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Degradation of Methylene Blue Dye in the Presence of Visible Light Using SiO2@α-Fe2O3 Nanocomposites Deposited on SnS2 Flowers

Semiconductor materials have been shown to have good photocatalytic behavior and can be utilized for the photodegradation of organic pollutants. In this work, three-dimensional flower-like SnS2 (tin sulfide) was synthesized by a facile hydrothermal method. Core-shell structured SiO2@α-Fe2O3 nanocomposites were then deposited on the top of the SnS2 flowers. The as-synthesized nanocomposites were characterized by X-ray diffraction (XRD), Raman spectroscopy, field emission scanning electron microscopy (FE-SEM), transmission electron microscopy (TEM), X-ray photoelectron spectroscopy (XPS), UV–Vis Spectroscopy, Brunauer–Emmett–Teller (BET) surface area analysis, and photoluminescence (PL) spectroscopy. The photocatalytic behavior of the SnS2-SiO2@α-Fe2O3 nanocomposites was investigated by observing the degradation of methylene blue (MB). The results show an effective enhancement of photocatalytic activity for the degradation of MB especially for the 15 wt % SiO2@α-Fe2O3 nanocomposites on SnS2 flowers.


Introduction
Environmental pollution is largely caused by the willful disposal of waste and toxic pollutants without proper treatment. Increasingly, this leads to soil and water degradation, which is deleterious to human health [1,2]. In order to rectify this problem, a variety of processes have been adopted to remove pollutants from wastewater, including adsorption [3], oxidation [4], reduction, and flocculation [5]. Among these various methods, photocatalysis has shown good potential for the removal of organic pollutants [6][7][8]. It has been reported that a number of semiconductors can be used to degrade a variety of organic pollutants using irradiation of light with different wavelengths [9,10]. When compared with other organic compounds, dyes are the most tested substrates in photocatalytic degradation under solar light, because dyes are considered as the common industrial pollutants, and their concentrations can be easily monitored using a UV-Vis spectrometer. However, the dyes also absorb light, especially in the visible range, the influence of this photo absorption by dyes should be excluded from the evaluation of the real photocatalytic activity of photocatalysts. Among the various dyes, methylene blue (MB) is a heterocyclic aromatic compound, which is poisonous and highly dangerous and causes breathing hazards, vomiting, hyperhidrosis, and mental disorders [11,12]. Many researchers have focused on thiazine dyes with a dominance of methylene blue, and 37% of published papers reported on the photodegradation of MB dye [13,14].
There are several semiconductor materials that have been used for the promotion of photocatalytic activity. Among these, ecofriendly iron oxide (α-Fe 2 O 3 ) nanomaterials exhibit favorable photocatalytic activity [15] due to their high specific surface area and high crystallinity, and they have the additional advantage of being low cost [16,17]. Hematite (α-Fe 2 O 3 ) is the most stable iron oxide under ambient conditions, and due to its narrow band gap, it can act as a visible light photocatalyst [18]. This makes α-Fe 2 O 3 a good potential candidate for a photocatalyst, yielding an enhancement of quantum efficiency when irradiated by visible light [9]. Nowadays, many researchers have tried to improve the photocatalytic behavior of Fe 2 O 3 by coupling it with different semiconductor metal oxide nanoparticles, nanotubes, and nanoflowers [19,20]. Metal sulfide semiconductors [21], such as SnS 2 , usually have high light absorption qualities in the visible and shorter wavelengths near the infrared (IR) regions [22]. SnS 2 has also been used as an n-type semiconductor due to its low band gap value of 2.2 eV [23]. Tin sulfide is also widely used as an energy material due to its simple binary composition and the abundance of tin and sulfur [24,25]. It is often used in research because of its unique physicochemical properties with low toxicity and good chemical stability and because it is inexpensive [26]. In addition, with its unique multilayer flower-like structure, SnS 2 exhibits superior photocatalytic degradation of MB under visible light [27].
In this research, SiO 2 nanoshells were used to maintain the structure of the nanocomposites and also to avert their aggregation during photocatalytic reactions [28,29]. This is very important in order to ensure the imperishability of the photocatalyst [30]. The preference of SiO 2 for the inner core is based on the following two considerations: First, the silica nanospheres can produce multiple reflections of the visible light irradiated into the internal cavity [31]; second, the well-ordered and smooth structure of SiO 2 promotes the adsorption of dye molecules to the semiconductor material [32,33]. Also, the SiO 2 nanospheres are possessing large active sites that enable easy access of pollutants and, consequently, to improve the catalytic activity when the TiO 2 and Fe 2 O 3 nanoparticles are deposited on the SiO 2 nanospheres [34][35][36].
We report a simplified approach for the synthesis of SnS 2 -SiO 2 @α-Fe 2 O 3 nanocomposites by means of the hydrothermal method. The photocatalytic activity of the SnS 2 -SiO 2 @α-Fe 2 O 3 nanocomposites was examined for the degradation of MB under irradiation by visible light. Additionally, samples with different weight percentages of SiO 2 @α-Fe 2 O 3 on the SnS 2 flowers were studied to find the optimal ratio for the best photocatalytic activity.

