- Nano Express
- Open Access
Synthesis, Characterization, and Photocatalytic Properties of Sulfur- and Carbon-Codoped TiO2 Nanoparticles
© Ivanov et al. 2016
- Received: 1 December 2015
- Accepted: 2 March 2016
- Published: 12 March 2016
One-step TiO2 nanoparticle synthesis based on the interaction between thiourea and metatitanic acid is applied for sulfur and carbon anatase codoping. The synthesis of the doped TiO2 has been monitored by means of differential thermal analysis and thermogravimetric analysis (DTA-TG), which allows determining the optimal thermal conditions for the process. Electron microscopy showed micrometer-sized (5–15 μm) randomly distributed crystal aggregates, consisting of many 15–40-nm TiO2 nanoparticles. The obtained phase composition and chemical states of the doping elements are analyzed by means of X-ray diffraction (XRD), X-ray photoelectron spectroscopy (XPS), infrared (IR) and Raman spectroscopies, and electron paramagnetic resonance (EPR). XRD displays in both samples (doped and pristine) the existence of only one crystalline phase—the tetragonal modification of TiO2—anatase. Further data assessment by means of Rietveld refinement allowed detection of a slight c lattice parameter and volume increase related to incorporation of the doping elements. XPS demonstrated the presence of carbon and sulfur as doping elements in the material. It was confirmed that carbon is in elemental form and also present in oxygen-containing compounds, which are adsorbed on the particle surface. The binding energy for sulfur electron core shell corresponds to the established data for sulfate compounds, where sulfur is in 6+ oxidation state. The synthesized S- and C-codoped TiO2 showed excellent photocatalytic performance during the degradation of organic dyes (rhodamine B, methylene blue), gas-phase oxidation of ethanol under visible light, and photocatalytic hydrogen generation from ethanol under ultraviolet light.
- TiO2 nanoparticle
- Metatitanic acid
- Sulfur-carbon doping
- X-ray photoelectron spectroscopy
One of the promising directions in solving global problems of alternative energy and environment is the application of advanced technologies based on photocatalytic processes. Catalytically active TiO2 has been a subject of considerable attention due to its optical properties, chemical stability, non-toxicity, and high photoactivity. Therefore, this type of material is widely used for decomposition and synthesis of a number of organic compounds . Furthermore, photocatalytic TiO2 has already been implemented in different practical fields such as antiviral and antibacterial agent [2, 3], for the destruction of cancer cells [4, 5], decomposition of volatile organic compounds, and water splitting. TiO2 is essential in medical and dental research due to its favorable properties, i.e., biocompatibility and low reactivity . It already finds application in the construction of dental implants and hollow drug-containing structures. For instance, TiO2 nanotubes are implemented in medicine for gradual drug release .
One of the most important actual applications of TiO2 lies in the field of renewable energy conversion and storage . The overall trend of the world’s energy systems requires broader introduction of hydrogen energy. In particular, the development of new technologies for hydrogen production through the design of suitable catalytic materials such as TiO2 is highly important. Advanced photocatalytic methods can lead to a significant cost reduction of both the hydrogen and the auxiliary systems. However, development of competitive materials with improved catalytic performance is required.
In particular, the doping of TiO2 structures with extra elements allows sensitizing the material in the visible wavelengths and/or increasing the photoactivity in the ultraviolet spectrum . Doping with transition metals such as Fe, Mn, V, and Cr [10–15] displays low photocatalytic activity due to the thermal instability of the material  and furthermore creates environmental concerns. In the recent years, modification of TiO2 with nonmetal elements has received much attention, since they demonstrate effective doping, do not introduce ecological issues, and offer a low production cost. For example, the incorporation of nitrogen [17–22], carbon [23–26], sulfur [27–29], and iodine  in TiO2 structure can lower its band gap and therefore shift its optical response to the visible light region.
It was recently found that sulfur-doped TiO2 exhibits a strong antibacterial effect under visible light, enabling effective inhibition of Micrococcus lylae and most of the Gram-positive bacteria . The formation of hydroxyl radicals during irradiation of the structure by visible light plays a central role for the bactericidal activity of the material.
