One of the main aspects this review refers to is the approach of how different synthesis methods and experimental parameters affect the photocatalytic properties of SnO2-based materials.
4.1. Pure SnO2-Based Photocatalysts
Besides being synthesized in its pure form, SnO2 has been prepared in its doped form with metals or nonmetal ions, as well as in the form of composites with other semiconductor materials, or even impregnated in inert, non-active photocatalytic materials. It is well known that the generation of electrons/holes (e−/h+) pairs by absorption of a photon of equal energy, to or higher than the band gap energy induced by light, is a basic prerequisite for a semiconductor to be used in photocatalysis. Because of its wide band gap of SnO2 (3.6 eV), no absorption response to the visible light would be achieved, and this is the main disadvantage of this material, which restricts its application in practical devices. A wide variety of pure semiconductor materials, particularly SnO2, have been investigated regarding the photocatalytic properties, but only few of them are considered effective photocatalysts.
Besides the value of the forbidden band energy corresponding to absorption in the visible region, it is required that the energy levels of the conduction and valence bands are suited to the redox potential of the water, so as to produce reactive agents to promote breaking of organic pollutants molecules. Therefore, different authors have employed various synthesis methods and varied experimental conditions in order to change particle characteristics, which include size, morphology, and texture, as well as the crystallinity and the presence of defects, in order to design efficient photocatalysts under UV irradiation. These parameters can play an important role during photocatalysis, as they can affect the adsorptive and photo-absorption capacity of the catalyst, besides reducing photogenerated changes of recombination during photoexcitation. In addition, some authors also explored the reaction mechanisms involved in the photodegradation of the dyes and how the reactive species act for the photocatalysis to occur. These points are discussed throughout the review.
For instance, considering pure tin oxide as a photocatalyst, Akram et al. [
90] prepared SnO
2 nanoparticles by the continuous microwave flow synthesis (CMFS) method in a domestic microwave oven operating at 600 W, using tin chloride pentahydrate (SnCl
4·5H
2O), sodium hydroxide (NaOH), ethanolic solutions. The solutions were pumped through the microwave with the aid of peristaltic pumps to attain 10 min of retention time inside the device. The resulting suspension was filtered, washed, and dried at 80 °C for 12 h, followed by heating at 200 °C for 2 h to obtain SnO
2 samples. The photocatalytic properties of the nanoparticles were investigated toward the photodegradation of Methylene blue (MB) dye under UV irradiation (365 nm). In their study, the authors also investigated the effect of the concentration of the reacting SnCl
4·5H
2O and NaOH materials on the crystallinity, particle size, and morphology, as well as the photocatalytic behavior of the SnO
2 nanoparticles. The authors evidenced that crystalline SnO
2 samples with tetragonal, rutile-type structures were obtained only after heating at 200 °C. The increase in the concentration of SnCl
4·5H
2O (from 0.25 to 0.75 M) and NaOH (from 1 to 3 M) provoked an increase in sample crystallinity and an average particles size from 4.33 to 8.56 nm, with no meaningful change in morphology. This phenomenon was attributed to the increased number of nuclei sites formed by the reacting species, as well as to the microwave irradiation that favors better nucleation and crystal growth. Surprisingly, a decrease of the band gap (
Eg) values from 3.33 to 3.19 eV was also observed as a function of the precursor’s concentration, and it was associated to the increase of the particle size. In relation to the photocatalytic property of the samples, that sample was prepared using the lower concentration of the reacting species, which presented the lowest degree of crystallinity (63%), smallest particle size (4.43 nm), largest surface area (153.57 m
2 g
−1), and widest band gap (3.33 eV), and this was the most efficient in the photodegradation of MB dye, reaching up to 93% of degradation in 240 min. According to the authors, the higher efficiency observed for that sample was mainly due to the large surface area and higher concentration of defects.
Still considering pure tin oxide photocatalysts, Abdelkader et al. [
92] synthesized SnO
2 nanoparticles via a sol-gel method and calcined it at different temperatures (80, 450, and 650 °C) for 4 h, in order to achieve different crystallinity and particle morphology. The authors investigated the photocatalytic efficiency of the synthesized samples toward Congo red (CR) dye degradation under UVA irradiation. For the synthesis of the nanoparticles, tin chloride (SnCl
2 2H
2O) was dissolved in 250 mL of deionized water to obtain a white suspension of a 0.4 M Sn (II) concentration. The suspension was stirred for 1h at room temperature and oxalic acid was added dropwise to the aqueous solution as a chelating agent with a molar ration of 1:1 (oxalic acid: tin cations). The obtained suspension was centrifuged, filtered, and washed several times to eliminate chloride ions. The washed precipitate was dried at 80 °C/24 h and calcined at 450 to 650 °C for 4 h. According to the results, the sample obtained after drying at 80° for 24 h (SnO
2-80) crystallizes in pure tin oxalate (SnC
2O
4) with a monoclinic structure. On the other hand, pure SnO
2 with a
P42/mnm tetragonal, rutile-type structure was obtained after calcinations at 450 (SnO
2-450) and 650 °C (SnO
2-650). The authors draw attention to the use of oxalic acid as a chelating agent, and it affected the particle characteristics for controlling the nucleation and crystal orientation, as well as the calcination temperature in the control of the crystallinity. The authors evidenced that samples calcined at higher temperatures are more aggregated with a foamed aspect because of the smallest particle size of the powders. The samples calcined at different temperatures also presented a specific surface area that varied from 66.41 to 37.54 m
2 g
−1, and with band gap values from 3.35 to 3.49 eV for the SnO
2-450 and SnO
2-650 samples, respectively.