Synthesis of Flower-Like SnS 2
SnS 2 flowers were prepared through a facile hydrothermal method using the same procedure as reported previously [37]. In brief, the procedure for the synthesis of the SnS 2 flowers is as follows: 0.45 g SnCl 4 ·5H 2 O and 0.33 g thioacetamide (TAA) were dissolved in 30 mL isopropyl alcohol. After 30 min of vigorous stirring, the solution was transferred to a Teflon-lined stainless-steel autoclave with a volume of 50 mL and then transferred to a muffle furnace where a hydrothermal was applied Materials 2018, 11, 1030 3 of 17 treatment at 180 • C for 24 h. The golden colored precipitates were then centrifuged and rinsed with copious amounts of deionized water and ethanol before being dried in a vacuum for 12 h at 80 • C.

Synthesis of SiO 2 @α-Fe 2 O 3 Composite Spheres
In this experiment, silica spheres were synthesized using the same procedure described in our previous work [38]. A mixture of tetraethyl orthosilicate (TEOS) (5 mL), anhydrous ethanol (25 mL), and (5 mL) water was stirred at room temperature for 30 min, followed by the addition of 1 mL of ammonia solution. Next, 15 mL of anhydrous ethanol was added to the above mixture, which was stirred for 12 h at room temperature. After centrifugation, the SiO 2 was collected and washed several times with water and ethanol. Finally, the obtained SiO 2 spheres were dried in a vacuum oven at 60 • C for 12 h. Using ultrasonication, 100 mg of SiO 2 spheres were uniformly dispersed in 40 mL of water, followed by the addition of 50 mg iron (III) chloride hexahydrate and 30 mg urea. The mixture was continuously stirred at 95 • C for 6 h. The FeOOH-coated SiO 2 spheres were separated by centrifugation and then washed several times with water and ethanol. Finally, the spheres were dried in a vacuum oven at 60 • C for 12 h. The resulting FeOOH-coated SiO 2 composite spheres were calcined at 450 • C for 4 h to get crystalline α-Fe 3 O 4 nanoparticles.

Degradation of MB Dye
The as-synthesized SnS 2 -SiO 2 @α-Fe 2 O 3 (SSF-15 wt %) nanocomposites (40 mg) were dispersed in 100 mL of 5 ppm MB dye solution and stirred at 30 min in the dark. The reaction dye solution was then irradiated under visible light. A 410 nm LED light (Shenzhen Run lite Tech., Shenzhen, China; T2835-0.06W, 12V DC) was placed on the top of the sample bottle used as a visible light source. A 5 mL sample was taken every 15 min, and the degradation was monitored by using UV-Vis spectroscopy. The proceeding degradation of MB obtained by using α-Fe 2 O 3 , SnS 2 , and SiO 2 @α-Fe 2 O 3 were observed to check on the photocatalytic activity.

X-Ray Diffraction
The crystalline nature of the obtained samples was confirmed by XRD. The XRD results for the as-prepared SnS 2 and SnS 2 -SiO 2 @α-Fe 2 O 3 (SSF-X) (X = 5, 10, 15, 20, and 25 wt %) are shown in Figure 1. The inset to the figure shows the set of peaks at 28.29 • , 32.2 • , 41.8 • , 50.1 • , 52.5 • , and 55.2 • , which can be indexed to the pure hexagonal phase of SnS 2, as confirmed by JCPDS 75-0367 [39]. A peak at 23 • confirms the amorphous SiO 2 , and the peak appearance at 33 • and 35.8 • corresponds to α-Fe 2 O 3 in Figure S1. After the addition of various concentrations of SiO 2 @α-Fe 2 O 3 to the SnS 2 flowers, the intensity of the SnS 2 decreased due to the deposition of the SiO 2 @α-Fe 2 O 3 nanocomposites. Figure 1 clearly shows the 2θ peak at 32.2 • , which corresponds to the (011) diffraction planes indexed to the (011) crystalline SnS 2, which in turn decreased with an increase in the concentration of the SiO 2 @α-Fe 2 O 3 nanocomposites on SnS 2 , confirming the deposition of SiO 2 @α-Fe 2 O 3 nanocomposites. 23° confirms the amorphous SiO2, and the peak appearance at 33° and 35.8° corresponds to α-Fe2O3 in Figure S1. After the addition of various concentrations of SiO2@α-Fe2O3 to the SnS2 flowers, the intensity of the SnS2 decreased due to the deposition of the SiO2@α-Fe2O3 nanocomposites. Figure 1 clearly shows the 2θ peak at 32.2°, which corresponds to the (011) diffraction planes indexed to the (011) crystalline SnS2, which in turn decreased with an increase in the concentration of the SiO2@α-Fe2O3 nanocomposites on SnS2, confirming the deposition of SiO2@α-Fe2O3 nanocomposites.

