray irradiation are compared, the results revealed that degradation
of MB is much more in sunlight than the degradation obtained in UV
ray irradiation. In sunlight, the as-prepared mixed metal oxide NPs
efficiently degrade 97% of MB, which is higher than the 72% degradation
obtained under UV ray irradiation yielded in a reaction time of 150
min. Hence, it is confirmed that the photocatalyst ZnO/Eu2O3/NiO is most effective in sunlight, and all the further
optimization experiments are carried out under sunlight. The degradation
results obtained are illustrated in Figure .
Figure 7
Variation of light source on the degradation of MB.
Variation of light source on the degradation of MB.
Effect of Amount of Catalyst
After the confirmation
of the source of light for the efficient photocatalytic performance
of the as-prepared heterostructure, the optimum amount of catalyst
for the degradation of MB is evaluated by varying the catalyst in
the range 5–40 mg under visible light. A 65% degradation of
MB dye is observed when 5 mg of photocatalyst is used. The amount
of catalyst is increased from 15 to 30 mg, and an increase in the
degradation of MB from 82 to 97% is observed. However, when the amount
of catalyst is increased further to 40 mg, then a decrease of degradation
efficiency of the catalyst is observed and an 80% degradation of MB
is obtained.This reduction in the degradation of MB may be
due to accumulation and sedimentation of the catalyst particles at
higher concentrations, which in turn causes the increase in light
scattering, which results in a decrease in the light path inside the
solution; moreover, the higher concentration of the catalyst may also
cause agglomeration of the photocatalyst, ensuing a decrease in the
number of photocatalytic active sites.[48−50] Hence, the optimum amount
of photocatalyst for efficient degradation of MB is confirmed as 30
mg. The results obtained are graphically illustrated in Figure .
Figure 8
Effect of catalyst amount for the efficient degradation of MB.
Effect of catalyst amount for the efficient degradation of MB.
Effect of Concentration of MB
Further, the efficiency
of the as-synthesized heterostructure, that is, ZnO/Eu2O3/NiO NPs, is evaluated for varying concentrations of
MB in the range of 5–20 ppm under visible light with the amount
of catalyst employed as 30 mg. From the results obtained, it is observed
that the degradation of MB decreased from 96 to 65% when the concentration
of MB is increased from 5 to 20 ppm. This may be attributed to the
decreased absorption of light on the surface of photocatalyst with
an increase in dye concentration, which leads to reduction in the
generation of hydroxyl radicals, playing an important role in the
degradation of MB present in the system. Therefore, it is essential
to increase the suitable concentration of photocatalyst with increased
dye concentration (Figure ).
Figure 9
Effect of dye concentration on the photocatalytic efficiency of
ZnO/Eu2O3/NiO NPs.
Effect of dye concentration on the photocatalytic efficiency of
ZnO/Eu2O3/NiO NPs.
Effect of pH
It is well reported in the literature
that the catalytic efficiency of a photocatalyst is directly related
to the availability of hydroxyl radicals in the solution, which confirms
that the rate of photocatalysis is usually more in alkaline solutions.In order to understand the optimum pH for the efficient performance
of the as-prepared mixed metal oxide, that is, ZnO/Eu2O3/NiO NPs, the pH of the MB solutions is varied from 6 to 10
pH. It is observed that when the reaction condition is pH 6, the degradation
of MB obtained is 78%; however, when the pH is increased, then the
degradation efficiency of the photocatalyst is highly improved and
a 93 and 97% degradation of MB is obtained for pH 7 and pH 10, respectively.
This can be attributed to the generation of higher rate hydroxyl radicals
and due to the accumulation of hydroxyl radicals on the surface of
the catalyst at higher pH (Figure ).[51,52]
Figure 10
Effect of pH on the degradation of MB.
Effect of pH on the degradation of MB.
Comparative Studies
A comparison of the photocatalytic
activity of ZnO/Eu2O3/NiO for the degradation
of MB with that of the previously reported ZnO-based photocatalytic
systems is presented in Table . It is evident that the ternary ZnO/Eu2O3/NiO photocatalyst in the present study showed superior photodegradation
activity than several other catalysts reported in the literature.
Table 1
Comparison of Photocatalytic Activity of ZnO/Eu2O3/Mn3O4 for MB Degradation
with Previously Reported Photocatalysts Containing ZnO NPs
catalyst
MB concentration
light source
catalyst amount
time (min)
degradation (%)
ref.