Curiously, regarding the photocatalytic behavior of the samples prepared by Abdelkader et al. [
92], the highest efficiency in the degradation of CR dye (catalyst/CR dye concentration of 0.5 g L
−1) was achieved using SnO
2-650 that presented a lower surface area. This sample presented a dye photodegradation efficiency of 61.53% after 100 min under irradiation. The authors pointed out that the highest efficiency observed for this sample is especially due to its greater crystallinity that gives less surface defects as well as particle aggregation. The lower density of surface defects (Sn
2+ and oxygen vacancies) could reduce recombination of the electron–hole (e
−/h
+) pairs. Because of this fact, the authors proposed the photocatalytic mechanism involved in the CR photodegradation. The reactions mechanism can be represented by Equations (1)–(6). According to the authors, under UVA light, electrons are excited from the VB to the CB of SnO
2 (Equation (1)) and, simultaneously, holes are created in the VB. The photoinduced e
− in the CB can directly reduce Sn
4+ to Sn
2+ (Equation (2)). However, as Sn
4+ can act as a scavenger of e
−, Sn
2+ can influence the photo-reactivity by altering a e
−/h
+ recombination (Equation (3)). The h
+ in the VB is captured by H
2O generating hydroxyl
•OH radicals (Equation (4)). In addition, according to the band energy position, the authors stated that the h
+ in the VB of SnO
2 (+3.50 eV/NHE) is more positive than that of the H
2O/OH couple (+1.9 eV/NHE), which is required for organic pollutant decomposition R/R
•+ (+1 V/NHE), indicating that the photoinduced holes in the VB can oxidize the adsorbed CR dye and H
2O molecules on the SnO
2 surface. Thus, the formation of organic cation-radicals (R
•+) is formed (Equation (5)). As a result, all the O
2•−,
•OH, and R
•+ radicals participate in redox reactions responsible for decomposing CR dye (Equation (6)).
Although most studies concerning photocatalytic degradation of dyes using pure SnO
2 have been performed under UV light, some authors investigated the photocatalytic properties of SnO
2 under visible light and sunlight. For instance, Kumar et al. [
94] reported the use of SnO
2 particles prepared by a simple, eco-friendly, and low-cost biosynthesis process using guava (
Psidium guajava) leaf extract in the photodegradation of Reactive yellow 186 (RY186) dye under sunlight. The authors prepared the samples by mixing a 2.1 M SnCl
4 solution with the extracts in a ratio of 1:1, and kept under stirring at 60 °C for 4 h, followed by calcination at 400 °C for 4 h to obtain SnO
2 nanoparticles. The authors evidenced that the SnO
2 single-phase nanoparticles with a size of 8–10 nm showed a high photocatalytic efficiency, degrading 90% of RY186 dye in 180 min. For the photocatalysis, a concentration of 1 g L
−1 of SnO
2 sample was used. According to the authors, superoxide (O
2•−) and hydroxyl (
•OH) radicals are responsible for the photodegradation of dye. The efficiency of the photocatalyst in the degradation and mineralization of RY186 was confirmed by CO
2 evolution during the photocatalysis, which was analyzed by GC analysis. The authors evidenced the complete mineralization of dye led to CO
2 (0.8 μmol) and H
2O. As the photostability and reusability of the photocatalyst are important aspects, the authors evaluated them by performing five consecutive photocatalytic cycles. The photoactivity of the catalyst remained about constant even up to five experiments, although gradual losses in activity were expected. It is important to highlight that the use of powdered samples in photocatalysis might be disadvantageous due to the loss in the amount of the catalyst after centrifugation and filtration processes, which leads to a loss in photoactivity. However, the authors reinforced that the synthesized catalyst is easily separable from the solution.