FE-SEM Structure
The structural morphologies of SnS2, α-Fe2O3, and SnS2-SiO2@α-Fe2O3 were studied using FE-SEM. The flower-like morphology of the as-prepared SnS2 can be clearly observed in the FE-SEM images. This morphology is produced by the accumulation of several nanosheets assembled at one solitary point. Interestingly, the uniform nanosheet morphology is primarily caused by the intrinsic anisotropic growth of SnS2 crystals [37]. The size of each nanosheet is about 20 nm, and the size of the full flower-like structure is in a range between 3 and 4 µ m, as shown in Figure 2a. In the SnS2-SiO2@α-Fe2O3 composites, α-Fe2O3 nanoparticles are deposited on the surface of SiO2 spheres with a size of around 150 nm, as shown in Figure 2b. The SiO2@α-Fe2O3 nanocomposites rest on the surface of the SnS2 flowers, as shown in Figure 2c. The SiO2 core-shell structure allows the multiple reflections of visible light, and the α-Fe2O3 and SnS2 are used to enhance the absorbance sites. An energy dispersive X-ray Analysis (EDX) observations confirmed the presence of SnS2-SiO2@α-Fe2O3 composites. The EDX results give energy peaks congruent with the elements of Sn, S, Fe, O, and Si in Figure 2d.

FE-SEM Structure
The structural morphologies of SnS 2 , α-Fe 2 O 3 , and SnS 2 -SiO 2 @α-Fe 2 O 3 were studied using FE-SEM. The flower-like morphology of the as-prepared SnS 2 can be clearly observed in the FE-SEM images. This morphology is produced by the accumulation of several nanosheets assembled at one solitary point. Interestingly, the uniform nanosheet morphology is primarily caused by the intrinsic anisotropic growth of SnS 2 crystals [37]. The size of each nanosheet is about 20 nm, and the size of the full flower-like structure is in a range between 3 and 4 µm, as shown in Figure 2a

TEM
The detailed structural and morphological properties of as-prepared SnS2 and nanocomposites were examined by transmission electron microscopy (TEM). Figure 3 shows the TEM images of assynthesized flower-like SnS2 (a). The SiO2@α-Fe2O3 nanospheres are arranged on the surface of SnS2 flowers (b). This clearly indicates that the SiO2@α-Fe2O3 nanocomposites are observed on the SnS2 flower, still maintains the flower like structure.

TEM
The detailed structural and morphological properties of as-prepared SnS 2 and nanocomposites were examined by transmission electron microscopy (TEM). Figure 3 shows the TEM images of as-synthesized flower-like SnS 2 (a). The SiO 2 @α-Fe 2 O 3 nanospheres are arranged on the surface of SnS 2 flowers (b). This clearly indicates that the SiO 2 @α-Fe 2 O 3 nanocomposites are observed on the SnS 2 flower, still maintains the flower like structure. Materials 2018, 11, x FOR PEER REVIEW 6 of 17

XPS
To further confirm the elements, their composition, chemical bonding, and oxidation state of the materials, we used X-ray photoelectron spectroscopy (XPS). Figure 4a is the XPS survey spectrum of SnS2-SiO2@α-Fe2O3 (SSF-15 wt %) nanocomposite. This demonstrates that the corresponding signals of the main elements Sn, S, Si, O, and Fe were present in the composite. Figure 4b-f shows the highresolution XPS spectra of Sn 3d, S 2p, O 1s, Fe 2p, and Si 2p. In Figure 4b, the distinctive peaks at 496.7 and 488 eV correspond to the binding energies of Sn 3d5/2 and Sn 3d3/2, respectively, indicating the Sn 4+ oxidation state of Sn [40]. Figure 4c shows the enlarged XPS spectrum of S-contained peaks at 161.2 and 163.4 eV, ascribed to the binding energies of S 2p3/2 and S 2p1/2, showing the presence of S in S 2− state [41]. In the high-resolution XPS spectrum of O in Figure 4d, the typical peaks at 531.6 and 533.4 could be assigned to O 1s having O in O 2− state [42]. Figure 4e shows the narrow-scan XPS spectrum of Fe 2p having binding energies at 711.3, 715.9, and 718.3 eV, assigned to the Fe 2p3/2, satellite peak and Fe 2p1/2, respectively [43,44]. The peaks at binding energy 103.6 and 105.1 eV correspond to Si 2p3/2 and Si 2p1/2 of Si 4+ in SiO2 [45]. From the XPS results, the successful formation of a SnS2-SiO2@α-Fe2O3 nanocomposite can be proved by the binding energies of each element.

XPS
To further confirm the elements, their composition, chemical bonding, and oxidation state of the materials, we used X-ray photoelectron spectroscopy (XPS). Figure 4a is the XPS survey spectrum of SnS 2 -SiO 2 @α-Fe 2 O 3 (SSF-15 wt %) nanocomposite. This demonstrates that the corresponding signals of the main elements Sn, S, Si, O, and Fe were present in the composite. Figure 4b-f shows the high-resolution XPS spectra of Sn 3d, S 2p, O 1s, Fe 2p, and Si 2p. In Figure 4b, the distinctive peaks at 496.7 and 488 eV correspond to the binding energies of Sn 3d 5/2 and Sn 3d 3/2 , respectively, indicating the Sn 4+ oxidation state of Sn [40]. Figure 4c shows the enlarged XPS spectrum of S-contained peaks at 161.2 and 163.4 eV, ascribed to the binding energies of S 2p 3/2 and S 2p 1/2 , showing the presence of S in S 2− state [41]. In the high-resolution XPS spectrum of O in Figure 4d, the typical peaks at 531.6 and 533.4 could be assigned to O 1s having O in O 2− state [42]. Figure 4e shows the narrow-scan XPS spectrum of Fe 2p having binding energies at 711.3, 715.9, and 718.3 eV, assigned to the Fe 2p 3/2 , satellite peak and Fe 2p 1/2 , respectively [43,44]. The peaks at binding energy 103.6 and 105.1 eV correspond to Si 2p 3/2 and Si 2p 1/2 of Si 4+ in SiO 2 [45]. From the XPS results, the successful formation of a SnS 2 -SiO 2 @α-Fe 2 O 3 nanocomposite can be proved by the binding energies of each element.