ZnO/Eu2O3/NiO
5 ppm
sunlight
30 mg
150
98
herein
S–ZnO NPs
20 μM
sunlight
30 mg
45
61.5
(53)
N/La–ZnO
15 ppm
sunlight
50 mg
60
97
(54)
ZnO–SiO2
9 ppm
sunlight
10 mg
90
97.8
(55)
ZnO NWs
10 ppm
sunlight
100 mg/L
4320
100
(56)
WO3/ZnO@rGO
5 ppm
vis. 200 W
10 mg
90
94.1
(57)
Ag–ZnO/GO
15 ppm
Xe 20 W × 5
20 mg
180
85
(58)
TiO2/ZnO/rGO
0.3 ppm
Xe 300 W
0.1 g/L
120
92
(59)
Mn–ZnO
10 ppm
UV lamp
24 mg
90
60
(60)
rGO–ZnO
5 × 10–4 mol/L
vis. light
100 mg/L
120
90
(61)
ZnO–CdO
3 × 10–5 mol/L
Xe 250 W
360
97.8
(62)
ZnO NPs
15 ppm
Hg lamp 10 W
100 mg
120
90
(63)
Ag/ZnO
2 × 10–5 M
Xe 100 W
100 mg
120
76
(64)
ZnO/AC
2 × 10–5 M
Hg lamp, 30 W
25 mg
45
92.2
(65)
Photocatalytic Mechanism
Based on the above experimental
findings, a possible mechanism for the enhanced photocatalytic efficacy
of ZnO/Eu2O3/NiO photocatalyst upon visible
light irradiation is proposed and schematically illustrated in Scheme . Under visible irradiation,
the ZnO/Eu2O3/NiO photocatalyst can be readily
excited, and electron–hole pairs are generated on its surface.
Moreover, due to the presence of Eu3+ in the photocatalyst,
most probably sublevels beneath the conductive band are introduced
and hence enhance the visible light response.[66−68] Hence, the
excited electrons and holes could be efficiently separated, overturning
the potential of charge carrier reunion; consequently, •OH
active radicals are generated from the electrons in the CB over a
two-electron oxidation path,[69,70] which directly decomposes
the organic pollutant, MB dyes. As a result, the photoinduced •OH
and h+ active radicals are responsible for the degradation,
and the plausible mechanism is summed up as follows
Scheme 2
Plausible Photocatalytic Reaction Mechanism for the Photodegradation
of MB in the Presence of ZnO/Eu2O3/NiO NPs under
Visible Light Irradiation
Experimental Methods
Synthesis of ZnO/Eu2O3/NiO
Stoichiometrically
calculated amounts of zinc nitrate, nickel acetate, and europium nitrate,
that is, 48.5 wt % Zn(NO3)2. 6H2O,
48.5 wt % Ni(CH3CO)2, and 3 wt % Eu(NO3)3.5H2O, are dissolved in 10 cm3 of distilled water and 6 cm3 perished curd is added to
it under constant stirring for about 20 min. Subsequently, the thoroughly
mixed mixture is kept in a muffle furnace at 400 °C. After 10
min, a blackish green powder is obtained, which is calcined at the
same temperature for 3 h.
Characterization
The as-synthesized heterostructures
are characterized by XRD, UV–vis, FTIR, FESEM, and TEM. The
XRD characterization is carried out using a Bruker diffractometer
[Cu Kα (λ = 1.5406 Å) X-ray source]. The spectral
characterization is carried out using a PerkinElmer UV–vis
spectrometer and a Bruker IFS 66 v/S spectrometer for UV–vis
and FTIR spectral analysis, respectively. The microscopic analysis
such as SEM is carried out to understand the surface morphology, and
particle size analysis is carried out by FESEM. TEM images are recorded
with a transmission electron microscope, JEOL JEM2100 PLUS, operating
at a 200 kV accelerating voltage.
Conclusions
In conclusion, we report the successful synthesis of ternary heterojunction
ZnO/Eu2O3/NiO mixed metal oxides by a simple
combustion route. The characterization of the as-prepared material
revealed the crystalline nature and nanosize formation of ZnO/Eu2O3/NiO heterostructure. The as-prepared material
is tested as a photocatalyst for the degradation of MB dye, a harmful
industrial effluent. The photocatalyst displayed excellent degradation
efficiency under visible light, and the kinetics of the catalyst revealed
that up to 97% of degradation of MB can be obtained within 150 min
under sunlight. Hence, further studies into the kinetics and fine-tuning
of the economic and eco-friendly catalyst are in progress and shall
be reported in future.