Like Kumar et al. [
94], Haq et al. [
78] synthesized tin dioxide (SnO
2) nanoparticles by an eco-friendly process using leaves extracts. However, in the study conducted by Haq et al. [
78]
Daphne mucronata leaf extract was used as a cap** and reducing agent in order to control particle size and morphology. The authors evaluated the photocatalytic performance of the samples toward Rhodamine 6G (R6G) dye degradation using 0.4 g L
−1 of the catalyst. For the materials synthesis, a mixture of a 0.003M SnCl
4·5H
2O solution with 20mL of the leaf extract was kept under 500 rpm and stirring at 55 °C. A greenish gel was obtained after 40 min and aged for 24 h, which was subsequently washed with hot water, filtered, washed with ethanol, and finally dried at 100 °C for 6 h to obtain a fine, colorless powder. The authors obtained nanoparticle samples with an average particle size of 64 nm and specific surface area around 147 m
2 g
−1. A maximum of 99.70% of the dye degradation was observed after 390 min under simulated sunlight. The charge generation and photodegradation mechanism reported by Haq et al. [
78] is the same as the one described by Kumar et al. [
94] for RY186 dye [
94].
Kumar et al. [
94] synthesized SnO
2 nanocrystals by a solution-phase growth technique, and the structural, optical, and photocatalytic properties of the nanostructures were investigated. The effects of reaction temperature (180 and 200 °C), time (24 and 30 h), the use of CTAB (CetylTrimethylAmmonium Bromide) surfactant on the particle size, morphology, and band gap energy were evaluated. According to the authors, the SEM images showed that samples synthesized at 180 °C for 24 (Sample 1) and 30 h without the surfactant (Sample 2) presented particles with a rod-like morphology and crystallite size of 17.12 and 26.51 nm, respectively. When the sample was synthesized at 200 °C for 24 h without surfactant (Sample 3), SnO
2 nanostructures with a nanoflower-like morphology, with crystallite size at 28.25 nm were obtained. On the other hand, the samples prepared at 180 (Sample 4) and 200 °C for 24 h with the addition of CTAB (Sample 5) showed particles with a nanosphere-type morphology with sizes of 23.80 and 32.14 nm, respectively. The band gap (
Eg) values estimated for sample 1 (nanorods), Sample 2 (nanorods), Sample 3 (nanoflowers), Sample 4 (nanospheres), and sample 5 (nanospheres) were 4.05, 3.88, 3.84, 3.95, and 3.76 eV, respectively. The authors associated the variation of the
Eg values mainly to the temperature and time conditions of which the samples were prepared, that directly affected the particle size and morphology and, therefore, impacted photocatalytic activity of the samples. Despite the wide band gap of the samples, the authors evaluated their photocatalytic activity using 0.5 g L
−1 of the catalysts in the degradation of Rhodamine B (RB) dye under direct sunlight irradiation. Surprisingly, the authors observed a high photodegradation of dye under sunlight, and the efficiency of the SnO
2 nanostructures was strongly related to the particles’ morphology. According to the authors, even presenting a
Eg = 3.76 eV, sunlight was enough to promote photoexcitation in Sample 5 to degrade 91.7% of the dye after 2 h. As expected, Sample 1 (SnO
2 nanorods with
Eg = 4.05 eV) displayed the lowest dye degradation efficiency in 2 h (76% of the dye is degraded). The authors established that size, morphology, specific surface area, and dispersion of the catalysts played key role in the photodegradation of the dye.
Assis et al. [
58] used a polymeric precursors method to prepare SnO
2 particles at different temperatures (700, 800, and 900 °C). After being prepared, the powders were impregnated in polystyrene foams in order to increase surface area due to the porous characteristic of polystyrene, besides a favoring for the recovery of the material after use. The photocatalytic property of the samples was investigated in the degradation of RhB dye under UV irradiation with a catalyst/dye concentration of 0.4 g L
−1. The authors observed, using high-resolution transmission electron microscopy (HRTEM), that the SnO
2 samples present nanoparticles with sizes ranging between 20 and 80 nm. Moreover, the formation of agglomerates was observed in the samples calcined at higher temperatures (800 and 900 °C). The oxide obtained at lower temperatures presented a smaller particle size and a larger surface area, which resulted in a greater photocatalytic activity, degrading 98.2% of degradation of the rhodamine RhB after 70 min.
A very conventional synthesis procedure for obtaining oxide-based catalysts is the so-called sol-gel method. Thus, Najjar et al. [
93] synthesized SnO
2 nanoparticles by a green sol-gel method, using chitosan as a polymerizing agent, and calcined it at different temperatures (500, 700, 800, and 1000 °C). The authors also draw attention to the use of chitosan that may increase particle stability, prevent particles aggregation, and reduce the particles’ toxicity. According to the TGA-DTA analysis, the temperature of 700 °C (namely, SnO
2-NPs at 700 °C) proved to be more adequate to prepare the desirable SnO
2 catalyst. The material calcined at this temperature presented a spherical particle morphology with an average size of 10 nm, as observed by TEM analyses. The authors evaluated the photocatalytic properties of SnO
2-NPs at 700 °C toward the photodegradation of Eriochrome black T (EBT), an azo-type anionic dye. The photocatalytic tests were carried out by adding 21.1 mg L
−1 of the catalyst in 100 mL of EBT dye solution (10
−5 M) and kept at a constant stirring and UV irradiation (Hg vapor lamp, 500 W) for 270 min. Regarding the photocatalytic activity of the prepared SnO
2-NPs, a photodegradation efficiency of 77% was obtained after 270 min. In order to investigate the best conditions for optimum dye degradation using SnO
2-NPs, Najjar et al. [
93] also investigated the influence of the catalyst concentration (8.7, 21.1, and 43.2 mg L
−1) and the solution pH (3.5, 5, 7, and 9). The authors observed an increase of the photodegradation rate by increasing the concentration of the photocatalyst from 8.7 to 21.1 mg L
−1, decreasing afterwards. According to the authors, this decrease in photocatalytic efficiency of SnO
2-NPs in a higher concentration is due to the fact of accumulation of nanoparticles that lead to a decrease in the generation of reactive radicals, such as hydroxyls (
•OH). With respect to variation of the solution pH, the highest photodegradation efficiency (77%) was attained at the isoelectric point of SnO
2-NPs at pH 3.5 (Zeta potential = 0 eV). Curiously, the photodegradation of the anionic EBT dye at positive Zeta potential values (at pH 2) was not as expressive as that observed at the isoelectric point of the catalyst.