XPS
To further confirm the elements, their composition, chemical bonding, and oxidation state of the materials, we used X-ray photoelectron spectroscopy (XPS). Figure 4a is the XPS survey spectrum of SnS2-SiO2@α-Fe2O3 (SSF-15 wt %) nanocomposite. This demonstrates that the corresponding signals of the main elements Sn, S, Si, O, and Fe were present in the composite. Figure 4b-f shows the highresolution XPS spectra of Sn 3d, S 2p, O 1s, Fe 2p, and Si 2p. In Figure 4b, the distinctive peaks at 496.7 and 488 eV correspond to the binding energies of Sn 3d5/2 and Sn 3d3/2, respectively, indicating the Sn 4+ oxidation state of Sn [40]. Figure 4c shows the enlarged XPS spectrum of S-contained peaks at 161.2 and 163.4 eV, ascribed to the binding energies of S 2p3/2 and S 2p1/2, showing the presence of S in S 2− state [41]. In the high-resolution XPS spectrum of O in Figure 4d, the typical peaks at 531.6 and 533.4 could be assigned to O 1s having O in O 2− state [42]. Figure 4e shows the narrow-scan XPS spectrum of Fe 2p having binding energies at 711.3, 715.9, and 718.3 eV, assigned to the Fe 2p3/2, satellite peak and Fe 2p1/2, respectively [43,44]. The peaks at binding energy 103.6 and 105.1 eV correspond to Si 2p3/2 and Si 2p1/2 of Si 4+ in SiO2 [45]. From the XPS results, the successful formation of a SnS2-SiO2@α-Fe2O3 nanocomposite can be proved by the binding energies of each element.

EIS Spectra
The EIS spectra were obtained for the different SnS2-SiO2@α-Fe2O3 (SSF-X) (X = 5, 10, 15, 20, and 25 wt %) nanocomposite samples with a modified glassy carbon electrode (GCE) for the KCl (0.1 M) containing 5 mM of [Fe(CN)6] 3− and [Fe(CN)6] 4− . This EIS spectrum shows the electrical and interfacial properties of the aforementioned nanocomposite materials. The SSF-15 wt % nanocomposite produces a smaller semi-circle in comparison to the other composites. In Figure 5, the smallest semicircle, with a reduced diameter, indicates very low resistance. The electron transfer resistance observed is 154, 149, 150, 145, and 101 kΩ −1 for the various 25, 20, 15, 10, and 5 wt % composites, respectively. The low resistance observed for the SSF-15 wt % nanocomposite is due to the counterpart (stoichiometric) ratio between SnS2 and SiO2@α-Fe2O3. The deposition of SiO2@α-Fe2O3 on the SnS2 flowers plays an important role in enhancing the charge resistance, due to the low specific capacity of the nanocomposites. This increased electrical conductivity can also extend the lifespan of the charge carriers, as well as increase the reduction in the electron-hole recombination rate. It is also worth noting that higher impedance values were observed for the 15 wt % of SiO2@α-Fe2O3 nanocomposites, as opposed to all of the other nanocomposites.

EIS Spectra
The EIS spectra were obtained for the different SnS 2 -SiO 2 @α-  Figure 5, the smallest semi-circle, with a reduced diameter, indicates very low resistance. The electron transfer resistance observed is 154, 149, 150, 145, and 101 kΩ −1 for the various 25, 20, 15, 10, and 5 wt % composites, respectively. The low resistance observed for the SSF-15 wt % nanocomposite is due to the counterpart (stoichiometric) ratio between SnS 2 and SiO 2 @α-Fe 2 O 3 . The deposition of SiO 2 @α-Fe 2 O 3 on the SnS 2 flowers plays an important role in enhancing the charge resistance, due to the low specific capacity of the nanocomposites. This increased electrical conductivity can also extend the lifespan of the charge carriers, as well as increase the reduction in the electron-hole recombination rate. It is also worth noting that higher impedance values were observed for the 15 wt % of SiO 2 @α-Fe 2 O 3 nanocomposites, as opposed to all of the other nanocomposites.

