In this paper, we report the synthesis of zinc indium sulfide (ZnIn2S4) microspheres synthesized via a low-temperature route, and the as-synthesized material was used for photocatalytic degradation of malachite green (MG), methyl orange (MO), and Direct Red 80 (DR-80) dyes. The as-synthesized material was characterized by powder X-ray diffraction and field-emission scanning electron microscopy for studying the crystal structure and surface morphology, respectively. Fourier transform infrared spectroscopy was performed to determine the functional groups attached. UV-Visible absorption spectrometry was done for light absorbance and band gap analysis, and Mott-Schottky analysis was performed to determine the nature and flat band potential of the material. A scavenger study was performed to analyze the active species taking part in the degradation process. The reusability of the material was tested up to four cycles to check the reduction in efficiency after each cycle. A time-correlated single-photon counting study was performed to observe the average lifetime of generated excitons during photocatalysis. It was found that the as-synthesized porous sample is more efficient in degrading the cationic dye than anionic dyes, which is further explained in the article.
In this paper, we report the synthesis of zinc indium sulfide (ZnIn2S4) microspheres synthesized via a low-temperature route, and the as-synthesized material was used for photocatalytic degradation of malachite green (MG), methyl orange (MO), and Direct Red 80 (DR-80) dyes. The as-synthesized material was characterized by powder X-ray diffraction and field-emission scanning electron microscopy for studying the crystal structure and surface morphology, respectively. Fourier transform infrared spectroscopy was performed to determine the functional groups attached. UV-Visible absorption spectrometry was done for light absorbance and band gap analysis, and Mott-Schottky analysis was performed to determine the nature and flat band potential of the material. A scavenger study was performed to analyze the active species taking part in the degradation process. The reusability of the material was tested up to four cycles to check the reduction in efficiency after each cycle. A time-correlated single-photon counting study was performed to observe the average lifetime of generated excitons during photocatalysis. It was found that the as-synthesized porous sample is more efficient in degrading the cationic dye than anionic dyes, which is further explained in the article.
Increasing environmental pollution is
one of the major problems
for the whole world, in which the percentage of water pollution is
much greater.[1−3] In a survey by World Bank, nearly one-fifth of water
pollution comes from textile industries, which generates more waste
containing mainly dyes, during their manufacturing and dyeing processes.
The wastewater of synthetic textile industries shows low biodegradability
and strong color, whichhave features associated with the dyes, organic
pollutants, and other toxic chemicals. These chemical effluents accumulate
in water bodies, inhibiting photosynthesis, by which the production
of carcinogenic and mutagenic byproducts occur, which cause severe
harmful effects to the environment as well as living organisms.Direct Red 80 (DR-80) and methyl orange (MO) are among a large
group of synthetic industrial dyes, whereas malachite green (MG) is
an aniline-based dyestuff (a triphenylmethane salt) made by Dobner
and Fisher in 1877 that is available in the market. MG, MO, and DR-80
are mostly used for dyeing, printing of textiles, and killing of parasites
and fungi in fish tanks. As a dyestuff, all of these dyes are soluble
in water bodies and can cause lung cancer, colorectal cancer, asthma,
kidney damage, and other diseases directly or indirectly. These anionic
dyes are categorized in the azo class, which is the largest group
of synthetic industrial dyes, and exhibit coloration because of the
presence of certain functional groups in their molecular structure
such as chromophores (−N=N−) and auxochromes
(SO3–, =O).[4−8]According to the literature survey, several
methods have been used
to remove the chemical effluents containing dyes due to their potential
damage to the environment. Physical, chemical, and biological processes
such as adsorption, microbial decomposition, and enzymatic decomposition
have been used for a few decades to degrade these dyes. These processes
exhibit certain inefficiencies, as they usually demand high cost and
much time or generate toxic and carcinogenic intermediate products.