According to Najjar et al. [
93] the general mechanism involved in the dye photodegradation using SnO
2-NPs is summarized by Equations (7)–(12), that are similar to those reactions displayed in
Figure 1 for a hypothetical catalyst.
As the photostability of the catalyst is an important factor for its reuse in consecutive photocatalytic tests, cyclic experiments of EBT photodegradation were carried out for the SnO
2-NPs under the optimal conditions established in the work. Thus, Najjar et al. [
93] evidenced that the degradation rate of EBT remained over 74% after five cycles. In addition, using FTIR, XRD, TEM, and FESEM analysis, the authors showed that no visible changes were observed in the samples after the fifth cycle, which confirms the high photostability of the synthesized catalyst.
Recently, Luque et al. [
39] synthesized SnO
2 nanoparticles (SnO
2 NPs) by a green synthesis using
Citrus x paradisi extract as a stabilizing cap** agent. There were different concentrations of the extract (1, 2, and 4% in relation to the aqueous medium—SnO
2 NPs-1, 2, and 4%). It is important to highlight that a heating treatment at 400 °C for 1 h was completed to obtain crystallized SnO
2 NPs. The authors obtained crystalline SnO
2 nanoparticles with average sizes of 9.1, 5.1, and 4.7 nm when 1, 2, and 4% of the cap** agent was used in the synthesis, respectively. These samples also presented band gap values (
Eg) of 3.28, 2.77, and 2.69 eV, respectively, which were smaller than those
Eg values reported by Mahmood et al. [
95]. This confirmed the role of this cap** agent in controlling the particles’ size, as well as in the modification of optical band gap properties of SnO
2 NPs. The photocatalytic properties of the samples were then investigated under both solar and UV irradiation using a SnO
2 NPs/dye concentration of 1.0 g L
−1. Furthermore, Methyl orange (MO), Methylene blue (MB) and Rhodamine B (RhB) were used as target dyes. Regarding the photocatalytic efficiency of the SnO
2 NPs, SnO
2 NPs-4% presented the highest efficiency in the degradation of the dyes, degrading 100% of MO after 180 and 20 min under solar and UV irradiation, respectively. In relation to other dyes, SnO
2-NPs-4% degraded 100% of MB and RhB after 60 min under UV irradiation. The efficiency of this photocatalyst in degrading MO, MB, and RhB dyes under these conditions was confirmed by Turnover number (TON) and Turnover frequency (TOF) analysis. The authors associated the superior photocatalytic efficiency of SnO
2-NPs-4% to the smaller particle size, larger surface area, and the increased number of active sites present on the surface when compared to the other samples. Finally, the authors investigated the involvement in the degradation of dyes, and they evidenced that
•OH radicals are the main species responsible for degradation.
Apart from the above-mentioned SnO
2-based photocatalysts prepared by various synthesis methods and the experimental conditions, the search for different photocatalytic materials with the desired efficiency is still a challenge. In this context, different authors have prepared SnO
2 catalysts, owing to the flexibility of applications, including photocatalysis. Compared to powdered materials, the use of films in photocatalysis has some advantages, especially for being easily recovered and reused in different batches. For instance, Bezzerouk et al. [
80] deposited SnO
2 thin films on glass substrates at 450 °C by an ultrasonic spray pyrolysis technique, and desired polycrystalline SnO
2 films were obtained with a band gap of 3.80 eV, greater than that for bulk SnO
2 (
Eg = 3.6 eV). The authors evaluated the photocatalytic property of the films toward Methylene blue (MB) degradation under UV-LEDs (340–400 nm, 7 W) and ultrasound (US) transducer (40 KHz). Different degradation processes were investigated, such as: photolysis (UV), photocatalysis (SnO
2 + UV), the sonolysis process (US), and sonocatalysis (SnO
2 + US) as well as sonophotolysis (US + UV) and sono-photocatalysis (SnO
2 + UV + US). Curiously, SnO
2 film did not show meaningful activity in the degradation of MB dye under UV irradiation (photocatalysis). However, when US was employed, a pronounced increase in the dye degradation was observed, reaching to 88.33%, 94.31%, 97.28%, and 98.25% of efficiency when sono-photocatalysis (SnO
2 + UV + US), sonolysis (US), sonophotolysis (US + UV) and sonocatalysis (SnO
2 + US) processes were used, respectively. The authors associated the highest efficiency of dye degradation using sonocatalysis to the production of acoustic cavitation in the water that can favor the dissociation of water and the formation of an important quantity of
•OH radicals that participate in the degradation of dye. Finally, the authors associated the lower efficiency of the processes under UV irradiation to the rapid recombination of the electron–holes during SnO
2 photoexcitation. Therefore, authors showed different processes used to improve dye degradation using SnO
2-based material.