UV-Vis DRS Spectra
The broad optical absorption capabilities in the entire visible light spectrum in Figure 6, which is commonly defined in the wavelength range of 400-700 nm, imply that all composites are efficient visible light-sensitive photocatalysts. The SSF-15 wt % indicates that composites have strong and broader absorption in the visible light region, suggesting their potential capabilities effectively utilize visible light energy. This can be attributed to the synergetic effect between SnS2 and α-Fe2O3 nanocomposites. Consequently, the composition SSF-15 wt % enhanced the absorption in the visible light region, which may lead to a higher photocatalytic activity when compared with other weight percentage compositions.

UV-Vis DRS Spectra
The broad optical absorption capabilities in the entire visible light spectrum in Figure 6, which is commonly defined in the wavelength range of 400-700 nm, imply that all composites are efficient visible light-sensitive photocatalysts. The SSF-15 wt % indicates that composites have strong and broader absorption in the visible light region, suggesting their potential capabilities effectively utilize visible light energy. This can be attributed to the synergetic effect between SnS 2 and α-Fe 2 O 3 nanocomposites. Consequently, the composition SSF-15 wt % enhanced the absorption in the visible light region, which may lead to a higher photocatalytic activity when compared with other weight percentage compositions.

UV-Vis DRS Spectra
The broad optical absorption capabilities in the entire visible light spectrum in Figure 6, which is commonly defined in the wavelength range of 400-700 nm, imply that all composites are efficient visible light-sensitive photocatalysts. The SSF-15 wt % indicates that composites have strong and broader absorption in the visible light region, suggesting their potential capabilities effectively utilize visible light energy. This can be attributed to the synergetic effect between SnS2 and α-Fe2O3 nanocomposites. Consequently, the composition SSF-15 wt % enhanced the absorption in the visible light region, which may lead to a higher photocatalytic activity when compared with other weight percentage compositions.

FTIR Spectra
The FTIR spectra of the SnS 2 flowers, SiO 2 spheres, and α-Fe 2 O 3 and SnS 2 -SiO 2 @α-Fe 2 O 3 nanocomposites are shown in Figure 7. The inset to the figure shows the distinctive peaks at 1535 cm −1 and 1657 cm −1 representative of the SnS 2 . A strong stretching vibration of Si-O-Si at 1111 cm −1 , a symmetric vibration of the Si-O-Si at 800 cm −1 , and a symmetric stretching vibration of the Si-OH bond at 956 cm −1 and 3246 cm −1 can be observed. An absorption peak in the range between 3245 and 3450 cm −1 appears for all the samples after they have been annealed at 450 • C due to the stretching vibration of the OH band, which indicates the presence of the -OH group [38]. As the percentage of SiO 2 @α-Fe 2 O 3 increases from low to high, there is not much variation in the FTIR spectra. However, the stretching vibrations, which are observed for all the samples, confirm the presence of OH groups. The bands observed at 474 cm −1 and 572 cm −1 are due to the Fe-O metal oxide stretching vibration modes, while the peak at 1052 cm −1 indicates the presence of the Fe-OH group. The FTIR spectra of the SnS2 flowers, SiO2 spheres, and α-Fe2O3 and SnS2-SiO2@α-Fe2O3 nanocomposites are shown in Figure 7. The inset to the figure shows the distinctive peaks at 1535 cm −1 and 1657 cm −1 representative of the SnS2. A strong stretching vibration of Si-O-Si at 1111 cm −1 , a symmetric vibration of the Si-O-Si at 800 cm −1 , and a symmetric stretching vibration of the Si-OH bond at 956 cm −1 and 3246 cm −1 can be observed. An absorption peak in the range between 3245 and 3450 cm −1 appears for all the samples after they have been annealed at 450 °C due to the stretching vibration of the OH band, which indicates the presence of the -OH group [38]. As the percentage of SiO2@α-Fe2O3 increases from low to high, there is not much variation in the FTIR spectra. However, the stretching vibrations, which are observed for all the samples, confirm the presence of OH groups. The bands observed at 474 cm −1 and 572 cm −1 are due to the Fe-O metal oxide stretching vibration modes, while the peak at 1052 cm −1 indicates the presence of the Fe-OH group.  Figure 8 shows the Raman spectra for the SnS2-SiO2@α-Fe2O3 (SSF-X) (= 5, 10, 15, 20, and 25 wt %) nanocomposites observed in the range of 100 to 1000 cm −1 . The Raman spectrum for SnS2 exhibits an intense peak at about 315 cm −1 , which is attributed to the A1g mode [46,47] (Figure 8 [inset]). Increasing the concentration of SiO2@α-Fe2O3 produces no change in the SnS2 flower-like structure, as shown in Figure 8. For comparison, the Raman spectra of SiO2 and SiO2@α-Fe2O3 are shown in Figure S2.  Figure 8 shows the Raman spectra for the SnS 2 -SiO 2 @α-Fe 2 O 3 (SSF-X) (X = 5, 10, 15, 20, and 25 wt %) nanocomposites observed in the range of 100 to 1000 cm −1 . The Raman spectrum for SnS 2 exhibits an intense peak at about 315 cm −1 , which is attributed to the A1 g mode [46,47] (Figure 8 [inset]). Increasing the concentration of SiO 2 @α-Fe 2 O 3 produces no change in the SnS 2 flower-like structure, as shown in Figure 8. For comparison, the Raman spectra of SiO 2 and SiO 2 @α-Fe 2 O 3 are shown in Figure S2.