Hence, the effective and alternate method for the degradation of these
effluents is photocatalysis, which is a low-cost and lesser time-consuming
and eco-friendly process, as it uses the solar spectrum {E = hν} to generate free radicals such as •OH and •O in the presence of photons
that oxidize the effluents, which breaks these complex dyes into environment
friendly byproducts.[9]In this context,
a lot of work has been performed on photocatalysis
using various micro- and nanostructured catalysts, such as ZnO and
TiO2, which are the most popular photocatalysts but have
limited application due to their wide band gap (3.2 eV). This lies
in the UV region utilizing only 5% of the solar spectrum. According
to many reports, the efficiency of a photocatalyst can be enhanced
by changing the morphology, surface area, band gap, and many other
parameters.[10] Similarly, other materials
such as cadmium and lead chalcogenide have been studied extensively
during the past two decades.[11−15] Despite their exciting properties, they have limited applications,
due to the toxicity of cadmium and lead. Therefore, the ternary ABpCq
materials (A = Cu, Zn, and Ag, etc., B = Al, Ga, and In, etc., C =
S, Se, and Te) and quaternary Cu2XYZ4-type materials
(X = Mn, Fe, Co, Ni, and Zn, Y = Al, Ga, In, Si, Ge, and Sn, and Z
= S, Se, and Te) semiconductors are receiving attention as promising
alternatives.[16−20]These types of semiconductors have been extensively studied
because
of their unique optoelectronic and catalytic properties.[21−24] Among these compounds, zinc indium sulfide as one of the AB2C4 families has attracted considerable attention
because of its high potential for application in photocatalysis, charge
storage, and thermoelectricity.[25−33] Many dyes have been degraded previously using zinc indium sulfide
(ZnIn2S4) under visible light, but no reports
are present on photocatalytic degradation of MG and DR-80 dyes using
ZnIn2S4. Some of the reported results are mentioned
in Table .
Table 1
Reported Results on Photocatalytic
Degradation of Various Dyes Using ZnIn2S4 Materials
ZnIn2S4 is an interesting material for photocatalysis.
It is a direct semiconductor with band gap energies reported for different
structures, sizes, and shapes of micro- and nanoparticles lying between
2 and 3 eV.[43,49] ZnIn2S4 can be crystallized in two morphologies such as cubic and hexagonal
lattices. The cubic ZnIn2S4 lattice structure
exhibits remarkable thermoelectric properties,[33] while the hexagonal ZnIn2S4 lattice
variation shows photoluminescence and photoconductivity. Both polymorphs
are photocatalytically active materials.[38,50]In this article, we present the low-temperature solution method
synthesis of hexagonal ZnIn2S4 microspheres
and its ability to act as photocatalyst for the reduction of organic
dyes in the aqueous solution. The microspheres were synthesized with
a fixed amount of zinc, indium, and sulfur precursors. The structural
and optical properties and photocatalytic activity on MG, MO, and
DR-80 were studied.
Synthesis of ZnIn2S4 Microspheres
All chemicals used were analytical grade.
In a normal reaction, ZnSO4.7H2O (4.0 mmol)
and In2(SO4)3 (4.0 mmol) were added
by stoichiometric ratio, and
thioacetamide C2H5NS (TAA) (20.0 mmol) was mixed
in a conical flask with 250 mL capacity containing 80 mL of distilled
water. Then the conical flask was put into a water bath and maintained
at 80 °C for 6 h after sealing it with a ground glass stopper.
After completing the reaction, the conical flask was cooled to room
temperature. The yellowish precipitate was collected and washed with
deionized water, absolute ethanol, and acetone several times. The
final sample was dried in a vacuum oven at 60 °C for 6 h; the
powder was collected for characterization, and further photocatalytic
studies were performed. Figure shows the synthesis of ZnIn2S4.
Figure 1
Schematic diagram
of the synthesis of ZnIn2S4 microspheres.
Schematic diagram
of the synthesis of ZnIn2S4 microspheres.
Characterizations
X-ray powder diffraction
(XRD) was
performed with a XRD Smart Lab Guidance Rigaku diffractometer (40
kV, 40 mA) using Cu Kα X-ray radiation (λ = 1.5418 Å)
at a scanning rate of 0.02 deg/s. The obtained pattern was used to
analyze the phase constituents in samples. UV–vis spectra were
obtained with a Varian Cary 500 UV–vis–NIR spectrometer
to analyze the energy band gap using the Tauc plot. The Mott–Schottky
plot was obtained to find the flat band potential (EFB) using Metrohm auto lab. The scanning electron microscopy
(SEM) images were captured on a Zeiss Sigma field-emission scanning
electron microscope (FE-SEM), at an accelerating voltage of 10 kV
to examine the morphology of the obtained sample. Energy-dispersive
X-ray spectrometry (EDX) was carried out to analyze the chemical composition
using an EDX spectrometer attached to the same microscope. Fourier
transform infrared spectroscopy (FTIR) was analyzed using Vertex 70
V, Bruker spectrometer to study the functional groups and bond structure.