As one could see, several methods and experimental conditions were employed to synthesize undoped SnO
2 materials (in powder and film forms) with different characteristics and properties. It has been shown that these characteristics can directly impact the photocatalytic activity toward the degradation of dyes under UV-visible light, as well as under direct or simulated sunlight or even coupled with ultrasound irradiation. A summary of some important works concerning the photocatalytic applications of different undoped SnO
2 materials obtained by different methods is listed in
Table 2.
It is known that, to design an efficient system, photocatalysts usually need to meet some requirements, such as appropriate band gaps for light absorption, effective charge of carriers’ separation, and appropriate VB and CB edge potentials. However, it is difficult for pure SnO2-based photocatalysts to satisfy all of them. In this sense, do** SnO2 with different cations and the formation of SnO2-based composites with other materials have attracted interest, as they drive other possibilities of photocatalytic studies. Therefore, discussion of different works concerning the photocatalytic properties of doped SnO2 and SnO2-based composite is given in the following sections.
4.2. Doped SnO2 Photocatalysts
Although pure SnO2 nanoparticles with a different morphology have shown efficiency in the degradation of dyes under irradiation, different authors have developed strategies to overcome the low photoactivity of SnO2 under visible light exposure. For instance, do** SnO2 with different foreign ions has shown to be an efficient way to shorten its band gap and enhance its photoactivity.
Based on this fact, N. Mala et al. [
98] synthesized SnO
2 nanoparticles doped with Mg
2+ + Co
3+ cations by a low-cost chemical solution method and investigated the antibacterial activity and photocatalytic efficiency toward the degradation of Methylene blue (MB) and Malachite green (MG) dyes. The authors revealed that the samples presented a tetragonal crystalline phase, with an average crystallite size of 24 and 25 nm for pure SnO
2 and SnO
2-Mg:Co, respectively. The authors suggested that this slightl increase of the crystallite size after do** was due to local distortions in the SnO
2 lattice induced by the presence of dopants. A nanorod-like morphology was confirmed through SEM images, with a reduction in the crystal length and in the average diameter after do**. Surprisingly, an increase in the band gap energy estimated for SnO
2 (3.52 eV) and SnO
2-Mg:Co (4.22 eV) was observed. This behavior is attributed to the quantum confinement effect that normally happens when the nanoparticle size decreases. However, no meaningful variation was observed in the particle size for pure and doped SnO
2 samples. Regarding the photocatalytic activity of SnO
2 and SnO
2:Mg:Co nanoparticles, the authors observed that SnO
2 presented an efficiency of 82 and 86%, while SnO
2-Mg:Co displayed 89 and 92% efficiency toward MB and MG dyes degradation, respectively, under visible light after 60 min. The authors explained that three factors are responsible for the increase in the photocatalytic efficiency of doped SnO
2, which are: prevention of the recombination of electron–hole pairs photogenerated by surface defects, generation of greater number of oxidative species (
•OH, O
2−, and H
2O
2), and particle size reduction.
Chu et al. [
99] synthesized Bi
3+-doped SnO
2 by the hydrothermal method at 180 °C for 24 h, with a variation of bismuth molar content (3, 5 and 7%). The Rhodamine B (RhB) and Ciprofloxacin hydrochloride (CIP) were used as target molecules to evaluate the photocatalytic activity of the synthesized materials under simulated sunlight. XRD analysis confirmed the cassiterite tetragonal phase for all the samples, with no secondary phases, confirming that Bi
3+ is dissolved into the oxide crystal lattice by replacing Sn
4+ during the synthesis. The Bi
3+/Sn
4+ replacement in SnO
2 was confirmed by HR-TEM, UV–vis DRS, and XPS measurements. The average crystallite sizes decreased as a function of do** from 5.3 nm in SnO
2 to 3.3 nm in Bi-SnO
2(7%). In addition, the band gap (
Eg) values showed a subtle variation of 3.72, 3.75, and 3.78 eV for Bi-SnO
2(3%), Bi-SnO
2(5%), and Bi-SnO
2(7%) samples, against 3.86 eV for the pure one. The authors state that the introduction of new levels in the band gap of materials can act as a trap center for electron and hole, reducing charge recombination, which is beneficial to improve photocatalytic activity. By using PL spectroscopy, authors confirmed the lower recombination charge rate in the Bi-SnO
2(5%) sample for presenting the lowest PL emission among all samples. Regarding the photocatalytic activity, Bi-SnO
2(5%) showed an efficiency of 98.28% of RhB dye degradation after 100 min and 92.13% of CIP degradation after 90 min under irradiation. The excellent photodegradation efficiency of the doped samples was due to the increase in light absorption, as well as the effective separation and migration of photogenerated charge carriers. All the results also indicated that there is an ideal amount of Bi
3+ do** to optimize the mentioned characteristics in order to enhance the SnO
2 material functionality.