In most of the cases, the doping by appropriate amount of sulfur allows the use of S-TiO2 photoelectrodes in the visible spectrum region. Nevertheless, the structural aspects of sulfur integration in TiO2 are still debatable. Practically, the sulfur amount and its distribution in the TiO2 structure are to great extent influenced by the synthesis conditions. Recent studies in the field showed that sulfur is included in form of S4+ and S6+ predominantly on the surface of TiO2 nanoparticles . On the other hand, there are significant proofs that sulfur is integrated in the TiO2 lattice forming S–Ti–O bonds .
The doping of TiO2 with carbon brings considerable potential advantages over other types of non-metallic doping. Carbon increases the conductivity of the structure , can accept the photon-excited electrons, enhances the separation of photo-generated carriers [34, 35], and displays visible light absorption in the wavelength of 400–800 nm [36, 37]. Most of the structural analyses of carbon-doped TiO2 indicated incorporation of this element into the lattice, substituting an O atom and forming O–Ti–C bond. The visible light absorbance in this case can be explained by the formation of a hybrid orbital above the valence band of TiO2 caused by carbon integration [38, 39].
Optimization and tuning the photocatalytic properties of the doped TiO2 is important with respect of its practical application. One of the appropriate methods in this direction is TiO2 co- and multiple doping, showing in a number of cases visible synergetic effects. Literature survey on sulfur-carbon TiO2 codoping shows that the topic is just approached and requires further analytical information on the influence of synthesis method and different structural factors.
In the present work, one-step TiO2 nanoparticles synthesis based on the interaction between thiourea and metatitanic acid is applied for sulfur and carbon anatase codoping. The integration of the doping elements is characterized by a number of physical methods, revealing the structural aspects of the doping process. A central task in our study is to test the photocatalytic activity of the SC-codoped TiO2 during decomposition of methylene blue, gas-phase photocatalytic oxidation of ethanol, and photocatalytic hydrogen generation from ethanol. According to the authors’ knowledge, the SC-TiO2 material has not yet been tested for the processes of photocatalytic ethanol oxidation and hydrogen generation. The impact of sulfur as a doping element in TiO2 is discussed in terms of its photocatalytic activity, compared to other already known TiO2 dopants.
Chemicals and Materials
Thiourea was provided by Wako Pure Chemical Industry. Other chemicals were obtained from commercial sources as guaranteed reagents and were used without further purification.
Synthesis of SC-codoped and Non-doped TiO2 Nanopowders
Two samples of SC-codoped TiO2 nanopowders were synthesized using a solid-phase method; 12.2 g (sample 1) and 18.6 g (sample 2) of a metatitanic acid and 12.8 g (sample 1) and 6.4 g (sample 2) of thiourea were triturated in an agate mortar to obtain a homogeneous mass, which was further annealed in air atmosphere at 500 °C for 1 h.
The resulting powder samples differ in the amounts of doping elements. According to EDX analysis, sample 1 contains 0.23 wt.% sulfur and 10.68 wt.% carbon and sample 2 contains 0.45 wt.% sulfur and 2.38 wt.% carbon. The white non-doped TiO2 nanopowder was synthesized from metatitanic acid in the absence of thiourea under identical thermal conditions.
Structural and Spectroscopic Characterization
The morphology and particle size of prepared nanoparticles were analyzed by SEM and TEM. A high-resolution scanning electron microscope Hitachi S-4800 II was used. The JEOL-JEM-1011 TEM microscope, operated at an accelerating voltage of 80 kV with a resolution of 0.2 nm, was used. The powder samples were prepared by air-drying a drop of a sonicated suspension onto copper grids.
The phase identification of sulfur-doped TiO2 structure was carried out by powder X-ray, using a Siemens D5000 diffractometer in reflection mode with Cu target Kα radiation. XRD patterns were recorded in the 2θ range of [15; 100°] with a step size of 0.02° and a stay time of 1 s/step.
Differential thermal analysis and thermogravimetric analysis (DTA-TG) was performed in air in the temperature range T = [20 °C; 800 °C] at a scan rate of 10 °C min−1 using derivatograph Q-1500 Paulik.