Time-correlated single-photon counting (TCSPC) was performed on a
Horiba DeltaFlex-01-DD measurement spectrometer to evaluate the lifetime
of charge carriers at an excitonic emission wavelength of 401 nm.
The biexponential kinetic model was used to fit the decay curves of
the sample, and the best fitting was done with χ2 equal to 2.712. All of the measurements were carried out at room
temperature.
Photocatalytic Activity Measurement
The photocatalytic
degradation activity of hexagonal structure-type material ZnIn2S4 was performed in an aqueous solution on anionic
and cationic dyes such as anionic MO, DR-80, and cationic MG in the
presence of sunlight. In this activity, each dye such as MO, MG, and
DR-80 was taken (10 ppm) separately in three different 250 mL capacity
beakers with 20 mg of ZnIn2S4 containing 100
mL of distilled water. Before irradiation, the solution was stirred
in the dark for 30 min to ensure the establishment of an adsorption
and desorption equilibrium. During irradiation, nearly 2–3
mL of the suspension was collected, centrifuged, and filtered through
a Millipore filter to separate the photocatalyst particles. The filtrate
was placed on a Varian Cary 500 Scan UV–Vis–NIR spectrophotometer
to analyze the absorption peaks at a maximum absorption wavelength
of dye. The abatement percentage of the dye concentration is described
as C/C0, where C is the value of the absorption peak point of dye at each
irradiated time interval and C0 is the
value of the absorption peak point of the dye when adsorption and
desorption equilibrium was achieved.
Results and Discussion
Structural
Analysis
The XRD pattern of the sample prepared
at 80 °C for 6 h is shown in Figure . The diffraction peaks of the 2θ angle
at 21°, 27.6°, 30.1°, 39.5°, 47.2°, 52.2°,
and 55.6° correspond to the (006), (102), (104), (108), (110),
(116), and (022) planes of hexagonal ZnIn2S4 (JCPDS No. 03-065-2023), respectively, and a small diffraction peak
of 2θ angle at 33.6° (shown in Figure through a letter c) corresponds to the (400)
plane of cubic ZnIn2S4 (JCPDS No. 00-048-1778).
Crystallographic planes of hexagonal ZnIn2S4 (JCPDS No. 03-065-2023) and cubic ZnIn2S4 (JCPDS
No. 00-048-1778) indicate the formation of nearly pure hexagonal ZnIn2S4. The particle size of the as-synthesized microsphere
was calculated by Scherrer’s formula using eq .[51]where D (nm) symbolizes the crystallite size of a particular hkl plane, λ is the Cu Kα radiation wavelength
of X-ray radiation (λ = 1.540 Å), β denotes the full
width at half-maxima (FWHM) of the hkl plane peak,
and θ (radian) denotes Bragg’s diffraction angle.
Figure 2
XRD patterns
of ZnIn2S4 microspheres.
XRD patterns
of ZnIn2S4 microspheres.In the hexagonal lattice, the relationship between interplanar
spacing d of hkl planes and the lattice constants a and c is as shown in eq .The lattice constants a and c of ZnIn2S4 microspheres were calculated
using
(006) and (110) planes, as shown in Table . The calculated lattice parameters agreed
with the standard values a = 3.85 Å and c = 24.68 Å corresponding to the hexagonal ZnIn2S4 sample.
Table 2
Lattice Constants
(a, c) and Average Crystallite Size
(D) for ZnIn2S4 Microspheres
sample
a (Å) (lattice constant)
c (Å) (lattice constant)
crystallite
size (Dhkl) (nm) average
d-spacing
ZnIn2S4
25.50
4.91
d006 = 4.25
3.94
d110 = 1.92
Surface Morphology
The FE-SEM images of ZnIn2S4 microspheres
are shown in Figure a–c, which show clear microsphere
morphologies containing nanoflower-like petals around it in Figure b. Microspheres look
like puffy flowers with densely packed petals. The average dimensions
of microspheres have a ∼1 μm radius and ∼18 nm
thick petals, as clear from the Figure c.
Figure 3
(a–c) Low- and high-resolution SEM images of ZnIn2S4 microspheres. (d) EDX spectra of ZnIn2S4 microspheres.
(a–c) Low- and high-resolution SEM images of ZnIn2S4 microspheres. (d) EDX spectra of ZnIn2S4 microspheres.Energy-dispersive X-ray spectroscopy was used to check the chemical
composition of the as-synthesized sample ZnIn2S4 shown in Figure d. The EDX spectra verified the existence of Zn, In, and S elements
in the ZnIn2S4 microsphere. The chemical composition
mapping of the ZnIn2S4 microsphere is given
in Table .