Although doped SnO
2 is most prepared in powder, thin films based on doped SnO
2 have also been studied in photocatalysis. For instance, S. Vadivel and G. Rajaraja et al. [
84] prepared magnesium-doped SnO
2 films by the chemical bath deposition method, varying Mg
2+ molar concentrations (1, 5, and 10%). The films were deposited on glass, and after deposition they were annealed at 500 °C for 5 h in air to promote crystallization. From XRD analysis, the tetragonal rutile phase was confirmed in all films. Atomic force microscopy (AFM) images revealed that the surface roughness decreases with increasing dopant concentration. The optical band gap energy for pure SnO
2 was 3.63 eV, decreasing to 3.42 eV for the film doped with 10% Mg. The photocatalytic activities of the films were evaluated by the degradation of Methylene blue (MB) and Rhodamine B (RhB) dyes under UV irradiation. The maximum photodegradation of the dyes was reached for 10% Mg-doped SnO
2 film, degrading 80% of MB and 90% of RhB after 120 min. Fast electron transfer and high efficiency in electron–hole pairs separation led to a significant improvement of photocatalytic activity in the doped sample.
In the work conducted by Haya et al. [
82] films of pure SnO
2 and doped with 2, 4, 6, and 8% of Sr
2+ were prepared by a chemical solution deposition method using the sol-gel method to deposit the solution coating on a glass substrate. The effect of do** on the structural, optical, morphological, and photocatalytic properties of the films were studied. According to the results, the increase in Sr
2+ do** promotes a decrease in crystallite size and an increase in the lattice distortion. These effects generate a greater number of defects, such as grain boundaries, micro-stresses, and displacements in the thin film lattice. The average crystallite size decreased from 7.61 nm for undoped SnO
2 to 3.80 nm for 8% Sr-SnO
2. It was also observed by UV-visible analysis that the presence of dopants introduced new intermediate levels in the semiconductor band gap (
Eg), decreasing
Eg from 3.86 eV for pure SnO
2 film to 3.76 eV for Sr-richer SnO
2 film. Additionally, the morphology of the films was analyzed by AFM, and a smaller grain size was observed for 8% Sr-SnO
2 (4.96 nm). Consequently, it showed the lower surface roughness when compared to the other films. Concerning the photocatalytic activity, the greatest efficiency in the degradation of MB dye under irradiation was attained for 8% Sr-SnO
2 film, which was attributed to smaller grain sizes and surface roughness, as well as the introduction of new energy levels below the conduction band of the pure material, resulting from the Sr do**.
Using a non-conventional method to prepare thin films, Loyola Poul Raj et al. [
83] prepared SnO
2 thin films doped with 3 and 6 mol% of Tb
3+ on a glass substrate by the spray nebulized pyrolysis (NSP) method and calcined them at 400 °C to crystallize the materials. The authors investigated the photocatalytic property of the films in the degradation of MB dye under UV irradiation. According to the authors, do** SnO
2 films with up to 6% of Tb
3+ cations induces a decrease in the grain size from 80 to 56 nm, and the band gap from 3.51 to 3.36 eV, which directly impacts photocatalysis, as reported by other authors. Indeed, a maximum of 85% of dye degradation was observed after 120 min under UV irradiation using SnO
2 film doped with the 6 mol% Tb
3+. Using PL spectroscopy, the authors reveal that Tb do** leads to the creation of more defects that act as reactive sites for catalyzed reactions. As a consequence of the study, the authors concluded that Tb do** favored photocatalytic reactions by reducing particle size, and therefore increasing the surface area and the number of reactive sites on the surface, which allows the dye adsorption. In addition, Tb do** induces a decrease in the band gap of the materials, which favors photo-absorption, aiming to potentialize charge carriers to participate in photocatalytic reactions.
Other studies based on the synthesis of doped SnO
2 catalysts and their applications in the photodegradation of different organic dyes are listed in
Table 3.
4.3. SnO2-Based Composite Photocatalysts
As one can see from studies discussed in the sections above, pure and doped SnO2 particles and films have been well explored. However, SnO2 has also been combined with other different semiconductors in order to reduce recombination of the photoinduced charge carriers, to therefore improve photocatalytic activity.