BET Surface
The surface areas of the as-synthesized SnS2-SiO2@α-Fe2O3 (SSF-X) (X = 5, 10, 15, 20, and 25 wt %) composites are characterized by nitrogen adsorption-desorption Brunauer-Emmett-Teller (BET) analysis, as shown in Table 1. From the results of BET analysis, the specific surface areas of SSF-X (X = 5, 10, 15, 20, and 25 wt %) are calculated to be 41.61, 39.41, 42.8, 41.93, and 40.47 m 2 /g, respectively. From the above results, it can be seen that the surface area of SSF-15 is slightly higher among all specimens. This implies that the enhancement of the adsorption capacity occurred in SSF-15, compared to that of the plain SnS2 flowers.  Figure 9, shows the PL spectra of SnS2-SiO2@α-Fe2O3 (SSF-X) (X = 10, 15, and 25 wt %) nanocomposites. The board peak at 600 nm indicates the emission band of SnS2 flower-like structure. After deposition of various concentrations of SiO2@α-Fe2O3 nanocomposites on SnS2, the peak at 600 nm is decreased, indicating the reduction of the recombination rate of electron-hole pairs. The SSF-15 wt % shows minimum intense PL spectra and demonstrates the efficient charge separation of the composites, as shown in Figure 9. This lower excitonic of PL intensity is due to the stronger capacity

BET Surface
The surface areas of the as-synthesized SnS 2 -SiO 2 @α-Fe 2 O 3 (SSF-X) (X = 5, 10, 15, 20, and 25 wt %) composites are characterized by nitrogen adsorption-desorption Brunauer-Emmett-Teller (BET) analysis, as shown in Table 1. From the results of BET analysis, the specific surface areas of SSF-X (X = 5, 10, 15, 20, and 25 wt %) are calculated to be 41.61, 39.41, 42.8, 41.93, and 40.47 m 2 /g, respectively. From the above results, it can be seen that the surface area of SSF-15 is slightly higher among all specimens. This implies that the enhancement of the adsorption capacity occurred in SSF-15, compared to that of the plain SnS 2 flowers.  After deposition of various concentrations of SiO 2 @α-Fe 2 O 3 nanocomposites on SnS 2 , the peak at 600 nm is decreased, indicating the reduction of the recombination rate of electron-hole pairs. The SSF-15 wt % shows minimum intense PL spectra and demonstrates the efficient charge separation of the composites, as shown in Figure 9. This lower excitonic of PL intensity is due to the stronger capacity of dopants to capture photo-induced electrons, increase the separation rate of photoinduced electrons and holes, and increase photocatalytic activity. Further, a decrease in the light emission intensity indicates the direct radiative recombination and lower recombination of generated carriers. This result shows that a significant reduction in the recombination rate of photogenerated electron-hole pairs is observed in SSF-15 wt % when compared with other nanocomposites. The SSF-15 wt % composite has the lowest full width at half maximum (FWHM) value of 93.23 compared to that of SSF-10 wt % (99.61) and 25 wt % (105.67), respectively. The lowest FWHM value of SSF-15 wt % demonstrated the longer lifetime of the electron-hole pair and thus has the best intrinsic photocatalytic property.   Figure 10a, b show the process of MB dye degradation after exposure to visible light irradiation in the presence of SnS2 and SnS2-SiO2@α-Fe2O3 (SSF-15 wt %) photocatalysts. The UV-visible absorption spectrum shows a peak at 664 nm, as was observed for the MB dye in Figure 10a,b. When irradiation time was increased, the absorption intensity of the peak at 664 nm decreased, which confirms the progress of the degradation of the MB dye used as a synthesized photocatalyst. For the 15 wt % SnS2-SiO2@α-Fe2O3 sample, complete degradation of the MB dye took only 100 min.  Furthermore, the photodegradation activities of SnS2-SiO2@α-Fe2O3 (SSF-X) with different concentrations of SiO2@α-Fe2O3 were analyzed. The degradation efficiency SSF catalyst with 5, 10, and 15 wt % SiO2@α-Fe2O3 increased as 47%, 62%, 96%, respectively. Upon increasing the concentration as 20 and 25 wt %, the degradation efficiency was decreased to 58% and 53 %, respectively, as shown in Figure 11. It might be due to the accumulation of SiO2@α-Fe2O3 on SnS2 that reduces the penetration of light into the photocatalyst and generates the larger amount of photon adsorbed on the catalyst surface. Hence, the SSF-15 wt % of the SiO2@α-Fe2O3 is an appropriate amount for the excellent photodegradation of the MB solution.  Dye degradation efficiencies of 19%, 42%, 48%, and 96% were observed for the α-Fe2O3, SnS2, and SiO2@α-Fe2O3 and SnS2-SiO2@α-Fe2O3 (SSF-15 wt %) nanocomposites, respectively, at 100 min. The degradation of phenol (25 ppm) was also carried out in order to evaluate the catalytic activity of the Furthermore, the photodegradation activities of SnS 2 -SiO 2 @α-Fe 2 O 3 (SSF-X) with different concentrations of SiO 2 @α-Fe 2 O 3 were analyzed. The degradation efficiency SSF catalyst with 5, 10, and 15 wt % SiO 2 @α-Fe 2 O 3 increased as 47%, 62%, 96%, respectively. Upon increasing the concentration as 20 and 25 wt %, the degradation efficiency was decreased to 58% and 53%, respectively, as shown in Figure 11. It might be due to the accumulation of SiO 2 @α-Fe 2 O 3 on SnS 2 that reduces the penetration of light into the photocatalyst and generates the larger amount of photon adsorbed on the catalyst surface. Hence, the SSF-15 wt % of the SiO 2 @α-Fe 2 O 3 is an appropriate amount for the excellent photodegradation of the MB solution. Furthermore, the photodegradation activities of SnS2-SiO2@α-Fe2O3 (SSF-X) with different concentrations of SiO2@α-Fe2O3 were analyzed. The degradation efficiency SSF catalyst with 5, 10, and 15 wt % SiO2@α-Fe2O3 increased as 47%, 62%, 96%, respectively. Upon increasing the concentration as 20 and 25 wt %, the degradation efficiency was decreased to 58% and 53 %, respectively, as shown in Figure 11. It might be due to the accumulation of SiO2@α-Fe2O3 on SnS2 that reduces the penetration of light into the photocatalyst and generates the larger amount of photon adsorbed on the catalyst surface. Hence, the SSF-15 wt % of the SiO2@α-Fe2O3 is an appropriate amount for the excellent photodegradation of the MB solution.    Dye degradation efficiencies of 19%, 42%, 48%, and 96% were observed for the α-Fe 2 O 3 , SnS 2 , and SiO 2 @α-Fe 2 O 3 and SnS 2 -SiO 2 @α-Fe 2 O 3 (SSF-15 wt %) nanocomposites, respectively, at 100 min. The degradation of phenol (25 ppm) was also carried out in order to evaluate the catalytic activity of the SnS 2 -SiO 2 @α-Fe 2 O 3 nanocomposite ( Figure S3). In the presence of visible-light irradiation, the samples were taken at equal time intervals. The decrease in the distinct peak of phenol at 270 nm indicates the decomposition of phenol. This reveals the effective photocatalytic degradation of phenol done by the SnS 2 -SiO 2 @α-Fe 2 O 3 nanocomposite. Therefore, the degradation of dye is related to the photocatalytic activity of SnS 2 -SiO 2 @α-Fe 2 O 3, rather than to the sensitization of dye.