The optical properties were characterized by light absorption in the UV-vis and infrared region (FTIR) and Raman spectroscopy. The UV-vis absorption spectra for pure TiO2 and TiO2 doped by sulfur samples were recorded by an Evolution 300 UV-vis spectrophotometer (Thermo Scientific) in the range from 300 to 800 nm. The FTIR spectroscopy measurements were performed by Specord M-80 spectrometer in the middle infrared wavelengths (400–4000 cm−1). The Raman spectra were obtained using the Smart Raman DXR (Thermo Scientific) spectrometer. The semiconductor laser of 12-mW power and 780-nm wavelength was used as a light source.
The analysis of surface composition was carried out by means of X-ray photoelectron spectroscopy (XPS) using XSAM-800 Kratos spectrometer. The sample surface composition was determined using photoelectron line area ratio taking into account their sensitivity factors. The thickness of analyzed layer was ~5 nm.
The zeta potential measurement was performed by means of Zetasizer (Malvern Instrument Ltd.). The tested samples were suspended in water (pH = 7), vortexed and sonicated before measurement. The experiments were repeated three times for each sample, at T = 25 °C (±0.1 °C) and 1 mL of sample volume. The electrophoretic mobility and zeta potential were determined according to Smoluchowski’s equation.
EPR spectra of nanopowders were investigated in air at room temperature using spectrometer RADIOPAN X-85.
Photocatalytic Measurements, Sample Preparation
Photocatalytic properties of synthesized powders were evaluated during the degradation of organic dyes (I), photocatalytic hydrogen generation in water-alcohol suspensions (II), and gas-phase oxidation of volatile organic compounds (IІI).
(I) Photocatalytic activity of gel samples containing SC-TiO2 nanoparticles has been tested for the decomposition of rhodamine B and methylene blue. Activation process has been performed using power LEDs with emission bands in the visible range of the spectrum (λ = 455 nm, λ = 525 nm).
Gelatin and polyvinyl alcohol (PVA) were selected as available and environment-friendly raw materials for obtaining gel—SC-TiO2 coatings. However, the application of gelatin is not practical due to the insufficient gel stability at low temperatures (3–6 °C). For the synthesis of gels based on PVA, aqueous solutions of varying content (5, 10, 15, 20, and 25 wt.%) were prepared. In order to dissolve PVA, the solutions were heated at 100 °C for about 10 min. Solutions containing 25 and 20 % (w/w) PVA have been instantly transformed into a gel, 15 % in 10–15 min and 5 % in 1 day. Therefore, 10 % PVA solution was selected for our research, since its gel transition takes approximately 2 h, which is sufficient for the necessary operations. The required amount of synthesized SC-TiO2 and hydrogen peroxide was added to the viscous PVA solution (~1 h after preparation) and stirred. This solution was applied to the inner surface of a quartz cuvette. After the formation of the gel, the surface is ready for photocatalytic reactions.
(II) Kinetic studies of hydrogen generation have been carried out in a thermostatted glass reactor (volume of 10.0 ml). The suspension of water, alcohol (ethanol containing 4 mol/L H2O), and sample of SC-TiO2 (0.05 g) was placed in the reactor. Irradiation of the reactor has been performed by a mercury lamp with DRSh ~ 1000 λ = 365 nm (UFS-2, the light intensity (I 0 = 7 · 10−6 Einstein/min) was measured by ferrioxalate actinometer); 0.01 g of Pd/SiO2 was acting as a catalyst. The temperature of the reaction mixture was equal to 40 °C. During the reaction, the solution was not stirred. Solutions were evacuated before radiation. The amount of formed hydrogen in the reactor during irradiation of the solution was determined chromatographically by means of LHhM-8MD chromatograph with thermal conductivity detector. The measurements were performed by using carrier gas argon and chromatograph columns filled with molecular sieve NaX.
(III) The study of ethanol gas-phase oxidation kinetics was carried out in a thermostatted glass reactor (volume of 130 ml). Two milliliters of ethanol with a sample of SC-TiO2 (0.05 g) was placed in the reactor. Irradiation of the reactors has been performed by a mercury lamp with DRSh ~ 1000 λ = 310–390 nm (UFS-2); the light intensity was 1.2 · 10−5 Einstein/min and the light of mercury lamp with DRSh ~ 1000 λ ≥ 420–440 nm (UFS-2). The temperature of the reaction mixture was ~20 °C. During the reaction, the solution was not stirred. The amount of the ethanol remaining in the reactor and quantity of the generated acetaldehyde were determined chromatographically. The concentration of ethanol and acetaldehyde was measured by Chrome-5 chromatograph with flame ionization detector (column filled by SEPARON-SDA08 and carrier gas argon).