Considering this fact, Abdel-Messih et al. [
105] synthesized SnO
2/TiO
2 nanoparticles with a spherical mesoporous morphology synthesized by the sol-gel process, using polymethylmethacrylate as a template. The amount of SnO
2 (0–25%) in relation to the mass of pure TiO
2 was varied to obtain composites with different compositions. The samples were calcined at 800 °C for 3 h to ensure complete organic polymer decomposition. In relation to the photocatalytic property of the materials, photodegradation of Rhodamine B (RhB) dye was performed under UV irradiation using a catalyst/dye concentration of 1 g L
−1. The photodegradation efficiency of the composites increased with the increase of tin oxide content up to 10% (about 92% of the dye degraded after 3 h). However, the sample with 25 mol% of SnO
2 showed the lowest efficiency, which was attributed to the loss of the titanium anatase phase. The authors concluded that there is an optimal amount of SnO
2 to achieve the maximum efficiency. In addition, the remarkable reduction in particle size by the existence of SnO
2 in the composites enhanced the oxidizing power and extended the photoinduced charge separation, and these were the main reasons for the increase in the catalytic activity of the samples.
Das et al. [
36] prepared Sn/SnO
2 nanocomposites by the precipitation method, followed by carbothermal reduction and calcination at 800 °C for 2 h. The authors investigated the photocatalytic property of Sn/SnO
2 composites in the degradation of methylene blue under UV irradiation using a catalyst concentration of 0.5 g L
−1. It was found that there was a maximum efficiency of 41% for pure SnO
2 after 210 min under irradiation, while the Sn/SnO
2 composite showed a higher photocatalytic activity of 99%. The highest efficiency observed for the composite was related to the role of Sn on the surface of SnO
2 nanoparticles. As the Fermi energy level of Sn is higher than that observed for SnO
2 due to its lower work function, when metallic Sn is bound on the surface of SnO
2 nanoparticles, electrons migrate from Sn to SnO
2 to reach Fermi-level equilibrium. The effect of the pH solution on the photocatalytic efficiency of the composites was also evaluated. The pH had a direct influence on the photocatalytic process, being the neutral pH favorable for the degradation of MB dye. Finally, the authors investigated the reusability of the composites after three cycles and confirmed that the photocatalyst is stable, but gradual loss in efficiency was observed due to the loss of the material during recovery processes.
Li et al. [
85] synthesized carbon-coated, mixed-phase (tetragonal/orthorhombic) SnO
2 (i.e., tetragonal/orthorhombic) nanorods photocatalysts by a combined chemical precipitation and hydrothermal method at 180 °C for 6 h. The SnO
2-C composite with a SnO
2 tetragonal phase was obtained after calcination of the hydrothermal products at 550 °C for 4 h. The photocatalytic activities of the samples were investigated toward the degradation of Methyl orange (MO) dye under UV irradiation using a catalyst/dye concentration of 0.6 g L
−1. The as-prepared mixed-phase SnO
2 showed a photodegradation activity of 52% against an efficiency of 39% for pure SnO
2 with a tetragonal phase after 60 min under irradiation, indicating the influence of different phases on the junction formation to tune photocatalytic activity. Coating mixed-phase SnO
2 nanorods with carbon provided a degradation activity of 98%. The tetragonal/orthorhombic-SnO
2 material exhibits very high stability after three cycles, remaining about constant without apparent deactivation. Photocatalytic activity was not primarily attributed to the narrower band gap or visible light absorption tail. By demonstrating that the transfer and separation of photogenerated electron–hole pairs are improved by the introduction of a carbon layer in interparticle space. To understand the photocatalytic mechanism, different scavengers were used in the study—triethanolamine (TEOA), tert-butyl alcohol (TBA), and benzoquinone (BQ). The results indicated that the species
,
, and
played important roles in the degradation of MO.
Constantino et al. [
97] synthesized a porous composite based on SnO
2/cellulose acetate with the electrospinning method and calcined it at 120 °C for 48 h. The photocatalytic activity of the nanocomposites was studied toward the degradation of MO and MB dyes under UV irradiation using a catalyst/dye concentration of 1.3 g L
−1. The photocatalytic efficiency of SnO
2/cellulose was approximately 92% of MO degradation after 210 min and 95% of MB degradation after 240 min. It is worth mentioning that the photodegradation process did not alter the average diameter and morphology of the fibers as well as their surface chemistry. From TOC analysis, the authors evidenced that only 54% and 79% of MO and MB dye are mineralized after the photocatalytic process. However, presence of other compounds as by-product of dye degradation was confirmed by LC–MS.