Table 3
Composition Analysis of ZnIn2S4 Microspheres
element
weight concentration
(%)
atomic concentration
(%)
Zn
5.11
4.92
In
64.48
35.37
S
30.40
59.71
UV–Visible Absorption
and Band Gap
Optical absorption
and band gap of the prepared sample were analyzed by UV–vis
absorption spectroscopy using a Varian Cary 500 UV–Vis–NIR
spectrometer. The UV–Vis absorption spectra were plotted in
terms of absorption versus wavelength (nm), as shown in Figure a, and the Tauc plot (hν vs (αhν)2) of the prepared sample ZnIn2S4 microsphere
is shown in Figure b, where h is the Planck constant (h = 6.626 × 10–34 J·s), ν is the
frequency, and α is the absorption constant, defined as α
= 2.303A/t, where A and t are absorbance
and thickness of the cuvette, respectively. The band gap of the ZnIn2S4 microspheres was estimated as Eg = 2.1 eV with the help of a Tauc plot.
Figure 4
(a) UV–vis absorption,
(b) Tauc plot, and (c) Mott–Schottky
(MSK) plot of ZnIn2S4.
(a) UV–vis absorption,
(b) Tauc plot, and (c) Mott–Schottky
(MSK) plot of ZnIn2S4.To understand the process of charge transfer in the ZnIn2S4 microsphere semiconductor and the flat band potential
(EFB), the Mott–Schottky (MSK)
analysis was performed. The EFB was obtained
by extrapolating the positive slope of the MSK plot to the x-axis, as shown in Figure c, and the positive slope of the as-synthesized photocatalyst
depicts the n-type electronic nature of the semiconductor. Hence,
due to the n-type nature, the degradation efficiencies of the cationic
dyes are much better than those of anionic dyes, which can be seen
through rate kinetic studies, as well, in Figure . The value of the EFB was obtained as 1.7 V versus the normal hydrogen electrode
(NHE).
Figure 5
FTIR spectra of ZnIn2S4 microsphere.
Figure 6
Time-dependent UV–vis spectra of different dyes
using 20
mg of ZnIn2S4 photocatalyst (a–c) dark
reaction of ZnIn2S4 with DR-80, MG, and MO,
respectively, (d) MO, (e) MG, and (f) DR-80. (g) C/C0 versus time graph of the three dyes.
(h) Photodegradation kinetics.
FTIR spectra of ZnIn2S4 microsphere.Time-dependent UV–vis spectra of different dyes
using 20
mg of ZnIn2S4 photocatalyst (a–c) dark
reaction of ZnIn2S4 with DR-80, MG, and MO,
respectively, (d) MO, (e) MG, and (f) DR-80. (g) C/C0 versus time graph of the three dyes.
(h) Photodegradation kinetics.The position of the conduction band edge potential ECB and the valence band edge potential EVB for the ZnIn2S4 microsphere was
calculated by using the Butler and Ginley equation, as given below
in eqs and 4.[52]where X represents the absolute
electronegativity of the semiconductor determined as the geometrical
mean of electronegativity of the constituent atoms (i.e, XZnIn = 4.84), Ee (4.5 eV) represents the free electron’s energy
on the hydrogen (H2) scale, and Eg represents the band gap energy of the semiconductor. The
obtained values of XZnIn, Ee, Eg, EVB versus NHE, and ECB versus NHE corresponding to ZnIn2S4 are presented in Table and Figure .
Table 4
Energy Band Structure Parameters of
As-Synthesized ZnIn2S4 Microsphere
XZnIn2S4
EFB
Ee (eV)
band gap Eg (eV)
EVB (eV) vs NHE
ECB (eV) vs NHE
4.84
–1.7
4.5
2.1
1.39
–0.71
Figure 8
Proposed mechanism of photocatalytic degradation and charge transfer.
Optical Studies
FTIR analysis was carried out to find
the functional groups and impurities, attached to the surface of the
catalyst, as shown in Figure . A broad strong peak present at 3400–3550 cm–1 represents OH and NH stretching vibrations. Peaks present at 2922
and 2852 cm–1 represent aliphatic CH stretching
vibration of CH, CH2, or CH3. The peak at 1635
cm–1 was assigned to the deformation vibration of
N–H. The C=C stretching vibration occurs at 1650–1450
cm–1. The peak present at 1161 cm–1 occurs due to the hydroxyl group. FTIR spectra confirm that our
synthesized sample does not contain any impurity contents.