Synthesis and Structural Characterization
The processes taking place during the synthesis of SC-codoped TiO2 nanoparticles were characterized by means of thermogravimetry, where the thermal behavior of the individual reaction components (thiourea and metatitanic acid) and their mixture was analyzed.
Endothermal process with a maximum at 135 °C related to a dehydration metatitanic acid;
Endothermal effects with a maximum at 175 and 195 °C connected to the melting of thiourea;
Exothermal process at 240 °C linked to crystallization of anatase within presence of thiourea and simultaneous thermal degradation to the above described gaseous products;
Exothermal processes with a maximum at 315 and 415 °C showing the thermal oxidation of the organic residues, sulfur, and continued crystallization of anatase.
X-ray phase analysis of the mixture between metatitanic acid and thiourea, annealed at 315 °C at a heating rate of 10 °C/min, displays the anatase crystallization, confirming our statements.
Based on the literature data [41, 42] and DTA results for the mixture of thiourea and metatitanic acid (Fig. 1c), it can be concluded that the loss of weight on heating is completed at a temperature of 415 °C, in contrast to weight loss during individual thiourea thermolysis, which lasts up to 500 °C and beyond. Obviously, in this case, the formed elemental sulfur oxidizes slowly; and in the case of the mixture, sulfur interacts with anatase. Thus, it was determined that the optimum temperature for the sintering of samples is 500 °C which is the temperature of completion of the process with an exothermic maximum at 415 °C.
TiO2 crystal lattice parameters assessed by Rietveld refinement method
Spectra of sample I and sample II SC-doped TiO2 powders are similar with main lines at 638, 516, 396, and 145 cm−1, which confirm the structure of anatase. The Raman lines can be assigned as the Eg, A1g, B1g, and Eg modes of the anatase phase, respectively . The most informative is Eg band at 145 cm−1 arising from the external vibration of the anatase structure. If the line becomes weak or broad, there occur probably the local lattice imperfections .
In the IR spectrum of the samples, the absorption band at 3700–3500 cm−1 is due to vibrations of OH bonds on the surface of TiO2. It can be seen that the absorption has a low intensity, due to a small amount of OH groups as a result of relatively high annealing temperatures . The bands observed in the region at 2350–2000 and 1650–1500 cm−1 are related to a presence of adsorbed carbon monoxide . The absorption at 1700–1000 cm−1 is characterized with vibrations in the surface-linked carboxyl compounds. The observed oscillations at 1560 and 1350–1420 cm−1 allowed us to attribute the resulting carbonate-carboxylate group to the bidentate carbonate [47–49]. Absorption band at 2200–2000 cm−1 relates to vibrations of the C=O bonds in complexes that are decomposed at 150 °C. Such form occurs only due to adsorption interaction of carbon (II) oxide at 20 °C with the surface of TiO2. The oscillation maxima at 2347, 2064, and 2215 cm−1 are related to CO adsorption, showing that the sample substantially adsorbs CO.
The band at 1470–1000 cm−1, visible only for the doped TiO2 samples, characterizes sulfur-containing functional groups. In particular, according to , the absorption at 900–700 cm−1 is associated with the vibrations of ν S–O. Furthermore, the presence of additional band in the range 1100–1040 cm−1 is linked to ν S=O vibrations and 1400–1310 cm−1 and 1230–1120 cm−1 to ν SO2 vibrations. In the particular case of SC-TiO2, the presence of absorption with maximums at 1379, 1348, and 1113 cm−1 can be attributed to variation of ν SO2 oscillations, characteristic for a sulfate group. The weak absorption peaks at 1260–1150, 1080–1010, and 700–600 cm−1 are representative for SO2OH group.