Dye Degradation
decline in the recombination of e−/h+ pairs, while the charge separation efficiency is increased. Therefore, an efficient charge separation may occur through the strong interfacial interaction in the SnS2/SiO2@α-Fe2O3 heterostructures, reducing the photogenerated charge recombination rate and improving the photocatalytic activity. The α-Fe2O3 nanoparticles used to trap electrons enhance the photocatalytic activity. Due to the reaction between these trapped electrons and dissolved oxygen in the system, the superoxide radical anions (O2 •− ) are formed, which in turn result in the formation of hydroxyl radicals (•OH). These •OH radicals are principally responsible for the oxidation of the organic compounds. This mechanism can be observed in terms of the active surface sites on the catalyst surface and the contact area of the dye and the catalyst. The 15 wt % concentration in SiO2@α-Fe2O3 nanocomposites increases the number of active sites, which in turn increases the number of hydroxyls (•OH) and superoxide (O2 •− ) radicals. Furthermore, degradation efficiency is reduced when the concentration of nanocomposites exceeds the normal range. This may be due to the agglomeration of the nanocomposites, which reduces the penetration of light, as well as the absorbance of the dye and the catalyst. In Figure 12b, the plot of ln(C/Co) vs time shows that the photocatalytic degradation of MB follows the pseudo-first-order kinetics. The rate constant-k value for the SnS2-SiO2@α-Fe2O3 composite is 1.96 × 10 −2 min −1 , which is about 8, 4, and 3 times greater than that for α-Fe2O3 (2.01 × 10 −3 min −1 ), SnS2 (4.43 × 10 −3 min −1 ), and SiO2@α-Fe2O3 (6.12 × 10 −3 min −1 ). The sudden increase in rate constant (k) between 90 and 100 min was due to the gradual rise in pH of the reaction medium (7.1-10.3). The oxidation potential, physicochemical, and surface charge properties of the catalyst were affected by the pH of the solution. The alkaline medium favored (i.e., the formation of •OH by the influences of OH − ions on the surface of the catalyst) the decolorization of the dye more than the acidic medium [49,50]. The highest photocatalytic activity was attained with the SSF-15 wt % nanocomposite. Hence, we can prove that the as-synthesized nanocomposite heterostructures enhance the photocatalytic activity. In photocatalytic oxidation reactions, there are several reactive species, such as •OH, O2 •− , holes, and electrons involved in the reaction. To examine the contribution The enhancement of the photocatalytic activity of the SnS 2 -SiO 2 @α-Fe 2 O 3 (SSF-15 wt %) photocatalyst can be explained by two causes. First, the nanocomposites are prepared by a hydrothermal method having a higher surface area. Secondly, SSF-15 wt % has a very low impedance value in the EIS Nyquist plot. Here, the SiO 2 spheres act as large adsorption sites and good locations for holding the α-Fe 2 O 3 nanoparticles and adsorbing the dye molecules. During the photocatalytic reaction, the SnS 2 and α-Fe 2 O 3 act as photoactive centers and require a strong interaction between the dye and the surface of the catalyst for the effective degradation of dye [21,48]. Furthermore, the CB of α-Fe 2 O 3 is slightly more negative, while the VB is much more positive than that of SnS 2 . This increases the driving force of holes migration when compared to electron transfer. This leads to a decline in the recombination of e−/h+ pairs, while the charge separation efficiency is increased. Therefore, an efficient charge separation may occur through the strong interfacial interaction in the SnS 2 /SiO 2 @α-Fe 2 O 3 heterostructures, reducing the photogenerated charge recombination rate and improving the photocatalytic activity. The α-Fe 2 O 3 nanoparticles used to trap electrons enhance the photocatalytic activity. Due to the reaction between these trapped electrons and dissolved oxygen in the system, the superoxide radical anions (O 2 •− ) are formed, which in turn