Photocatalytic
Activity
An absolute study of as-synthesized
material ZnIn2S4 with three different dyes,
i.e., MO, MG, and DR-80, was conducted to test the photocatalytic
behavior and the degradation efficiencies of organic dyes, as shown
in Figure .The procedure to study photocatalytic behavior is as follows. First,
the dark reaction (in the absence of light) was performed using DR-80
aqueous dye solution, such that ZnIn2S4 catalyst
was allowed to react with the dye in the absence of light. The UV–vis
absorption spectra were calculated for time t = 0
and 30 min in the dark, as shown in Figure a–c. It was clear from the figure
that there was no change in the absorption intensity even after 30
min, confirming that the degradation does not occur in the dark due
to the surface adsorption phenomenon.Figure d–f
(abs/time) illustrates the photocatalytic degradation of MO, MG, and
DR-80, respectively, using 20 mg of ZnIn2S4 and
10 ppm dyes in 100 mL of deionized water. The samples were collected
at t = 0, 15, 30, 45, 60, 75, and 90 min to study
the time-dependent photocatalytic activities.The C/C0 versus time
graph is plotted as shown in Figure g. It is observed that the cationic dye MG is more
degraded than anionic dye MO and azo dye DR-80. The C/C0 is the ratio of absorbance intensity
at any recorded time (say, t = 0, 15, 30, 45, 60,
75, and 90 min) to the absorbance intensity at zero time (t = 0 min). Here, the photocatalytic degradation process
follows the first-order rate kinetics as defined by the given eqs , 6, and 7.where C stands
for the intensity of absorbance at any recorded time (t), C0 is the initial intensity of absorbance
at time (t = 0 min) and k is the
rate constant of reaction. The rate constant k was
determined by plotting a graph between −ln(C/C0) versus time (t)
and by drawing the corresponding slope. The rate constants were observed
to be 0.55, 0.199, and 0.065 min–1 for MO, MG, and
DR-80, respectively, using 20 mg of the catalysts and 10 ppm of the
above-mentioned dyes, as shown in Figure h.As obvious from Figure , ∼57.54, 99.68, and
90.79% of the dyes (MO, MG, and
DR-80, respectively) were degraded in the first 30 min using ZnIn2S4 photocatalyst, and from the rate constants,
it was also observed that the ZnIn2S4 photocatalyst
was more active for the cationic group, such as MG, than for the anionic
group, such as MO and DR-80.
Figure 7
Comparative efficiencies of the three dyes MO,
MG, and DR-80 using
20 mg of ZnIn2S4 and 10 ppm dyes.
Comparative efficiencies of the three dyes MO,
MG, and DR-80 using
20 mg of ZnIn2S4 and 10 ppm dyes.The photocatalytic degradation efficiency was calculated
using
the following formula, as shown in eq .where η is degradation
efficiency, C is the intensity at a recorded time
(t), and C0 is the intensity
at time (t = 0 min).The photocatalytic degradation
efficiencies (η) were 99.43%
for MO, 99.68% for MG, and 99.12% for DR-80 within 90, 30, and 75
min, respectively, as shown in Figure , using 20 mg of ZnIn2S4 photocatalyst
and 10 ppm dyes in 100 mL of DI water.
Scavenger Study and Degradation
Mechanism
Active species
trapping experiment was performed to get a deep insight into the primary
and secondary species responsible for the degradation of MG, MO, and
DR-80 dyes during the photocatalysis process. Different scavengers
like tetrabutanol (TBA) for •OH, 1,4-benzoquinone (BQ) for
•O2–, and potassium iodide (KI) for both •OH and h+ were used in this experiment. As can be seen from Figure , the TBA
and KI have a least considerable effect on the degradation process,
suggesting •OH and h+ as secondary species in the
degradation, whereas BQ shows a great impact on the degradation process,
suggesting •O2– as the main primary species helping in the degradation
process.
Figure 9
Scavenger study of zinc indium sulfide microsphere photocatalysts
using BQ, KI, and TBA scavengers.