Vibrational frequency of ν O–O bonds in O2− ions can be identified in the range 1180–1060 cm−1 . As it can be seen from the figure, the peaks at 1113 and 1024 cm−1 are slightly shifted to lower frequencies but obviously are responsible for the vibrations of ν O–O. Actually, the existence of such bonds suggests activity of the synthesized powders towards photocatalytic oxidation processes.
Finally, the absorption at 750–400 cm−1 can be attributed to oscillations of the atoms in Ti–O and Ti–O–Ti bonds. In particular, the disappearance of the absorption band (750–550 cm−1) is due to the breaking of surface Ti–O bonds during high-temperature treatment .
The analysis showed identical features for both types of doped SC-TiO2 samples. The results display big amount (about 30 %) of carbon, where three signal components at binding energies of 285.0, 287.0, and 289.0 eV are observed. The main maximum at 285.0 eV is attributed to elemental disordered carbon. However, multiple carbon sources, including adventitious carbon (in vacuo or external post-synthesis contamination) and chemical doping during synthesis theoretically can be the origin of its presence. Typically, the in vacuo contamination rates are very low compared with the detected carbon amount in our work. In most of the cases, adventitious carbon is in form of up to a nanometer thin island-type deposit, which thickness is far below the penetration depth of XPS source. Therefore, the detected high amount of surface carbon originates probably not from in vacuo contamination. Furthermore, the powder samples for XPS measurements are coated on a carbon tape attached to the sample holder, where a complete coverage of the substrate was achieved in order to exclude eventual signal from the carbon tape. On the other hand after annealing at high temperature in oxygen-containing atmosphere (for our experimental conditions 1 h at 500 °C in air), the existence of high amount of elemental carbon is less probable, suggesting that the high-intensity peak at 285 eV can be a result from external post-synthesis (not in vacuo) contamination.
The shoulder at 287.0 and the maximum at 289.0 eV are attributed to C–O and C=O bonds, where carbon can substitute lattice Ti atoms forming a Ti–O–C structure . C=O groups are usually adsorbed on the surface, terminating the carbon interface or adsorbed on TiO2. Furthermore, the results from the infrared spectroscopy correlate well with XPS analysis confirming the presence of carbon-oxygen groups on the SC-TiO2 surface.
Oxygen is involved in the form of oxides (Eb = 530.6 eV), carbon-containing and OH groups adsorbed on the surface (shoulder at 532 eV). The binding energy of titanium (459.0 ± 0.3 eV) and sulfur (169.0 ± 0.3 eV) core shell for SC-TiO2 powders corresponds to established data for TiO2 and MeSO4 compounds, respectively. In particular, sulfur is found exclusively in the oxidation state +6.
Quantitative elemental analysis of TiO2 samples
C, % at.
O, % at.
Ti, % at.
S, % at.
C–H ~ 90 %
C–O ~ 10 %
Еb = 458.8 еV
Ti4+ ~ 100 %
Еb = 168,8 еV
S6+ ~ 100 %
The zeta potential, electrophoretic mobility, and dynamic light scattering analysis (hydrodynamic diameter and polydispersity) for non-doped TiO2 and SC-TiO2 powders
Zeta potential (mV)
Electrophoretic mobility (μmcm/Vs)
Particle size (nm)
−43.5 mV ±0.7
−24.2 mV ±1.0
−25.0 mV ±0.5
The zeta potentials of all TiO2 samples, summarized in Table 3, showed negative values. The values of zeta potential for SC-doped TiO2 samples are about −25 mV which closely resemble the threshold value, indicating moderate stability of tested materials and low interaction affinity. Completely stable suspensions are considered, those with particles less than −30 or higher than 30-mV zeta potential. This condition is met by pure TiO2 and it is consistent with literature data .
It can be seen that the spectrum displays only one narrow line with the g-factor of 2.004 + −0.001. The amplitude of the line does not depend on the illumination in this spectral range. The line with g-factor 2.004 is associated with a single-electron-trapped oxygen vacancy . Therefore, sensitization process of the nanopowders doped by sulfur and carbon is a result of the formation of additional oxygen vacancies in TiO2 structure.