result in the formation of hydroxyl radicals (•OH). These •OH radicals are principally responsible for the oxidation of the organic compounds. This mechanism can be observed in terms of the active surface sites on the catalyst surface and the contact area of the dye and the catalyst. The 15 wt % concentration in SiO 2 @α-Fe 2 O 3 nanocomposites increases the number of active sites, which in turn increases the number of hydroxyls (•OH) and superoxide (O 2 •− ) radicals. Furthermore, degradation efficiency is reduced when the concentration of nanocomposites exceeds the normal range. This may be due to the agglomeration of the nanocomposites, which reduces the penetration of light, as well as the absorbance of the dye and the catalyst. In Figure 12b, the plot of ln(C/Co) vs time shows that the photocatalytic degradation of MB follows the pseudo-first-order kinetics. The rate constant-k value for the SnS 2 -SiO 2 @α-Fe 2 O 3 composite is 1.96 × 10 −2 min −1 , which is about 8, 4, and 3 times greater than that for α-Fe 2 O 3 (2.01 × 10 −3 min −1 ), SnS 2 (4.43 × 10 −3 min −1 ), and SiO 2 @α-Fe 2 O 3 (6.12 × 10 −3 min −1 ). The sudden increase in rate constant (k) between 90 and 100 min was due to the gradual rise in pH of the reaction medium (7.1-10.3). The oxidation potential, physicochemical, and surface charge properties of the catalyst were affected by the pH of the solution. The alkaline medium favored (i.e., the formation of •OH by the influences of OH − ions on the surface of the catalyst) the decolorization of the dye more than the acidic medium [49,50]. The highest photocatalytic activity was attained with the SSF-15 wt % nanocomposite. Hence, we can prove that the as-synthesized nanocomposite heterostructures enhance the photocatalytic activity. In photocatalytic oxidation reactions, there are several reactive species, such as •OH, O 2 •− , holes, and electrons involved in the reaction. To examine the contribution of these species, tertiary butyl alcohol (t-BuOH), potassium persulfate (K 2 S 2 O 8 ), acrylamide (AA), and ethylenediaminetetraacetic acid (EDTA) were used as scavenger materials for •OH, electrons, O 2 •− , and the holes, respectively, in the reaction process ( Figure 12c). The degradation efficiency slightly decreased when the addition of K 2 S 2 O 8 showed that the electrons play a minimal role in the photocatalytic reaction. The degradation rate of MB further decreased with the addition of AA, indicating reduced involvement of the O 2 •− species. The degradation efficiency reduced during the addition of t-BuOH, which shows the partial involvement of •OH. The rate of MB degradation was significantly affected by EDTA, clearly indicating that holes play a major role in the photocatalytic degradation reaction. To prove the stability and durability of the SnS 2 -SiO 2 @α-Fe 2 O 3 nanocomposite photocatalyst, the recycle experiments were carried out (Figure 12d). Moreover, the results show that only 9.75% of degradation efficiency was lost during the third cycle, which proves that the SnS 2 -SiO 2 @α-Fe 2 O 3 nanocomposites possessed higher stability and reusability efficiency ( Figure S4).

Conclusions
Flower-like SnS 2 and SnS 2 -SiO 2 @α-Fe 2 O 3 nanocomposites with different weight percentages were successfully synthesized using a simple hydrothermal method. The SSF-15 wt % nanocomposites have higher catalytic activity than other samples. The as-prepared nanocomposites enhanced the amount of adsorption of cationic dye (MB) molecules with the addition of SiO 2 @α-Fe 2 O 3 composites on the SnS 2 flowers, thereby increasing the photocatalytic degradation activity. Due to the simplicity of preparation, it is possible to produce a low-cost photocatalyst with higher activity and stability, making it a good candidate material for applications in environmental purification. Based on our results, it should be noted that •OH, O 2 •− , and the holes played a vital role and enhanced the photocatalytic reaction.