Silva et al. [
37] synthesized spherical nanoparticles and microrods of Ag
3PO
4/SnO
2 composites, by the in situ coprecipitation method, with various molar ratios of 5, 10, 15, and 20% of SnO
2 in relation to the mass of pure Ag
3PO
4, followed by calcination at 350 °C for 2 h. The photocatalytic performance of the samples was investigated by the degradation of Rhodamine B (RhB) dye under visible light irradiation using a catalyst/dye concentration of 0.6 g L
−1. The authors observed superior photocatalytic activity for all the composites when compared to pure Ag
3PO
4. The authors evidenced that the excess of SnO
2 damaged the interfacial contact between the Ag
3PO
4 and SnO
2, which was due to the high degree of particle agglomeration. The photocatalytic mechanism involved in the photodegradation of the dye was also investigated for pure Ag
3PO
4 and Ag
3PO
4/SnO
2-15%. It has been confirmed that the photogenerated holes participated in the direct degradation of RhB when Ag
3PO
4 was a photocatalyst. On the other hand, there was a significant participation of
radicals when Ag
3PO
4/SnO
2-15% is used. The highest photodegradation efficiency presented by the Ag
3PO
4/SnO
2-15% composite was confirmed by total organic carbon (TOC) analysis. Reusability tests were also performed for Ag
3PO
4/SnO
2-15% and a loss of 43.2% of its photocatalytic efficiency was observed after the third cycle, which was similar to that observed for pure Ag
3PO
4. Using the X-ray diffraction technique, the presence of Ag in the composition of the samples was observed after the photocatalysts were used in photocatalysis.
Apart from the above-mentioned studies performed using composite particles, SnO
2-based composite photocatalysts have also been explored as films. For instance, porous SnO
2/TiO
2 films were prepared using Ar-assisted, modified thermal evaporation, followed by the atomic layer deposition (ALD) technique at 300 °C in the reaction chamber [
62]. To prepare SnO
2/TiO
2 films, TiO
2 layers were deposited on porous SnO
2 nanofoam, with those previous deposited on 2 × 2 cm
2 Si (100) wafers or ITO substrates, with variation in deposition cycles of TiO
2 (10, 25, 50, and 100 cycles) by ALD. The samples were denoted SnO
2/TiO
2-10, SnO
2/TiO
2-25, SnO
2/TiO
2-50, and SnO
2/TiO
2-100, respectively. After the TiO
2 deposition, the material was calcined at 700 °C for 1 h. The photocatalytic properties of the films were evaluated by the degradation of MB at a concentration of 1.2 mg L
−1 under UV irradiation. The nanofoam heterostructures showed higher photocatalytic activity when compared to the porous SnO
2 nanofoam. SnO
2/TiO
2-50 nanofoam, which exhibited the highest efficiency, reached to 99% of MB degradation after 300 min. The authors correlated this fact to being due to a synergistic effect occurring between SnO
2 and TiO
2, and due to the sparse deposition of the TiO
2 layer on porous SnO
2. Separation of charge carriers due to the potential difference between SnO
2 and TiO
2 increases the lifetime of the charge and improves the interfacial charge transfer to the species adsorbed on the surface. This phenomenon, along with the strong oxidant
•OH radicals formed in the VB of the TiO
2 layer, improves photocatalytic efficiency of the SnO
2/TiO
2 heterostructure.
Other important works reporting the activity of SnO
2-based composite photocatalysts for the degradation of dyes are summarized in
Table 4.
Most of the authors reported that the number of materials for the formation of the SnO2 with a different particle size and morphology, besides doped SnO2 with an appropriate amount and type of dopant, and also the formation of the composite with SnO2, plays an important role in improving the photocatalytic activity of the SnO2 material. In relation to composites, the excess of both species can be harmful to the contact surface between the phases, mainly due to the high degree of particle agglomeration. Tests using scavengers, such as p-benzoquinone (BZ, C6H4O2), isopropanol (ISO, (CH3)2CHOH), and ammonium oxalate monohydrate (AO, (NH4)2C2O4·H2O) indicate •OH is the main species in most photocatalytic mechanisms. However, to obtain more insights about the photocatalytic mechanism involved in composite materials, we seek to understand the charge transfer between the phases from the band structures of each individual material. Structural and electronic defects can also generate energy levels between the VB and CB, and, therefore, modify the photocatalytic mechanism of composites. The creation of different interfaces between the phases may reduce charge carriers’ recombination, leading to the formation of a great number of free radicals to improve photocatalysis. In addition, several other parameters can impact the photocatalytic efficiency of composites, such as phase composition, surface area, morphology, particle size, pore structure, electron–hole recombination rate, and band gap energy of the individual components. Some authors showed that the high surface area and the presence of pores are more effective parameters that affect dye degradation since the existence of several active sites, responsible for the adsorption of molecules, is crucial for the photocatalysis to occur.
Based on the findings above, it can be concluded that to design a new photocatalytic material with specific characteristic, one has to consider optimizing type and amount of dopants and interface characteristics between materials, or even the nature of the desired product (powder, film, etc.), besides the microstructure of the material (particle size and morphology), and by a choice of specific synthesis methodology and appropriate experimental conditions.