Proposed mechanism of photocatalytic degradation and charge transfer.Scavenger study of zinc indium sulfide microsphere photocatalysts
using BQ, KI, and TBA scavengers.The ZnIn2S4 microspheres, cationic dye MG,
and anionic dyes MO and DR-80 were used to study the mechanism of
photocatalytic degradation, as shown in Figure . When the incident photon, with an energy
equal to or greater than the energy band gap of ZnIn2S4 (Eg = 2.1 eV) (hν ≥ Eg) strikes the surface
of the photocatalyst, the valence band electron (e–) moves toward the conduction band after absorbing energy from incident
photon, leaving behind a hole (h+). Thus it creates an
electron–hole pair. A reaction between hole (h+)
and water (H2O) takes place, yielding hydroxyl radical
(•OH) and H+ ions, as shown in the following eqs , 10, and 11.Similarly, another
reaction between electrons (e–) and oxygen (O2) occur, yielding superoxide radicals.
These radicals react with toxins and reduce them into harmless or
less toxic byproducts, as shown in eqs and 13.
Reusability Study
The reusability and the cyclic stability
are always an important part of the photocatalysts. The stability
and the reusability of the ZnIn2S4 microspheres
were determined for four cycles, as shown in Figure . In the first cycle, the efficiency is
99.32% using 50 mg of ZnIn2S4 in 10 ppm DR-80
dye in 100 mL of solution. Photocatalysts were separated from the
DR-80 dye solution by filtration after each cycle, washed, dried,
and reused in the next cycle. The light irradiation time (30 min),
dye solution quantity, and concentration were kept the same for each
cycle. ZnIn2S4 microspheres possessed good reusability
and showed 70.83% efficiency after four cycles. Such decreased efficiency
was due to waste of photocatalyst during filtration after each cycle.
Therefore, the as- synthesized ZnIn2S4 microsphere
is an effective and stable photocatalyst for the degradation of DR-80
dye.
Figure 10
Cyclic stability of ZnIn2S4 microspheres
in photocatalytic degradation of DR-80 dye for four cycles under visible
light irradiation.
Cyclic stability of ZnIn2S4 microspheres
in photocatalytic degradation of DR-80 dye for four cycles under visible
light irradiation.
Time-Correlated Single-Photon
Counting (TCSPC)
Time-resolved
transient and steady-state decay were analyzed to study the generation,
transfer, and decay of the excitons. Biexponential fitting of the
decay curve (Figure ) was performed using eq , with a least χ2 value of 2.712:To obtain the lifetimes of τ1 and τ2, I(t)
is the intensity, τ1 is the decay times for faster
nonradiative processes, whereas τ2 is the decay time
for slower radiative decay process. It can be seen from Table that τ1 contributes
89.22% to the deactivation of excited states, which suggests that
the degradation process happens due to the nonradiative pathways and
radiative pathways having the very least role in the degradation process
of dyes.
Figure 11
Time-correlated single-photon count spectra of ZnIn2S4.
Table 5
Lifetimes
of Generated Carriers
lifetime (ns)
relative intensities (%)
samples
τ1
τ2
A1
A2
χ2
ZnIn2S4
0.0480152
1.13987
89.22%
10.78%
2.712
Time-correlated single-photon count spectra of ZnIn2S4.
Conclusions and Future Work
An analytical
study was performed to understand the photocatalytic
performance of ZnIn2S4 on malachite green, methyl
orange, and Direct Red-80. The ZnIn2S4 sample
was synthesized using a low-temperature solution method inside a water
bath. Synthesized microspheres were found to be micron size and indicate
the formation of a nearly pure hexagonal ZnIn2S4 structure. Marigold flower-like morphology was obtained, which is
depicted from the FE-SEM micrographs. Photocatalytic performance was
largely dependent on ZnIn2S4 structure, morphology,
and optical characteristics. Degradation efficiency (η) of 99.68,
99.48, and 99.12 in 30, 90, and 75 min for MG, MO, and DR-80, respectively,
was achieved, which makes ZnIn2S4 a potential
candidate for degradation of both anionic and cationic dyes. Band
gap energy calculated using the Tauc plot was Eg = 2.1 eV corresponding to 590 nm wavelength, which makes
the photocatalyst suitable in the visible region. MSK analysis was
done to find the flat band potential of ZnIn2S4. An average crystallite size of 4.91 nm was obtained from XRD analysis.
A reusability study suggests a ∼5–10% decrease in efficiency
after consecutive cycles, where a part of a reduction in efficiency
is due to the quantity of sample decreasing during the collection
process after each cycle. All of these observations and analyses suggest
ZnIn2S4 is a potential and suitable candidate
for degrading both anionic and cationic dyes. In the future, we will
work on the synthesis of ZnIn2S4 with some other
materials to form a Z-scheme and heterostructure-based photocatalysts
to further extend the domain of the photocatalyst in degrading heavy
metals and more complex dyes.