Photocatalytic Properties of SC-doped TiO2 Samples
Photocatalytic activity of the SC-doped TiO2 nanopowders was tested for the discoloration of solutions containing rhodamine B and methylene blue. The samples were further applied for photocatalytic generation of hydrogen in the visible light wavelength.
Keeping constant the optimal concentration of hydrogen peroxide (6 wt.%), the gels with different content of SC-TiO2 (2, 8, 14, and 20 wt.%) were prepared to determine the effect of its amount on the photocatalytic activity of the coating. Methylene blue was poured in the cuvette with gel-like coating and the measurement of the sample absorption was carried out similar to the previous one (Fig. 10a). The kinetic dependences (Fig. 10b) show that 10 times increase of SC-TiO2 amount in the gel results in reduction of the decomposition duration of methylene blue already by about 6 times. Similarly, images of the solution before and after the discoloration are inserted in Fig. 10b.
The obtained results show that the nanosized SC-TiO2, introduced in gel-like matrix, has high photocatalytic activity for the degradation of organic dyes. This effect can be explained, by the sulfur-carbon doping of the TiO2 particles, providing extension of the light absorption to the visible range of the spectrum. Additionally, the use of SC-TiO2 with H2O2 makes possible to enhance the generation of OH radicals, which facilitates the kinetics of organic pollutants oxidation.
It was established that SC-TiO2 samples synthesized by both methods are active in the photocatalytic oxidation of ethanol under visible light (sample 1 (C2H5OH) = 3.5 × 10−8 mol/min, sample 2 (C2H5OH) = 2.3 × 10−8 mol/min).
The results indicate that the ethanol oxidation kinetic depends strongly on the method for synthesis. In the case of sol-gel-synthesized sample (sample 2), the ethanol concentration rapidly drops in 15 min, which allows detecting the maximum of acetaldehyde generation at the moment of almost complete dissociation of ethanol. In contrast, ethanol oxidation catalyzed by TiO2 synthesized by solid-state method (sample 1) is characterized by lower reaction rate, where the complete conversion of ethanol is achieved for more than 25 min and no maximum of acetaldehyde concentration is observed. The differences in the catalytic activities of the samples can be explained by the particular surface chemistry and defect density achieved by both synthetic methods. In general, SC-TiO2 materials display good photocatalytic activity for the gas-phase ethanol oxidation, which makes them appropriate for air decontamination.
Sulfur and carbon TiO2 codoping was accomplished by the interaction between thiourea and metatitanic acid. The nanopowder material was characterized by a number of physical methods.
The synthesis of the SC-TiO2 was studied by means of DTA-TG, which allowed determining the optimal temperature conditions of 500 °C for the synthesis and thermal post-treatment of the samples. Electron microscopy showed micrometer-sized (5–15 μm) randomly distributed crystal aggregates, consisting of many 15–40-nm TiO2 nanoparticles.
All types of TiO2 materials are crystallized in the anatase tetragonal phase. The incorporation of doping elements into the anatase crystal lattice was evidenced by XRD. It was confirmed that carbon is present in elemental form and also exists in carbon-oxygen compounds. The binding energy of titanium and sulfur core shells for SC-TiO2 powders corresponds to established data for TiO2 and MeSO4 compounds, respectively. XPS analysis revealed that sulfur is exclusively in 6+ oxidation state. Comparison of XPS and EDX data suggests that the doping elements are concentrated predominantly at the particle surface.
The EPR analysis revealed that the sensitization process of the nanopowders doped by sulfur and carbon is a result of the formation of additional oxygen vacancies into TiO2 structure, which are essential for the photocatalytic activity of the material.
The synthesized SC-TiO2 nanopowder can be applied in the processes of photocatalytic organic dyes degradation, gas-phase oxidation of water-alcohol mixtures, and hydrogen generation from ethanol, where the material exhibits high photocatalytic activity.
The authors acknowledged the financial support of the Ministry of Education and Science of Ukraine (grant DB\Tekton no 0115U000427). RW-N would also like to acknowledge the financial support of the Marie Curie Actions of the European Union Seventh Framework Programme FP7/2007-2013/ under REA grant agreement no. 295128 and Prof. D. Leszczynska (Jackson State University, USA) for the support and care during the program. Authors are thankful to V. Tataryn for his help in EPR analysis.
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